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	<id>https://acawiki.org/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Sj</id>
	<title>AcaWiki - User contributions [en]</title>
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	<updated>2026-05-24T16:51:01Z</updated>
	<subtitle>User contributions</subtitle>
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	<entry>
		<id>https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8996</id>
		<title>Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8996"/>
		<updated>2013-01-03T05:04:36Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio&lt;br /&gt;
|authors=J Haag, W Denk, A Borst&lt;br /&gt;
|url=http://adsabs.harvard.edu/abs/2004PNAS..10116333H&lt;br /&gt;
|tags=vision algorithms&lt;br /&gt;
|summary=It has been theorized that fly vision might switch from relying on Reichardt detectors to relying on some other mechanism such as gradient detectors in high signal-to-noise regimes.  This paper summarizes two experiments probing those regimes and testing different parts of the fly vision chain, and finds no evidence for any mechanism other than Reichardt detectors.  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
Gradient detectors are still considered a competing mechanism to Reichardt detectors in high signal-to-noise regimes.  And in order to work with elementary responses, experiments often work at the opposite end of the signal spectrum, aiming for the smallest signal that elicits a measurable response.  As a result few experiments have been carried out to test whether markers of gradient detection can be observed in fly motion vision under any circumstances.&lt;br /&gt;
&lt;br /&gt;
This paper describes two experiments to evaluate the hypothesis that gradient detectors are not part of the fly motion pathways at all. Both study direction selectivity in flies, the canonical test for fly motion vision.  &lt;br /&gt;
&lt;br /&gt;
One experiment tested for the dependence of optimal stimulus 'velocity' (the actual velocity of the pattern used as a stimulus) on the wavelength of the pattern.  This is expected to be directly correlated in the Reichardt detector case, and relatively uncorrelated in the gradient detector case.  It was simply measured by looking at neuron spikes of the motion-sensitive neuron H1.  This test was repeated over a wide range of mean luminance and of stimulus contrast (roughly 2 magnitudes in each case).&lt;br /&gt;
&lt;br /&gt;
The second more complex experiment improved on a traditional experiment to show Reichardt detection: observing the local modulations in signal along a dendrite as a pattern moves past it.  In the Reichardt case this is expected to move synchronous with the pattern, and to be phase-shifted along different parts of the dendrite.  However this was always previously done with 1-photon imaging, which has a side-effect of false positives that limits how small overall noise could be in such an experiment (and so limits the maximum pattern contrast).   This is addressed here by using 2-photon microscopy with luminescent Calcium markers, a technique that allows very high signal without false-positive noise.  Neurons of both vertical and horizontal systems were observed.&lt;br /&gt;
&lt;br /&gt;
These experiments benefitted from a clear understanding of fly biology, and did not measure conscious motion detection, but neuron-level detection within the lobula plate.  The flies had their heads opened and trachea and air sacs removed so that the lobula plate could be imaged directly from above; those subject to the higher SNR-requirement two-photon microscopy also had their proboscis and gut removed (they produce occasional reflexive signals).  Images were taken with a 64x64 pixel camera and transformed from fuorescence changes into projected DC + AC signal. &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
Results at all signal levels matched what would be expected of Reichardt detectors, and while there were some variations in response at different levels of signal intensity, no hallmarks of gradient detection were seen.&lt;br /&gt;
&lt;br /&gt;
This held true up to pattern contrasts of ~90% and luminance of 200cd/m^2, close to broad daylight.  Additionally, the total variation in [Ca2+] at the dendritic fringe increased with increasing contrast, the opposite of what might be expected with a gradient detector.&lt;br /&gt;
&lt;br /&gt;
This demonstrated that Reichardt detectors seem to model the mechanism of direction selectivity in fly neurons of the lobular plate, up to fairly high contrast and illumination levels, close to the maximum that flies are thought to distinguish.  While it cannot rule out the possibility of a mechanism like a gradient detector in use in the visual system, this is a strong indication that gradient detectors are not needed for effective motion detection. &lt;br /&gt;
&lt;br /&gt;
Three outstanding questions are noted as remaining support the idea that something other than Reichardt detectors, perhaps gradient detection, is involved in some regimes.  One is theoretical: a naive analysis suggests that gradient detectors would be the simplest, and perhaps most efficient, detection scheme.  If this is not true in any regime, where does the simple model fail?  And a few experimental results are also unexplained: &lt;br /&gt;
* Reichardt detectors have a quadratic relationship between signal amplitude and stimulus contrast.  But this becomes contrast-independent slightly above 10% contrast, in Drosophila, Musca, and others.   &lt;br /&gt;
* Humans perceive low-contrast gratings to be slower than high-contrast gratings. &lt;br /&gt;
* Srinivasan (1991) notes free-flying honey bees moving through a tunnel can detect actual image velocity, not just pattern wavelength. &lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* [[:File:Reichardt-forever.pdf|Visual summary]] (presentation form, pdf)&lt;br /&gt;
* M. V. Srinivasan, M. Lehrer, W. H. Kirchner, S. W. Zhang (1991) Visual Neuroscience 6.&lt;br /&gt;
|relevance=This is a concise demonstration that a Reichardt-detector process, or something very close to it, continues to be the dominant way gradients and edges are detected in fly vision, even in environments with low noise.  &lt;br /&gt;
&lt;br /&gt;
Historically, gradient detection has been a top contender for a mechanism for vision in low-noise environments, because of their theoretical simplicity and high precision.  This experiment tried two unrelated methods of finding indications of gradient detection in fly vision, removing much more noise from their method and increasing the signal dramatically beyond previous experiments; but without success.&lt;br /&gt;
|journal=PNAS&lt;br /&gt;
|pub_date=2004/11/01&lt;br /&gt;
|doi=10.1073/pnas.0407368101&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User_talk:Aaronshaw&amp;diff=8995</id>
		<title>User talk:Aaronshaw</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User_talk:Aaronshaw&amp;diff=8995"/>
		<updated>2013-01-03T05:03:59Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;'''Go for it!'''&lt;br /&gt;
&lt;br /&gt;
{{Welcome|name=Aaron}}&lt;br /&gt;
PS-As far as import from Zotero goes, I think the summary has to be in a particular field. Abstract, maybe? [[User:Jodi.a.schneider|Jodi.a.schneider]] 08:08, 2 July 2010 (UTC)&lt;br /&gt;
&lt;br /&gt;
: Hi there, stranger :) [[User:Sj|Sj]] 06:03, 3 January 2013 (CET)&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User_talk:Sj&amp;diff=8994</id>
		<title>User talk:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User_talk:Sj&amp;diff=8994"/>
		<updated>2013-01-03T05:02:46Z</updated>

		<summary type="html">&lt;p&gt;Sj: /* Welcome */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Hello, welcome to my talk page.  You can [http://acawiki.org/index.php?title=User_talk:Sj&amp;amp;action=edit&amp;amp;section=new leave me a message here], or leave me one on the [[m:user talk:sj|Meta-wiki]] for fastest response.  [[User:Sj|Sj]]&lt;br /&gt;
&lt;br /&gt;
== Welcome ==&lt;br /&gt;
&lt;br /&gt;
Welcome to Acawiki! Glad to see you around here as well! Thanks so much for your contributions! I look forward to reading more! —&amp;lt;b&amp;gt;[[User:Benjamin Mako Hill|&amp;lt;font color=&amp;quot;#C40099&amp;quot;&amp;gt;m&amp;lt;/font&amp;gt;&amp;lt;font color=&amp;quot;#600099&amp;quot;&amp;gt;a&amp;lt;/font&amp;gt;&amp;lt;font color=&amp;quot;#2D0399&amp;quot;&amp;gt;k&amp;lt;/font&amp;gt;&amp;lt;font color=&amp;quot;#362365&amp;quot;&amp;gt;o&amp;lt;/font&amp;gt;]][[User talk:Benjamin Mako Hill|&amp;lt;font color=&amp;quot;#000000&amp;quot;&amp;gt;๛&amp;lt;/font&amp;gt;]]&amp;lt;/b&amp;gt; 00:48, 3 January 2013 (CET)&lt;br /&gt;
: Hey thanks.  Using the site for a couple weeks made me think more deeply about how to handle citations.  And how to get this hosted on a faster server :)  [[User:Sj|Sj]] 06:02, 3 January 2013 (CET)&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8993</id>
		<title>Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8993"/>
		<updated>2013-01-03T04:52:33Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio&lt;br /&gt;
|authors=J Haag, W Denk, A Borst&lt;br /&gt;
|url=http://adsabs.harvard.edu/abs/2004PNAS..10116333H&lt;br /&gt;
|tags=vision algorithms, edge detection&lt;br /&gt;
|summary=It has been theorized that fly vision might switch from relying on Reichardt detectors to relying on some other mechanism such as gradient detectors in high signal-to-noise regimes.  This paper summarizes two experiments probing those regimes and testing different parts of the fly vision chain, and finds no evidence for any mechanism other than Reichardt detectors.  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
Gradient detectors are still considered a competing mechanism to Reichardt detectors in high signal-to-noise regimes.  And in order to work with elementary responses, experiments often work at the opposite end of the signal spectrum, aiming for the smallest signal that elicits a measurable response.  As a result few experiments have been carried out to test whether markers of gradient detection can be observed in fly motion vision under any circumstances.&lt;br /&gt;
&lt;br /&gt;
This paper describes two experiments to evaluate the hypothesis that gradient detectors are not part of the fly motion pathways at all. Both study direction selectivity in flies, the canonical test for fly motion vision.  &lt;br /&gt;
&lt;br /&gt;
One experiment tested for the dependence of optimal stimulus 'velocity' (the actual velocity of the pattern used as a stimulus) on the wavelength of the pattern.  This is expected to be directly correlated in the Reichardt detector case, and relatively uncorrelated in the gradient detector case.  It was simply measured by looking at neuron spikes of the motion-sensitive neuron H1.  This test was repeated over a wide range of mean luminance and of stimulus contrast (roughly 2 magnitudes in each case).&lt;br /&gt;
&lt;br /&gt;
The second more complex experiment improved on a traditional experiment to show Reichardt detection: observing the local modulations in signal along a dendrite as a pattern moves past it.  In the Reichardt case this is expected to move synchronous with the pattern, and to be phase-shifted along different parts of the dendrite.  However this was always previously done with 1-photon imaging, which has a side-effect of false positives that limits how small overall noise could be in such an experiment (and so limits the maximum pattern contrast).   This is addressed here by using 2-photon microscopy with luminescent Calcium markers, a technique that allows very high signal without false-positive noise.  Neurons of both vertical and horizontal systems were observed.&lt;br /&gt;
&lt;br /&gt;
These experiments benefitted from a clear understanding of fly biology, and did not measure conscious motion detection, but neuron-level detection within the lobula plate.  The flies had their heads opened and trachea and air sacs removed so that the lobula plate could be imaged directly from above; those subject to the higher SNR-requirement two-photon microscopy also had their proboscis and gut removed (they produce occasional reflexive signals).  Images were taken with a 64x64 pixel camera and transformed from fuorescence changes into projected DC + AC signal. &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
Results at all signal levels matched what would be expected of Reichardt detectors, and while there were some variations in response at different levels of signal intensity, no hallmarks of gradient detection were seen.&lt;br /&gt;
&lt;br /&gt;
This held true up to pattern contrasts of ~90% and luminance of 200cd/m^2, close to broad daylight.  Additionally, the total variation in [Ca2+] at the dendritic fringe increased with increasing contrast, the opposite of what might be expected with a gradient detector.&lt;br /&gt;
&lt;br /&gt;
This demonstrated that Reichardt detectors seem to model the mechanism of direction selectivity in fly neurons of the lobular plate, up to fairly high contrast and illumination levels, close to the maximum that flies are thought to distinguish.  While it cannot rule out the possibility of a mechanism like a gradient detector in use in the visual system, this is a strong indication that gradient detectors are not needed for effective motion detection. &lt;br /&gt;
&lt;br /&gt;
Three outstanding questions are noted as remaining support the idea that something other than Reichardt detectors, perhaps gradient detection, is involved in some regimes.  One is theoretical: a naive analysis suggests that gradient detectors would be the simplest, and perhaps most efficient, detection scheme.  If this is not true in any regime, where does the simple model fail?  And a few experimental results are also unexplained: &lt;br /&gt;
* Reichardt detectors have a quadratic relationship between signal amplitude and stimulus contrast.  But this becomes contrast-independent slightly above 10% contrast, in Drosophila, Musca, and others.   &lt;br /&gt;
* Humans perceive low-contrast gratings to be slower than high-contrast gratings. &lt;br /&gt;
* Srinivasan (1991) notes free-flying honey bees moving through a tunnel can detect actual image velocity, not just pattern wavelength. &lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* [[:File:Reichardt-forever.pdf|Visual summary]] (presentation form, pdf)&lt;br /&gt;
* M. V. Srinivasan, M. Lehrer, W. H. Kirchner, S. W. Zhang (1991) Visual Neuroscience 6.&lt;br /&gt;
|relevance=This is a concise demonstration that a Reichardt-detector process, or something very close to it, continues to be the dominant way gradients and edges are detected in fly vision, even in environments with low noise.  &lt;br /&gt;
&lt;br /&gt;
Historically, gradient detection has been a top contender for a mechanism for vision in low-noise environments, because of their theoretical simplicity and high precision.  This experiment tried two unrelated methods of finding indications of gradient detection in fly vision, removing much more noise from their method and increasing the signal dramatically beyond previous experiments; but without success.&lt;br /&gt;
|journal=PNAS&lt;br /&gt;
|pub_date=2004/11/01&lt;br /&gt;
|doi=10.1073/pnas.0407368101&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Mechanisms_Regulating_Variability_of_the_Single_Photon_Responses_of_Mammalian_Rod_Photoreceptors&amp;diff=8928</id>
		<title>Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Mechanisms_Regulating_Variability_of_the_Single_Photon_Responses_of_Mammalian_Rod_Photoreceptors&amp;diff=8928"/>
		<updated>2012-12-16T01:28:12Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors&lt;br /&gt;
|authors=Greg D. Field, Fred Rieke&lt;br /&gt;
|url=http://www.cns.nyu.edu/events/vjclub/archive/field2002.pdf&lt;br /&gt;
|tags=single photon response, photoreceptors, vision&lt;br /&gt;
|summary=Rod photoreceptors have good single-photon responses, but variability in that response limits the accuracy and timing of photon absorption.  This experiment studies how much fluctuation takes place, and what mechanisms are involved.  Rods of mammals and toads are tested to and their fluctuations compared to those of single molecules, to inform a model of single photon response.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
A weak fixed-strength flash was repeated to primate and guinea pig rods.  They both generate quantized responses to such stimulus.  Flash intensity was chosen to stimulate an average of 0.5 photoisomerization of Rhodopsin.  The dominant source of variability trial to trial in the response was expected to be Poisson fluctuation in the base current and the photon response.&lt;br /&gt;
&lt;br /&gt;
Single photon response was separated from failures (no response) and multiphoton response (easy to identify as a multiple of the single-photon resopnse - either 2x or 3x).  This was made easier by the weakness of the flash.&lt;br /&gt;
&lt;br /&gt;
Singles and failures were isolated across 3-4 flash strengths from each tested cell, to analyze contamination: as measured by the lack of dependence of isolated singles.  Rods with little observed contamination were used for the rest of the experiment.   &lt;br /&gt;
&lt;br /&gt;
Mechanisms were identified that might limit the single photon response:&lt;br /&gt;
# Local depletion of cGMP&lt;br /&gt;
# Depletion of the available transducin or PDE&lt;br /&gt;
# Feedback loops in rhodopsin activity&lt;br /&gt;
# Multistep shutoff&lt;br /&gt;
&lt;br /&gt;
The first would imply different results from uniform and localized illumination, which was not observed.  The second, third, and fourth were all parameterized and optimized to try to fit the observed mean data.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The fluctuations of rod responses to single photons are 3-4x smaller than other biological signals produced by single molecules.  This data is used to constrain models for how that photon response is controlled.&lt;br /&gt;
&lt;br /&gt;
Simple feedback of rhodopsin activity or transduction cascade saturation alone could not produce the observed results - they were perhaps too simple but also had the wrong relationwhip between their mean and variance. . The best model for single photon response identified was a multistep process involving some combination of rhodopsin shutoff and saturation.&lt;br /&gt;
&lt;br /&gt;
This model was then applied to the shape of the response curve under the load of a buffer (BAPTA).  Without changing the parameters of the model, it continued to fit this new scenario well.  Combinations of most models failed to improve on the multistep model, but a saturation + multistep model could potentially reduce the number of steps.  &lt;br /&gt;
&lt;br /&gt;
The authors however suggest that a multistep shutoff alone is the most likely candidate process. In this case molecular constraints on rhodopsin activation and reaction rates would include the need to have reverse rate constants ~20x smaller than the forward constant for a 10-step process. That would require a large free energy difference between active and inactive rhodopsin - in this case on the order of 20kcal/mol.&lt;br /&gt;
&lt;br /&gt;
|relevance=This provides baseline data on the fluctuations of mammalian rods to photons, and suggests a multistep model for rhodopsin shutoff and saturation that could account for it.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2002/08/15&lt;br /&gt;
|doi=10.1016/S0896-6273(02)00822-X&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8926</id>
		<title>Defining the Computational Structure of the Motion Detector in Drosophila</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8926"/>
		<updated>2012-12-16T00:43:18Z</updated>

		<summary type="html">&lt;p&gt;Sj: moved Deﬁning the Computational Structure of the Motion Detector in Drosophila to Defining the Computational Structure of the Motion Detector in Drosophila&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Deﬁning the Computational Structure of the Motion Detector in Drosophila&lt;br /&gt;
|authors=Damon A. Clark, Limor Bursztyn, Mark A. Horowitz, Mark J. Schnitzer, Thomas R. Clandinin&lt;br /&gt;
|url=http://www.cell.com/neuron/retrieve/pii/S0896627311004417&lt;br /&gt;
|tags=Drosophila, Reichardt detector, vision, motion&lt;br /&gt;
|summary=This paper tests the hypothesis that information about motion is extracted from shifting intensity patterns  on the back of the retina.  It shows that a Reichardt-detector model can closely match the neuronal response to visual inputs, and identifies two specific pathways that may carry out pieces of the related computation.  &lt;br /&gt;
&lt;br /&gt;
These two pathways (via laminar cells L1 and L2) are shown to respond differently to light vs. dark moving edges, and it is shown they both carry out part of the idealized computation described by a Reichardt detector.  A theoretical model is proposed that would be tuneable to match observed responses closely (possibly changing over time).  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
These experiments probe the structure and possible component parts of the part of motion detection in Drosophila that responds to moving edges like a Reichardt detector.  While no specific physical components have been identified as carrying out the individual steps of the Reichardt detector algorithm, this work tests the hypothesis that two pathways map to specific subsets of the overall Reichardt computation. &lt;br /&gt;
&lt;br /&gt;
Directional selectivity of flies is observed in response to light and dark edges in intensity patterns, the traditional input used to characterize Reichardt detection.  Responses to &amp;quot;phi&amp;quot; and &amp;quot;reverse phi&amp;quot; stimuli are also observed: changes in contrast in the same direction or in opposite direction.  Reverse phi is related to an illusion: it causes the observer to turn in the opposite direction that the spatial sequence of contrast change would -- into rather than away from an edge.  As it is also observed in animals other than flies, this suggests some overlap in analysis for future study.&lt;br /&gt;
&lt;br /&gt;
In this experiment the flies studied are conscious and held in place suspended just above a ball, which floats at low friction in an airstream.  The fly can move its legs to 'walk' along the ball, and the rotation of the ball captures its motion.  While in this setup, the flies are shown three screens, ahead and to the left and right; shown the image of a rotationg virtual cylinder with periodic patterns. &lt;br /&gt;
&lt;br /&gt;
First the response of wild-type Drosophila's Reichart correlation is characterized, by showing them two bars side by side, with a randomized range of contrast changes and time delays between successive images.  They are also shown rotating cylinders with a fixed periodic square wave.&lt;br /&gt;
Genetically modified Drosophila missing either the L1 or L2 pathway are then bred and tested with the same system.   &lt;br /&gt;
&lt;br /&gt;
Various tests of the L1 and L2 terminals are carried out to see whether each of them responded to both light and dark stimuli in isolation, and to both increases and decreases in intensity.  The response of flies to both phi and reverse phi stimuli are noted and compared to motion sensing in other species. &lt;br /&gt;
&lt;br /&gt;
To understand the role and function of edge selectivity in the L1 and L2 pathways, flies with only one or the other are shown a variety of inputs to find differential responses: including light-light, dark-dark, and phi and revers-phi stimuli.  &lt;br /&gt;
&lt;br /&gt;
It is a point of contemporary debate whether all four possible unit computations of the Reichardt detector are carried out: dark-dark, dark-light, light-dark, light-light.  Drosophila are shown not only the four combinations of dark and light bars, but also phi and reverse-phi stimuli.  Reverse phi stimuli are predicted to produce the opposite response of phi stimuli if all four computations are possible. &lt;br /&gt;
&lt;br /&gt;
A numerical model is developed to match observed edge preferences and responses, with parameters weighting the individual computations of the Reichardt detector to fit observations.&lt;br /&gt;
&lt;br /&gt;
Finally, the implications of two distinct pathways within each Reichardt detector process, for fly motion detection and for understanding other observations of fly neuron responses, are analyzed.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The fly response to randomly generated bars roughly matches that of an ideal Reichardt correlator.&lt;br /&gt;
&lt;br /&gt;
Losing L1 reduces response to only the light edges; losing L2 reduces response to only dark edges.  To distinguish edge detection from overall changes in light level, an equiluminant stimulus is developed where light and dark edges move in opposite directions at equal speeds, at once.  Control flies move only slightly; those without L1 turn towards the dark edge, those without L2 turned towards the light.  &lt;br /&gt;
&lt;br /&gt;
This strongly suggests that L1 and L2 pathways are tied to the ability to detect motion of light and dark edges, respectively.  However both L1 and L2 are found to respond similarly to light and dark flashes, and to respond to the motion of both light and dark edges.   They also respond highly linearly to changes in contrast - either increases or decreases.  In contrast to contemporary work that suggested L2 terminals respond to decreases and not increases in brightness, this is shown to be linear quite uniformly across the spectrum of stimulus intensity.&lt;br /&gt;
&lt;br /&gt;
As reverse phi stimuli produce the response predicted by a full Reichardt detector, the authors concluded that all four unit compoutations are carried out.  This did not entirely settle the question for other researchers however.  Reverse phi stimuli had another interesting property: they produced different complementary responses in flies missing L1 or L2 pathways. &lt;br /&gt;
&lt;br /&gt;
To understand this better, a numerical model is designed for an array of Reichardt detectors, with responses to phi and reverse-phi inputs tuned by weighting the four different unit multiplications in the detector.  Weighting phi stimuli equally while weighting reverse-stimuli differentially is enough to reproduce the edge-selction seen in L1 and L2 pathways.  &lt;br /&gt;
&lt;br /&gt;
As reverse phi responses are observed in many species other than Drosophila, the analysis and model presented at the end of this study are of potential interest to studies of edge and motion detection in other creatures.&lt;br /&gt;
&lt;br /&gt;
; Notes for future and contemporary researchers&lt;br /&gt;
The idea of half-wave rectification of the signal at each input has often been proposed since it is not known how sign-correct multiplication of inputs could be implemented.  Rectification may happen elsewhere in the neural circuit, however.  These experiments demonstrate that the L1 and L2 cells do not themselves carry out such rectification.   &lt;br /&gt;
&lt;br /&gt;
The authors tackle the ongoing debate between &amp;quot;two-computation&amp;quot; and &amp;quot;four-computation&amp;quot; models of a Reichardt detector, which are related to ideas about whether the fly visual system is organized into ON and OFF pathways or simply detecting light v. dark edges.  They conclude from their work that the fly visual system is not organized into ON / OFF pathways -- that is, that L1  transmits information about more than just increases in contrast, and L2 transmits information about more than just decreases.  This is in contrast to Joesch and Eichner. &lt;br /&gt;
&lt;br /&gt;
A few time dependencies are noted related to the laminar cells, as pointers to future study.  The flies studied remember the last image they had seen for at least 1 second for the purposes of future reactions.  L1 and L2 terminals show different kinetics in respond to prolonged stimuli.  And previous work suggests that electrical changes in the cell membrane potential would last for 50-100ms, in contrast to the Ca responses in axonal terminals that last for seconds.  This could indicate adaptation of the synapse, or processing within the axon.  &lt;br /&gt;
&lt;br /&gt;
Reverse phi is proposed as more than an illusion - but as a specific sort of motion captured by neurons, with functional use.  In humans for instance, reverse phi shares properties with motion aftereffects, and may contribute to perception of moving edges of a specific polarity.  Edge-detecting cells are a fundamental unit of visual computation, and this work suggests edge-polarity detection is as well.  &lt;br /&gt;
&lt;br /&gt;
Finally, as demonstrated most concisely in the numerical model presented, edge selectivity can be characterized by selective weighting of L1 and L2 pathways.  Furthermore, this study may only have captured a subset of the actual computations carried out.  Other cells may be involved as well - L4 cells may have a significant role to play.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* See [[Internal Structure of the Fly Elementary Motion Detector]], Eichner, Joesch, Schnell, Reiff, and Borst. Neuron, 2011 (published in the same issue, back to back).  An earlier related work by Joesh is referenced in this paper.&lt;br /&gt;
* [[Phi movement as a subtraction process]]. S.M. Anstis, Vision. (1970)&lt;br /&gt;
&lt;br /&gt;
|relevance=Changes in light and shadow over time and space are shown to be detected by a system that closely parallels a simple Reichardt detector  (or Hassenstein-Reichardt correlator).  A model for such a detector is proposed that can be tuned to detect moving edges of contrast.  &lt;br /&gt;
 &lt;br /&gt;
This clearly distinguished two different neuronal pathways (L1 and L2) as responsible for different parts of  vision,  by selectively disabling each one separately and quantifying the different changes in edge detection.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2011&lt;br /&gt;
|doi=10.1016/j.neuron.2011.05.023&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=De%EF%AC%81ning_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8927</id>
		<title>Deﬁning the Computational Structure of the Motion Detector in Drosophila</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=De%EF%AC%81ning_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8927"/>
		<updated>2012-12-16T00:43:18Z</updated>

		<summary type="html">&lt;p&gt;Sj: moved Deﬁning the Computational Structure of the Motion Detector in Drosophila to Defining the Computational Structure of the Motion Detector in Drosophila&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;#REDIRECT [[Defining the Computational Structure of the Motion Detector in Drosophila]]&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Unitary_response_of_mouse_olfactory_receptor_neurons&amp;diff=8925</id>
		<title>Unitary response of mouse olfactory receptor neurons</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Unitary_response_of_mouse_olfactory_receptor_neurons&amp;diff=8925"/>
		<updated>2012-12-16T00:28:34Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Unitary response of mouse olfactory receptor neurons&lt;br /&gt;
|authors=Yair Ben-Chaim, Melody M. Cheng, King-Wai Yau&lt;br /&gt;
|url=http://www.pnas.org/content/108/2/822&lt;br /&gt;
|tags=olfaction, mouse&lt;br /&gt;
|summary=This paper studies the response of mouse olfactory receptor neurons [ORNs] to a variety of odorants, and notes that the response is relatively uniform in amplitude and kinetics, unchanging across different neurons and different odors (hence 'elementary' or 'unitary' - responding to the entire experience of a novel smell as a single smelling-event).  The experiment involved followed earlier work by Yau and others on frog ORNs, showing that the same results hold for mice and so possibly for other mammals.  &lt;br /&gt;
&lt;br /&gt;
The olfactory response similar for different clusters of odorants  it had little amplification, triggering transduction through only just single molecular complex.  Successful response required only O(10) successful binding events.  Both traits are similar to the results found for frog ORNs in the earlier work. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The primary goal was to check the similarity between responses of mouse and frog ORNs to address the question of whether the properties of olfactory response in mammals might have similar traits.  Existing methodology was repeated with mouse cells: short bursts of odorants, varying either the concentration in bursts of fixed length or the length of bursts of fixed concentration.  &lt;br /&gt;
&lt;br /&gt;
The method used carried out a quantal analysis on results, assuming there was a minimum unitary response, and a Poisson distribution of individual responses.  The suction-pipette method was used to measure membrane currents.  As there are 1000 species of OR cells, a mixture of five odorants was used instead of two.&lt;br /&gt;
&lt;br /&gt;
Temperature effects were also studied - the most detailed experiment was run at room temperature, as the cells did not last as long at higher temperatures, but macroscopic analysis of cell behavior at 35 C was evaluated for differences.  &lt;br /&gt;
&lt;br /&gt;
The threshold number of binding events to trigger an action potential to the brain was measured, to provide a bound on the sensitivity threshold for olfaction.   &lt;br /&gt;
 &lt;br /&gt;
Finally, additional experiments were carried out to test the dependence of the concentration of G proteins on output signal strength.  Cells from adult mice that expressed half of the normal level of G protein involved in odorant activation were compared with those from mice with normal expression.  &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The overall process of olfaction in mouse ORNs seems to match that observed in frog ORNs. &lt;br /&gt;
The unitary response was the same across odorants and cells, even though the odorants varied in efficacy and each cell had different conditions and receptors.  &lt;br /&gt;
&lt;br /&gt;
The unitary response of neurons from mice with less of the needed G protein was also the same.  This adds evidence to the theory that there is little or no amplification cascade involving those proteins, which would otherwise have a nonlinear response varying with their density.  &lt;br /&gt;
&lt;br /&gt;
The total number of receptor bindings needed to signal the brain was estimated at 20-25 unitary events, increasing slightly at lower (room) temperature.  This is comparable to the 35 events predicted as a threshold upper bound for frog ORNs. &lt;br /&gt;
&lt;br /&gt;
Some parts of this analysis differed significantly from the frog ORN study.  A completely Ca2+-free solution was used, which avoids negative feedback and adaptation, but also enhances receptor current via an inward Cl- current.  &lt;br /&gt;
&lt;br /&gt;
Further study is needed on the olfactory threshold at consciousness.  &lt;br /&gt;
It is hypothesized that it may require only one or a few ORNs are needed to trigger perception.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]] . V Bhandawat, J Reisert, K-W Yau, Science (2005)&lt;br /&gt;
* [[Signaling by olfactory receptor neurons near threshold]]. V Bhandaat, J Reisert, K-W Yau, PNAS (2010)&lt;br /&gt;
* [[The electrochemical basis of odor transduction in vertebrate olfactory cilia]].  SJ Kleene, Chem Senses (2008)&lt;br /&gt;
|relevance=This paper replicates the results of [[Elementary Response of Olfactory Receptor Neurons to Odorants|Bhandawat, Reisert, and Yau]] (which used frog ORNs) with mouse ORNs.  It confirms the low amplification of smells at the single-neuron level, and provides a first upper bound on the number of odorant-binding events needed to trigger a signal in an ORN.&lt;br /&gt;
|journal=PNAS&lt;br /&gt;
|pub_date=2011/01/11&lt;br /&gt;
|doi=10.1073/pnas.1017983108&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8924</id>
		<title>Energy, Quanta, and Vision</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8924"/>
		<updated>2012-12-16T00:22:40Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Energy, Quanta, and Vision&lt;br /&gt;
|authors=Selig Hecht, Simon Shlaer, Maurice Henri Pirenne&lt;br /&gt;
|url=http://www.ncbi.nlm.nih.gov/pmc/articles/PMC2142545/pdf/819.pdf&lt;br /&gt;
|tags=vision quanta light eye&lt;br /&gt;
|summary=The authors note that there have been many studies of the visual threshold of the human eye, many improving on those before.   This paper includes a survey and history of experiments in the area, notes some inadequacies in past work and opportunity for improvement, and lays out and implements a new technique for measuring visual sensitivity.  Their practical noise-reduction is somewhat better than previous experiments, and they add a widely useful statistical technique that allows for a much stronger signal to be extracted from the intrinsically noisy data of observation.  &lt;br /&gt;
&lt;br /&gt;
The result is both a new and lower upper bound on the visual threshold, and a useful exercise in statistical data analysis.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The question of the fundamental sensitivity of the human eye is a long-standing one, and had been tested sporadically for decades.  This experiment reduced noise in a few ways, and analyzed the results assuming detection and observation of light would follow a Poisson distribution.&lt;br /&gt;
&lt;br /&gt;
;Noise reduction and measurement:&lt;br /&gt;
* Subjects were adapted to the dark for 40 minutes, &lt;br /&gt;
* Light was focused on an area in the retina's peripheral vision (where light response is optimal)&lt;br /&gt;
* Light was flashed at 510nm, a wavelength we are particularly sensitive to&lt;br /&gt;
* Flashes of 1 ms and a spot size smaller than 10 arcminutes were chosen.  A set of diaphragms and filters were used to vary the spot size and brightness without moving the rest of the setup.  The flashes were generated using a circular shutter with a tiny hole cut in it, rotating so quickly that at any give moment it lets light through for 0.001 s of a revolution&lt;br /&gt;
* All light was carefully passed through an equal thickness of glass for uniform illumination, with entrance and exist slits both 1.2mm wide, corresponding to the desired bandwidth of the beam.  &lt;br /&gt;
* A red light was provided to help fixate the eye so it did not jitter.  &lt;br /&gt;
&lt;br /&gt;
Measurements were taken with this apparatus over the course of two years and seven subjects.  Each of a series of intensities was presented many times, with the frequency of seeing a flash determined for each intensity, and calculating the associated number of quanta sent to the eye. &lt;br /&gt;
&lt;br /&gt;
This and the rest of the experiment assume that observer response is intrinsically probabilistic.  The participants in the study were trained to say they had seen a light only if they were sure, to minimize false positives.  A threshold was defined as the intensity which could be seen with a 60% frequency.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
;Light intensity and absorption&lt;br /&gt;
One of the more careful aspects of this paper is its analysis of reflection and absorption of light by the eye, and the estimated portion of light that reaches the retina.  &lt;br /&gt;
&lt;br /&gt;
The details of the filter and the light source were calibrated (more han once, to ensure constancy) so as to estimate the energy density sent to the pupil.  This was varied over the course of the experiment, and used as a gauge of how many quanta of light had potentially been absorbed by the eye.   &lt;br /&gt;
&lt;br /&gt;
Based on the absorption analysis, the number of quanta ''absorbed'' by the eye can be estimated from the total light intensity.  &lt;br /&gt;
&lt;br /&gt;
This suggested a value lower than any found in previous experiments.  So an additional statistical  model is used to cross-check the result, based on the Poisson distribution of light emitted in any one flash.  &lt;br /&gt;
&lt;br /&gt;
The probability of a given flash being observed is then assumed to be the probability that more than a hidden threshhold of quanta are detected by the eye.  In this version of the model it is primarily the signal  that varies -- whenever the signal passes some threshold, it is assumed to be seen.  However it is noted that human variability combines with the signal variability in this case and is not a significant factor in the analysis. &lt;br /&gt;
&lt;br /&gt;
The threshold estimated by this was compared to that estimated by calculating the % of total photons absorbed by the eye.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
Contemporary studies were used to estimate that 50% of light is transmitted through the cornea, and an upper limit of 20% of impinging light absorbed by retinal pigments (visual purple).  The latter is estimated anew in this paper based on data from frog retinas and pigment density.   Earlier work by Hecht provided data on scoptopic luminosity at the retina and the optimal frequency for detection.   This would mean a total absorption of 10% of incoming photons.&lt;br /&gt;
&lt;br /&gt;
The total energy density at the cornea is 54-148 quanta of light, which maps to 5-14 quanta absorbed by rods.  This is over a field of ~500 rods, suggesting that no rod absorbs more than one.&lt;br /&gt;
&lt;br /&gt;
For the statistical comparison, it is noted that the absolute threshold for vision seems to be small - 5 to 8 quanta.  And that this statistical estimate is easier to see when the total number of detections is small.  Variation in the biological capacity of the participants doesn't effect this analysis much.  So the agreement between this estimate and the energy-absorption estimate is significant.&lt;br /&gt;
&lt;br /&gt;
This suggests that, while in the past it has been assumed that light stimulus is constant and the observer variable, the primary factor in light detection is the variability of the signal.&lt;br /&gt;
&lt;br /&gt;
Future experiment is needed to determine whether there are differential threshold at some level of intensity, separate from the absolute threshold, for which a small number of events determines the differentiation.  Moreover, this is simply an upper bound, and the bound used to identify the number of photons absorbed by the retina is noted to seem high by a factor of 2.   The paper did not dwell on the training of the observers (most of whom were also co-authors).  However later studies would make a point of training people differently to note uncertainty differently than they note definite non-observation of light - a variation that lowers the threshold further.&lt;br /&gt;
|relevance=This paper has become a canonical reference for any discussion about how sensitive the human eye is to individual quanta of light.  While it was not the first to ask the question and carry out experiments to measure how small a signal was needed to stimulate the eye, it used a simple and universal technique, was careful in its error analysis, and compared its work cleanly with those of past attempts to measure the visual threshold.  Previous estimates of the visual threshhold were on the order of 20 quanta of light; this work used statistical analysis to reduce that to 5-7.&lt;br /&gt;
|journal=The Journal of General Physiology&lt;br /&gt;
|pub_date=1942&lt;br /&gt;
|doi=10.1085/jgp.25.6.819&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8923</id>
		<title>Energy, Quanta, and Vision</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8923"/>
		<updated>2012-12-16T00:22:26Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Energy, Quanta, and Vision&lt;br /&gt;
|authors=Selig Hecht, Simon Shlaer, Maurice Henri Pirenne&lt;br /&gt;
|url=http://www.ncbi.nlm.nih.gov/pmc/articles/PMC2142545/pdf/819.pdf&lt;br /&gt;
|tags=vision quanta light eye&lt;br /&gt;
|summary=The authors note that there have been many studies of the visual threshold of the human eye, many improving on those before.   This paper includes a survey and history of experiments in the area, notes some inadequacies in past work and opportunity for improvement, and lays out and implements a new technique for measuring visual sensitivity.  Their practical noise-reduction is somewhat better than previous experiments, and they add a widely useful statistical technique that allows for a much stronger signal to be extracted from the intrinsically noisy data of observation.  &lt;br /&gt;
&lt;br /&gt;
The result is both a new and lower upper bound on the visual threshold, and a useful exercise in statistical data analysis.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The question of the fundamental sensitivity of the human eye is a long-standing one, and had been tested sporadically for decades.  This experiment reduced noise in a few ways, and analyzed the results assuming detection and observation of light would follow a Poisson distribution.&lt;br /&gt;
&lt;br /&gt;
;Noise reduction and measurement:&lt;br /&gt;
* Subjects were adapted to the dark for 40 minutes, &lt;br /&gt;
* Light was focused on an area in the retina's peripheral vision (where light response is optimal)&lt;br /&gt;
* Light was flashed at 510nm, a wavelength we are particularly sensitive to&lt;br /&gt;
* Flashes of 1 ms and a spot size smaller than 10 arcminutes were chosen.  A set of diaphragms and filters were used to vary the spot size and brightness without moving the rest of the setup.  The flashes were generated using a circular shutter with a tiny hole cut in it, rotating so quickly that at any give moment it lets light through for 0.001 s of a revolution&lt;br /&gt;
* All light was carefully passed through an equal thickness of glass for uniform illumination, with entrance and exist slits both 1.2mm wide, corresponding to the desired bandwidth of the beam.  &lt;br /&gt;
* A red light was provided to help fixate the eye so it did not jitter.  &lt;br /&gt;
&lt;br /&gt;
Measurements were taken with this apparatus over the course of two years and seven subjects.  Each of a series of intensities was presented many times, with the frequency of seeing a flash determined for each intensity, and calculating the associated number of quanta sent to the eye. &lt;br /&gt;
&lt;br /&gt;
This and the rest of the experiment assume that observer response is intrinsically probabilistic.  The participants in the study were trained to say they had seen a light only if they were sure, to minimize false positives.  A threshold was defined as the intensity which could be seen with a 60% frequency.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
;Light intensity and absorption&lt;br /&gt;
One of the more careful aspects of this paper is its analysis of reflection and absorption of light by the eye, and the estimated portion of light that reaches the retina.  &lt;br /&gt;
&lt;br /&gt;
The details of the filter and the light source were calibrated (more han once, to ensure constancy) so as to estimate the energy density sent to the pupil.  This was varied over the course of the experiment, and used as a gauge of how many quanta of light had potentially been absorbed by the eye.   &lt;br /&gt;
&lt;br /&gt;
Based on the absorption analysis, the number of quanta ''absorbed'' by the eye can be estimated from the total light intensity.  &lt;br /&gt;
&lt;br /&gt;
This suggested a value lower than any found in previous experiments.  So an additional statistical  model is used to cross-check the result, based on the Poisson distribution of light emitted in any one flash.  &lt;br /&gt;
&lt;br /&gt;
The probability of a given flash being observed is then assumed to be the probability that more than a hidden threshhold of quanta are detected by the eye.  In this version of the model it is primarily the signal  that varies -- whenever the signal passes some threshold, it is assumed to be seen.  However it is noted that human variability combines with the signal variability in this case and is not a significant factor in the analysis. &lt;br /&gt;
&lt;br /&gt;
The threshold estimated by this was compared to that estimated by calculating the % of total photons absorbed by the eye.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
Contemporary studies were used to estimate that 50% of light is transmitted through the cornea, and an upper limit of 20% of impinging light absorbed by retinal pigments (visual purple).  The latter is estimated anew in this paper based on data from frog retinas and pigment density.   Earlier work by Hecht provided data on scoptopic luminosity at the retina and the optimal frequency for detection.   This would mean a total absorption of 10% of incoming photons.&lt;br /&gt;
&lt;br /&gt;
The total energy density at the cornea is 54-148 quanta of light, which maps to 5-14 quanta absorbed by rods.  This is over a field of ~500 rods, suggesting that no rod absorbs more than one.&lt;br /&gt;
&lt;br /&gt;
For the statistical comparison, it is noted that the absolute threshold for vision seems to be small - 5 to 8 quanta.  And that this statistical estimate is easier to see when the total number of detections is small.  Variation in the biological capacity of the participants doesn't effect this analysis much.  So the agreement between this estimate and the energy-absorption estimate is significant.&lt;br /&gt;
&lt;br /&gt;
This suggests that, while in the past it has been assumed that light stimulus is constant and the observer variable, the primary factor in light detection is the variability of the signal.&lt;br /&gt;
&lt;br /&gt;
Future experiment is needed to determine whether there are differential threshold at some level of intensity, separate from the absolute threshold, for which a small number of events determines the differentiation.  Moreover, this is simply an upper bound, and the bound used to identify the number of photons absorbed by the retina is noted to seem high by a factor of 2.   The paper did not dwell on the training of the observers (most of whom were also co-authors).  However later studies would make a point of training people differently to note uncertainty differently than they note definite non-observation of light - a variation that lowers the threshold further.&lt;br /&gt;
|relevance=This paper has become a canonical reference for any discussion about how sensitive the human eye is to individual quanta of light.  While it was not the first to ask the question and carry out experiments to measure how small a signal was needed to stimulate the eye, it used a simple and universal technique, was careful in its error analysis, and compared its work cleanly with those of past attempts to measure the visual threshold.  Previous estimates of the visual threshhold were on the order of 20 quanta of light; this work used statistical analysis to reduce that to 5-7.&lt;br /&gt;
|journal=The Journal of General Physiology&lt;br /&gt;
|pub_date=1942&lt;br /&gt;
|doi=10.1085/jgp.25.6.819&lt;br /&gt;
|subject=Biology&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8922</id>
		<title>Energy, Quanta, and Vision</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8922"/>
		<updated>2012-12-16T00:21:49Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Energy, Quanta, and Vision&lt;br /&gt;
|authors=Selig Hecht, Simon Shlaer, Maurice Henri Pirenne&lt;br /&gt;
|url=http://www.ncbi.nlm.nih.gov/pmc/articles/PMC2142545/pdf/819.pdf&lt;br /&gt;
|tags=vision quanta light eye&lt;br /&gt;
|summary=The authors note that there have been many studies of the visual threshold of the human eye, many improving on those before.   This paper includes a survey and history of experiments in the area, notes some inadequacies in past work and opportunity for improvement, and lays out and implements a new technique for measuring visual sensitivity.  Their practical noise-reduction is somewhat better than previous experiments, and they add a widely useful statistical technique that allows for a much stronger signal to be extracted from the intrinsically noisy data of observation.  &lt;br /&gt;
&lt;br /&gt;
The result is both a new and lower upper bound on the visual threshold, and a useful exercise in statistical data analysis.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The question of the fundamental sensitivity of the human eye is a long-standing one, and had been tested sporadically for decades.  This experiment reduced noise in a few ways, and analyzed the results assuming detection and observation of light would follow a Poisson distribution.&lt;br /&gt;
&lt;br /&gt;
;Noise reduction and measurement:&lt;br /&gt;
* Subjects were adapted to the dark for 40 minutes, &lt;br /&gt;
* Light was focused on an area in the retina's peripheral vision (where light response is optimal)&lt;br /&gt;
* Light was flashed at 510nm, a wavelength we are particularly sensitive to&lt;br /&gt;
* Flashes of 1 ms and a spot size smaller than 10 arcminutes were chosen.  A set of diaphragms and filters were used to vary the spot size and brightness without moving the rest of the setup.  The flashes were generated using a circular shutter with a tiny hole cut in it, rotating so quickly that at any give moment it lets light through for 0.001 s of a revolution&lt;br /&gt;
* All light was carefully passed through an equal thickness of glass for uniform illumination, with entrance and exist slits both 1.2mm wide, corresponding to the desired bandwidth of the beam.  &lt;br /&gt;
* A red light was provided to help fixate the eye so it did not jitter.  &lt;br /&gt;
&lt;br /&gt;
Measurements were taken with this apparatus over the course of two years and seven subjects.  Each of a series of intensities was presented many times, with the frequency of seeing a flash determined for each intensity, and calculating the associated number of quanta sent to the eye. &lt;br /&gt;
&lt;br /&gt;
This and the rest of the experiment assume that observer response is intrinsically probabilistic.  The participants in the study were trained to say they had seen a light only if they were sure, to minimize false positives.  A threshold was defined as the intensity which could be seen with a 60% frequency.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
;Light intensity and absorption&lt;br /&gt;
One of the more careful aspects of this paper is its analysis of reflection and absorption of light by the eye, and the estimated portion of light that reaches the retina.  &lt;br /&gt;
&lt;br /&gt;
The details of the filter and the light source were calibrated (more han once, to ensure constancy) so as to estimate the energy density sent to the pupil.  This was varied over the course of the experiment, and used as a gauge of how many quanta of light had potentially been absorbed by the eye.   &lt;br /&gt;
&lt;br /&gt;
Based on the absorption analysis, the number of quanta ''absorbed'' by the eye can be estimated from the total light intensity.  &lt;br /&gt;
&lt;br /&gt;
This suggested a value lower than any found in previous experiments.  So an additional statistical  model is used to cross-check the result, based on the Poisson distribution of light emitted in any one flash.  &lt;br /&gt;
&lt;br /&gt;
The probability of a given flash being observed is then assumed to be the probability that more than a hidden threshhold of quanta are detected by the eye.  In this version of the model it is primarily the signal  that varies -- whenever the signal passes some threshold, it is assumed to be seen.  However it is noted that human variability combines with the signal variability in this case and is not a significant factor in the analysis. &lt;br /&gt;
&lt;br /&gt;
The threshold estimated by this was compared to that estimated by calculating the % of total photons absorbed by the eye.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
Contemporary studies were used to estimate that 50% of light is transmitted through the cornea, and an upper limit of 20% of impinging light absorbed by retinal pigments (visual purple).  The latter is estimated anew in this paper based on data from frog retinas and pigment density.   Earlier work by Hecht provided data on scoptopic luminosity at the retina and the optimal frequency for detection.   This would mean a total absorption of 10% of incoming photons.&lt;br /&gt;
&lt;br /&gt;
The total energy density at the cornea is 54-148 quanta of light, which maps to 5-14 quanta absorbed by rods.  This is over a field of ~500 rods, suggesting that no rod absorbs more than one.&lt;br /&gt;
&lt;br /&gt;
For the statistical comparison, it is noted that the absolute threshold for vision seems to be small - 5 to 8 quanta.  And that this statistical estimate is easier to see when the total number of detections is small.  Variation in the biological capacity of the participants doesn't effect this analysis much.  So the agreement between this estimate and the energy-absorption estimate is significant.&lt;br /&gt;
&lt;br /&gt;
This suggests that, while in the past it has been assumed that light stimulus is constant and the observer variable, the primary factor in light detection is the variability of the signal.&lt;br /&gt;
&lt;br /&gt;
Future experiment is needed to determine whether there are differential threshold at some level of intensity, separate from the absolute threshold, for which a small number of events determines the differentiation.  Moreover, this is simply an upper bound, and the bound used to identify the number of photons absorbed by the retina is noted to seem high by a factor of 2.   The paper did not dwell on the training of the observers (most of whom were also co-authors).  However later studies would make a point of training people differently to note uncertainty differently than they note definite non-observation of light - a variation that lowers the threshold further.&lt;br /&gt;
|relevance=This paper has become a canonical reference for any discussion about how sensitive the human eye is to individual quanta of light.  While it was not the first to ask the question and carry out experiments to measure how small a signal was needed to stimulate the eye, it used a simple and universal technique, was careful in its error analysis, and compared its work cleanly with those of past attempts to measure the visual threshold.  Previous estimates of the visual threshhold were on the order of 20 quanta of light; this work used statistical analysis to reduce that to 5-7.&lt;br /&gt;
|journal=The Journal of General Physiology&lt;br /&gt;
|pub_date=1942&lt;br /&gt;
|subject=Biology&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8921</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8921"/>
		<updated>2012-12-16T00:20:22Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA, USA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein.  I try to keep [[user:Benjamin Mako Hill|Mako]]'s article updates in check. &lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
{| style=&amp;quot;font-size:120%;&amp;quot; width=&amp;quot;100%&amp;quot; cellpadding=0 cellspacing=0&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work]]&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]]&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
|} &lt;br /&gt;
{| style=&amp;quot;font-size:100%;&amp;quot; width=&amp;quot;100%&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;br /&gt;
--&amp;gt;&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8920</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8920"/>
		<updated>2012-12-16T00:19:54Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA, USA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein.  I try to keep [[user:Benjamin Mako Hill|Mako]]'s article updates in check. &lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
{| style=&amp;quot;font-size:100%;&amp;quot; width=&amp;quot;100%&amp;quot; cellpadding=0 cellspacing=0&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work]]&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]]&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
|} &lt;br /&gt;
{| style=&amp;quot;font-size:80%;&amp;quot; width=&amp;quot;100%&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;br /&gt;
--&amp;gt;&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8919</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8919"/>
		<updated>2012-12-16T00:15:04Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA, USA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein.  I try to keep [[user:Benjamin Mako Hill|Mako]]'s article updates in check.&lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
{| style=&amp;quot;font-size:100%;&amp;quot; width=&amp;quot;100%&amp;quot; cellpadding=0 cellspacing=0&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work]]&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]]&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
|} &lt;br /&gt;
{| style=&amp;quot;font-size:80%;&amp;quot; width=&amp;quot;100%&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8918</id>
		<title>Motility-associated hair-bundle motion in mammalian outer hair cells</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8918"/>
		<updated>2012-12-16T00:08:11Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Motility-associated hair-bundle motion in mammalian outer hair cells&lt;br /&gt;
|authors=Shuping Jia, David Z Z He&lt;br /&gt;
|url=http://courses.washington.edu/pbio525/Paper%20PDFs/Jia%202006%20Nat%20Neuro.pdf&lt;br /&gt;
|tags=hearing, cochlea, somatic motility&lt;br /&gt;
|summary=Mammalian hearing depends on mechanical feedback in he cochlea.  The outer hair cells (OHCs) function as the key elements in this feedback loop.   Both somatic motility and &amp;quot;active movement&amp;quot; of hair bundles are considered possible sources of motion-driven cochlear ampliﬁcation.  Active movement is known to be the source of such amplification in non-mammals, where somatic motility does not occur.   This experiment distinguishes which drives movement in part of the mammalian cochlea. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The goal is to distinguish between somatic motility and other active movement of hair bundles in the mammalian cochlea, focusing in part on past studies of gerbils and rats which linked hair bundle movement to active movement for gerbil inner hair cells (IHCs), and rat OHCs. &lt;br /&gt;
&lt;br /&gt;
To gain precision in measurement, cochlea from four groups of subjects were studied: Adult and neonatal gerbils, he latter of which have mechanotransduction but no OHC motility yet; and both wild and prestin-knockout mice, the latter of which have normal hair bundles and mechanotransducer function, but no OHC somatic motility at all.&lt;br /&gt;
&lt;br /&gt;
Somatic motility was measured by applying a voltage across a bundle and looking for voltage-evoked motion.  Mechanotransducer currents were also measured.  To fully separate the functions of the two different source of motion, streptomycin was used as an inhibitor - it entirely blocks mechanotransducer channels and elimiates spontaneous bundle motion.  &lt;br /&gt;
&lt;br /&gt;
Hair motion was measured by looking at the magnified image of bundles at 1260x magnification, in which regime they looked like bright V-shaped lines and movement could be measured at up to 1200 Hz and down to 5nm.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The OHCs showed bundle movement with peak responses of up to 830 nm. The movement was insensitive to manipulations that block mechanotransduction.  Adjacent OHCs were found to move in tandem with a target OHC when somatic motility was applied; a linkage which disappeared when the target OHC lost its turgor pressure.  This suggests the motion resulted from something like rotation of its reticular lamina, a feature of somatic motility.&lt;br /&gt;
&lt;br /&gt;
Finally, movement was entirely absent in neonatal OHCs and prestin-knockout OHCs. This strongly suggests that bundle movement originated in somatic motility for these specieis, and that it plays a central role in cochlear amplification in mammals.&lt;br /&gt;
&lt;br /&gt;
Sharp extracellular potential changes would be needed to drive OHCs at high frequency.  There is evidence that the organ of Corti could provide that drive, and theoretical models of OHC piezoelectric properties suggest ways their frequency response might be increased, addressing one outstanding concern with this theory.&lt;br /&gt;
&lt;br /&gt;
Finally, OHC motility can also stimulate freestanding IHC cilia, leading to their motion as well - formerly attributed to mechanotransduction.  Further study is needed to determine the source of IHC motion.&lt;br /&gt;
|relevance=This study distinguishes between two potential sources of hair-bundle motion: the reclosing of mechanotransduction channels and somatic electromotility.  Previous analyses had mainly demonstrated the possibility of either (including the possible presence of mechanotransduction-driven motion in IHCs of gerbils). &lt;br /&gt;
&lt;br /&gt;
It demonstrate conclusively that such motion is due predominantly to electromotility in the OHCs of some gerbils and mice.  It also suggests ways in which this motion in OHCs might excite IHCs and stimulate observed motion there as well, including possibly the observed motion of gerbil IHCs, which would make electromotility the primary mechanism for cochlear amplification in mammals.  This indicates  avenues for future research.&lt;br /&gt;
|journal=Nature Neuroscience&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=doi:10.1038/nn1509&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Mechanisms_Regulating_Variability_of_the_Single_Photon_Responses_of_Mammalian_Rod_Photoreceptors&amp;diff=8917</id>
		<title>Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Mechanisms_Regulating_Variability_of_the_Single_Photon_Responses_of_Mammalian_Rod_Photoreceptors&amp;diff=8917"/>
		<updated>2012-12-16T00:07:33Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors&lt;br /&gt;
|authors=Greg D. Field, Fred Rieke&lt;br /&gt;
|url=http://www.cns.nyu.edu/events/vjclub/archive/field2002.pdf&lt;br /&gt;
|tags=single photon response, photoreceptors, vision&lt;br /&gt;
|summary=Rod photoreceptors have good single-photon responses, but variability in that response limits the accuracy and timing of photon absorption.  This experiment studies how much fluctuation takes place, and what mechanisms are involved.  Rods of mammals and toads are tested to and their fluctuations compared to those of single molecules, to inform a model of single photon response.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The fluctuations of rod responses to single photons are 3-4x smaller than other biological signals produced by single molecules.  This data is used to constrain models for how that photon response is controlled.&lt;br /&gt;
&lt;br /&gt;
Simple feedback of rhodopsin activity or transduction cascade saturation alone would not produce the observed results. The best model for single photon response identified is a multistep process involving some combination of rhodopsin shutoff and saturation.  &lt;br /&gt;
 &lt;br /&gt;
|relevance=This provides baseline data on the fluctuations of mammalian rods to photons, and suggests a multistep model for rhodopsin shutoff and saturation that could account for it.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2002/08/15&lt;br /&gt;
|doi=10.1016/S0896-6273(02)00822-X&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Internal_Structure_of_the_Fly_Elementary_Motion_Detector&amp;diff=8916</id>
		<title>Internal Structure of the Fly Elementary Motion Detector</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Internal_Structure_of_the_Fly_Elementary_Motion_Detector&amp;diff=8916"/>
		<updated>2012-12-16T00:01:13Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Internal Structure of the Fly Elementary Motion Detector&lt;br /&gt;
|authors=Hubert Eichner, Maximilian Joesch, Bettina Schnell, Dierk F. Reiff, Alexander Borst&lt;br /&gt;
|url=http://www.sciencedirect.com/science/article/pii/S089662731100376X&lt;br /&gt;
|tags=Reichardt detector Drosophila vision motion&lt;br /&gt;
|summary=Building on recent experiments showing that Drosophila motion detection splits the visual input into two parallel (L1 and L2) channels, this study further assumes that those two channels encode increases and decreases in brightness (ON and OFF).  It then maps computations of directional selection to the implementation of an ON/OFF based Reichardt detector.&lt;br /&gt;
&lt;br /&gt;
Under these assumptions, direction-selection is found that matches same-sign but not opposite-sign sequences, suggesting a two-quadrant (2Q) variation of the Reichardt detector.  A model is proposed that both matches current observations and tries to account for past data that was interpreted as supporting four separate components to a (4Q) detector.  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
There are biological and philosophical reasons to imagine that a 2Q detector might be preferably to a 4Q detector: it takes half the energy and biological material, and is known to account for some of the same basic edge detection.  It might also explain how such detectors avoid signed multiplication, a process considered difficult to carry out biologically.  The question is whether it accounts for the full range of motion detection afforded by a 4Q Reichardt detector, and whether it matches observable responses of real flies. &lt;br /&gt;
&lt;br /&gt;
Apparent motion stimuli are used for these experiments, consisting of a sequence of light increments and decrements (from light to neutral to dark and back).  The H1 neuron in Calliphora and VS1-5 in Drosophila are both observed.  While an idealized analysis of the data would suggest that a 4Q detector is needed, that assumes that the detectors have no information about overall brightness.  In contrast, real-world neurons have some memory and some awareness of overall brightness.&lt;br /&gt;
&lt;br /&gt;
As a result, a real-world 2Q detector is modelled as an array of such detectors together covering a single period of a moving sine wave grating.  6 parameters are used to tune this model:  the time constant of the high-pass and low-pass filters, the DC fraction, the clip point for OFF rectification, and the synaptic imbalance, as well as a weighting of the output of the two half-detectors to mimic excitator and inhibitory synaptic transmission.&lt;br /&gt;
&lt;br /&gt;
Cells are assigned a primary and null direction (PD and ND), and a 'PD-ND inversion' effect is noted in which there is a differential response based on whether a PD or ND stimulus is encountered first.   This inversion is considered characteristic of real cells, and looked for in a succesful model.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The single-unit model developed is similar to a traditional Reichardt detector in many scenarios.  In many it parallels the response of a Reichardt detector.  It also responds to all four pairs of ON/OFF input combinations.  There also remain significant differences between the modelled behavior and observed behavior.  This is explained by the authors in part because firing rates 'can only decrease to 0 Hz'.&lt;br /&gt;
&lt;br /&gt;
The large-scale 200-unit array of such detectors is tested against a number of inputs.  It generally agrees with the expected output of a Reichardt detector.  When shown a standing grating before motion begins, it shows oscillations, but when shown a moving sine grating with pseudorandom velocity profile it shows similar behavior to a Reichardt detector.&lt;br /&gt;
&lt;br /&gt;
Overall the authors note a number of arguments for excluding the 2Q model, but have explanations for why each one can be neglected.  They identify a few observations that argue for excluding the 4Q model, and highlight those as conclusive.   Future research is needed into the presynaptic mechanism before signals get to the lobula plate, and the precise nature of the nonlinearity that takes place in the multiplication unit of the Reichardt detector (or similar model).  Some specific ideas are suggested for future exploration.&lt;br /&gt;
|relevance=This added to the literature trying to assess the complexity of the motion-detection mechanism of the fly.  It adds weight to the claim that a fly distinguishes two, rather than all four, pairwise interactions between sequences of responses to bright and dark edges.  It suggests a 2Q model with 6 parameters that can fit some past data; however this remains a question of interpretation and does not settle the question conclusively.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2011/06/23&lt;br /&gt;
|doi=10.1016/j.neuron.2011.03.028&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Internal_Structure_of_the_Fly_Elementary_Motion_Detector&amp;diff=8915</id>
		<title>Internal Structure of the Fly Elementary Motion Detector</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Internal_Structure_of_the_Fly_Elementary_Motion_Detector&amp;diff=8915"/>
		<updated>2012-12-15T23:53:04Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Internal Structure of the Fly Elementary Motion Detector&lt;br /&gt;
|authors=Hubert Eichner, Maximilian Joesch, Bettina Schnell, Dierk F. Reiff, Alexander Borst&lt;br /&gt;
|url=http://www.sciencedirect.com/science/article/pii/S089662731100376X&lt;br /&gt;
|tags=Reichardt detector Drosophila vision motion&lt;br /&gt;
|summary=Building on recent experiments showing that Drosophila motion detection splits the visual input into two parallel (L1 and L2) channels, this study further assumes that those two channels encode increases and decreases in brightness (ON and OFF).  It then maps computations of directional selection to the implementation of an ON/OFF based Reichardt detector.&lt;br /&gt;
&lt;br /&gt;
Under these assumptions, direction-selection is found that matches same-sign but not opposite-sign sequences, suggesting a two-quadrant (2Q) variation of the Reichardt detector.  A model is proposed that both matches current observations and tries to account for past data that was interpreted as supporting four separate components to a (4Q) detector.  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
There are biological and philosophical reasons to imagine that a 2Q detector might be preferably to a 4Q detector: it takes half the energy and biological material, and is known to account for some of the same basic edge detection.  The question is whether it accounts for the full range of motion detection afforded by a 4Q Reichardt detector, and whether it matches observable responses of real flies. &lt;br /&gt;
&lt;br /&gt;
Apparent motion stimuli are used for these experiments, consisting of a sequence of light increments and decrements (from light to neutral to dark and back).  The H1 neuron in Calliphora and VS1-5 in Drosophila are both observed.  While an idealized analysis of the data would suggest that a 4Q detector is needed, that assumes that the detectors have no information about overall brightness.  In contrast, real-world neurons have some memory and some awareness of overall brightness.&lt;br /&gt;
&lt;br /&gt;
As a result, a real-world 2Q detector is modelled as an array of such detectors together covering a single period of a moving sine wave grating.  6 parameters are used to tune this model:  the time constant of the high-pass and low-pass filters, the DC fraction, the clip point for OFF rectification, and the synaptic imbalance, as well as a weighting of the output of the two half-detectors to mimic excitator and inhibitory synaptic transmission.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The single-unit model developed is similar to a traditional Reichardt detector in many scenarios.  In many it parallels the response of a Reichardt detector.  It also responds to all four pairs of ON/OFF input combinations.  There also remain significant differences between the modelled behavior and observed behavior.  This is explained by the authors in part because firing rates 'can only decrease to 0 Hz'.&lt;br /&gt;
&lt;br /&gt;
The large-scale 200-unit array of such detectors is tested against a number of inputs.  It generally agrees with the expected output of a Reichardt detector.  When shown a standing grating before motion begins, it shows oscillations, but when shown a moving sine grating with pseudorandom velocity profile it shows similar behavior to a Reichardt detector.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
|relevance=This added to the literature trying to assess the complexity of the motion-detection mechanism of the fly.  It adds weight to the claim that a fly distinguishes two, rather than all four, pairwise interactions between sequences of responses to bright and dark edges.  It suggests a 2Q model with 6 parameters that can fit some past data; however this remains a question of interpretation and does not settle the question conclusively.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2011/06/23&lt;br /&gt;
|doi=10.1016/j.neuron.2011.03.028&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Segregation_of_object_and_background_motion_in_the_retina&amp;diff=8914</id>
		<title>Segregation of object and background motion in the retina</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Segregation_of_object_and_background_motion_in_the_retina&amp;diff=8914"/>
		<updated>2012-12-15T23:24:21Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Segregation of object and background motion in the retina&lt;br /&gt;
|authors=Bence P. Ölveczky, Stephen A. Baccus, Markus Meister&lt;br /&gt;
|url=http://www.oeb.harvard.edu/faculty/olveczky/docs/Nature.pdf&lt;br /&gt;
|tags=vision, retina, background, object discrimination&lt;br /&gt;
|summary=This study tries to determine where the process of distinguishing local motion within a scene begins en route to the brain.   This is complicated by the fact that the eye is generally in constant motion across a scene.  This distinction is  an essential part of detecting moving objects.  Responses of different cells in the retina are studied for receptivity to this motion, and a model of retinal circuitry is proposed that explains observed effects through nonlinear pooling over interneurons.&lt;br /&gt;
&lt;br /&gt;
This sort of motion detection is suppressed by global image motion - it depends on separating object from background motion.   A mechanism for this is proposed, and a plausible fast-responding biological process described.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
During fixation of the eye on an object, the retina still drifts over half a degree of retinal angle, at a speed of around 0.5 degrees/s.  Any visual  processing happens in the background of this drift.  Other animals show similar drift, including salamanders and rabbits (used in this experiment).  This motion has not received much attention even though a) it seems to make detecting object motion within a scene computationally hard and b) it feels effortless to humans.  This study aims to find an easy way for the eye to segregate object from image motion within the retina, before the images from both eyes merge.  &lt;br /&gt;
&lt;br /&gt;
The authors study the spike trains of ganglion cells in isolated retinas of salamanders and rabbits.  In both cases, scanning the whole retina while showing various images identified a number of ganglions that were highly selective for object motion within a scene and not at all for overall scene motion.  &lt;br /&gt;
The authors refer to these cells as object motion sensitive (OMS) cells, though they include several functional cell types.  In salamanders, these are classified as ON, Weak OFF, and Fast OFF cells; in rabbits they are classified as ON-OFF Direction Selective, ON Brisk Transient, OFF Brisk Transient, and Local Edge Detectors.    &lt;br /&gt;
&lt;br /&gt;
Visual images are projected from a computer monitor onto the photoreceptor layer, at a mean intensity of 8mW/m.  The spatiotemporal receptive fields of the retinas are mapped through reverse correlation to a flickering black-and-white checkerboard.&lt;br /&gt;
&lt;br /&gt;
By studying these cells in more detail, mechanisms for suppression of coherent motion detection are considered and evaluated, along with models for selectivity for object motion.  Underlying neural circuits are suggested to account for this selectivity, for both single and multiple images.  &lt;br /&gt;
&lt;br /&gt;
Analogies are drawn between the species studied and others known to have similar cells in their retinas.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The retina is clearly observed to sense differential motion via OMS cells, including up to 20% of the retinal cells.  They are excited by motion near the center of the field.  &lt;br /&gt;
&lt;br /&gt;
While neurons can be suppressed by peripheral motion, this is found to arrive in brief pulses of 100ms or less, when from a similar local feature as would trigger OMS sensing in the center field.  This does not account for the general inhibition of background motion.  By looking specifically for interneurons that might mediate this suppression, a large amacrine cell is found that responds to coherent jitter with sharp depolarization aligning with the excitation of OMS cells.&lt;br /&gt;
&lt;br /&gt;
By comparing the amacrine cell membrane potential to the time of a ganglion cell spike, an estimate of the precise function of inhibition was made.  These cells are polyaxona, with the size and reach to carry out this role&lt;br /&gt;
&lt;br /&gt;
Selectivity to object motion is independent of the pattern that is moving, and to the speed of jitter.   And the OMS cells seem to respond to very fine elements of a scene, suggesting they may work via nonlinear pooling of the rectified response of many different subunits, similar to Y-ganglia in cats.&lt;br /&gt;
&lt;br /&gt;
The similar distribution of magnocellular ganglia in primate retinas, known to have nonlinear spatial summation as well, suggests they may have similar OMS properties.  &lt;br /&gt;
&lt;br /&gt;
Finally, this mechanism would explain well-known motion illusions such as the Ouchi illusion, which occurs predominantly with images that have horizontal edges in the center field and vertical edges in the periphery, or vice-versa: since these perceptions are processed separately.  &lt;br /&gt;
|relevance=This analysis suggests that many species have cells that are specially sensitive to object motion, related to those known to carry out nonlinear spatial summation.  It presents an analysis that could be carried out in a variety of other settings to probe motion tracking and object-background distinction.&lt;br /&gt;
&lt;br /&gt;
It also identifies a class of illusion that this visual system explains. &lt;br /&gt;
|journal=Nature&lt;br /&gt;
|pub_date=2003/05/22&lt;br /&gt;
|doi=10.1038/nature01652&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8913</id>
		<title>Defining the Computational Structure of the Motion Detector in Drosophila</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8913"/>
		<updated>2012-12-15T22:54:19Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Deﬁning the Computational Structure of the Motion Detector in Drosophila&lt;br /&gt;
|authors=Damon A. Clark, Limor Bursztyn, Mark A. Horowitz, Mark J. Schnitzer, Thomas R. Clandinin&lt;br /&gt;
|url=http://www.cell.com/neuron/retrieve/pii/S0896627311004417&lt;br /&gt;
|tags=Drosophila, Reichardt detector, vision, motion&lt;br /&gt;
|summary=This paper tests the hypothesis that information about motion is extracted from shifting intensity patterns  on the back of the retina.  It shows that a Reichardt-detector model can closely match the neuronal response to visual inputs, and identifies two specific pathways that may carry out pieces of the related computation.  &lt;br /&gt;
&lt;br /&gt;
These two pathways (via laminar cells L1 and L2) are shown to respond differently to light vs. dark moving edges, and it is shown they both carry out part of the idealized computation described by a Reichardt detector.  A theoretical model is proposed that would be tuneable to match observed responses closely (possibly changing over time).  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
These experiments probe the structure and possible component parts of the part of motion detection in Drosophila that responds to moving edges like a Reichardt detector.  While no specific physical components have been identified as carrying out the individual steps of the Reichardt detector algorithm, this work tests the hypothesis that two pathways map to specific subsets of the overall Reichardt computation. &lt;br /&gt;
&lt;br /&gt;
Directional selectivity of flies is observed in response to light and dark edges in intensity patterns, the traditional input used to characterize Reichardt detection.  Responses to &amp;quot;phi&amp;quot; and &amp;quot;reverse phi&amp;quot; stimuli are also observed: changes in contrast in the same direction or in opposite direction.  Reverse phi is related to an illusion: it causes the observer to turn in the opposite direction that the spatial sequence of contrast change would -- into rather than away from an edge.  As it is also observed in animals other than flies, this suggests some overlap in analysis for future study.&lt;br /&gt;
&lt;br /&gt;
In this experiment the flies studied are conscious and held in place suspended just above a ball, which floats at low friction in an airstream.  The fly can move its legs to 'walk' along the ball, and the rotation of the ball captures its motion.  While in this setup, the flies are shown three screens, ahead and to the left and right; shown the image of a rotationg virtual cylinder with periodic patterns. &lt;br /&gt;
&lt;br /&gt;
First the response of wild-type Drosophila's Reichart correlation is characterized, by showing them two bars side by side, with a randomized range of contrast changes and time delays between successive images.  They are also shown rotating cylinders with a fixed periodic square wave.&lt;br /&gt;
Genetically modified Drosophila missing either the L1 or L2 pathway are then bred and tested with the same system.   &lt;br /&gt;
&lt;br /&gt;
Various tests of the L1 and L2 terminals are carried out to see whether each of them responded to both light and dark stimuli in isolation, and to both increases and decreases in intensity.  The response of flies to both phi and reverse phi stimuli are noted and compared to motion sensing in other species. &lt;br /&gt;
&lt;br /&gt;
To understand the role and function of edge selectivity in the L1 and L2 pathways, flies with only one or the other are shown a variety of inputs to find differential responses: including light-light, dark-dark, and phi and revers-phi stimuli.  &lt;br /&gt;
&lt;br /&gt;
It is a point of contemporary debate whether all four possible unit computations of the Reichardt detector are carried out: dark-dark, dark-light, light-dark, light-light.  Drosophila are shown not only the four combinations of dark and light bars, but also phi and reverse-phi stimuli.  Reverse phi stimuli are predicted to produce the opposite response of phi stimuli if all four computations are possible. &lt;br /&gt;
&lt;br /&gt;
A numerical model is developed to match observed edge preferences and responses, with parameters weighting the individual computations of the Reichardt detector to fit observations.&lt;br /&gt;
&lt;br /&gt;
Finally, the implications of two distinct pathways within each Reichardt detector process, for fly motion detection and for understanding other observations of fly neuron responses, are analyzed.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The fly response to randomly generated bars roughly matches that of an ideal Reichardt correlator.&lt;br /&gt;
&lt;br /&gt;
Losing L1 reduces response to only the light edges; losing L2 reduces response to only dark edges.  To distinguish edge detection from overall changes in light level, an equiluminant stimulus is developed where light and dark edges move in opposite directions at equal speeds, at once.  Control flies move only slightly; those without L1 turn towards the dark edge, those without L2 turned towards the light.  &lt;br /&gt;
&lt;br /&gt;
This strongly suggests that L1 and L2 pathways are tied to the ability to detect motion of light and dark edges, respectively.  However both L1 and L2 are found to respond similarly to light and dark flashes, and to respond to the motion of both light and dark edges.   They also respond highly linearly to changes in contrast - either increases or decreases.  In contrast to contemporary work that suggested L2 terminals respond to decreases and not increases in brightness, this is shown to be linear quite uniformly across the spectrum of stimulus intensity.&lt;br /&gt;
&lt;br /&gt;
As reverse phi stimuli produce the response predicted by a full Reichardt detector, the authors concluded that all four unit compoutations are carried out.  This did not entirely settle the question for other researchers however.  Reverse phi stimuli had another interesting property: they produced different complementary responses in flies missing L1 or L2 pathways. &lt;br /&gt;
&lt;br /&gt;
To understand this better, a numerical model is designed for an array of Reichardt detectors, with responses to phi and reverse-phi inputs tuned by weighting the four different unit multiplications in the detector.  Weighting phi stimuli equally while weighting reverse-stimuli differentially is enough to reproduce the edge-selction seen in L1 and L2 pathways.  &lt;br /&gt;
&lt;br /&gt;
As reverse phi responses are observed in many species other than Drosophila, the analysis and model presented at the end of this study are of potential interest to studies of edge and motion detection in other creatures.&lt;br /&gt;
&lt;br /&gt;
; Notes for future and contemporary researchers&lt;br /&gt;
The idea of half-wave rectification of the signal at each input has often been proposed since it is not known how sign-correct multiplication of inputs could be implemented.  Rectification may happen elsewhere in the neural circuit, however.  These experiments demonstrate that the L1 and L2 cells do not themselves carry out such rectification.   &lt;br /&gt;
&lt;br /&gt;
The authors tackle the ongoing debate between &amp;quot;two-computation&amp;quot; and &amp;quot;four-computation&amp;quot; models of a Reichardt detector, which are related to ideas about whether the fly visual system is organized into ON and OFF pathways or simply detecting light v. dark edges.  They conclude from their work that the fly visual system is not organized into ON / OFF pathways -- that is, that L1  transmits information about more than just increases in contrast, and L2 transmits information about more than just decreases.  This is in contrast to Joesch and Eichner. &lt;br /&gt;
&lt;br /&gt;
A few time dependencies are noted related to the laminar cells, as pointers to future study.  The flies studied remember the last image they had seen for at least 1 second for the purposes of future reactions.  L1 and L2 terminals show different kinetics in respond to prolonged stimuli.  And previous work suggests that electrical changes in the cell membrane potential would last for 50-100ms, in contrast to the Ca responses in axonal terminals that last for seconds.  This could indicate adaptation of the synapse, or processing within the axon.  &lt;br /&gt;
&lt;br /&gt;
Reverse phi is proposed as more than an illusion - but as a specific sort of motion captured by neurons, with functional use.  In humans for instance, reverse phi shares properties with motion aftereffects, and may contribute to perception of moving edges of a specific polarity.  Edge-detecting cells are a fundamental unit of visual computation, and this work suggests edge-polarity detection is as well.  &lt;br /&gt;
&lt;br /&gt;
Finally, as demonstrated most concisely in the numerical model presented, edge selectivity can be characterized by selective weighting of L1 and L2 pathways.  Furthermore, this study may only have captured a subset of the actual computations carried out.  Other cells may be involved as well - L4 cells may have a significant role to play.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* See [[Internal Structure of the Fly Elementary Motion Detector]], Eichner, Joesch, Schnell, Reiff, and Borst. Neuron, 2011 (published in the same issue, back to back).  An earlier related work by Joesh is referenced in this paper.&lt;br /&gt;
* [[Phi movement as a subtraction process]]. S.M. Anstis, Vision. (1970)&lt;br /&gt;
&lt;br /&gt;
|relevance=Changes in light and shadow over time and space are shown to be detected by a system that closely parallels a simple Reichardt detector  (or Hassenstein-Reichardt correlator).  A model for such a detector is proposed that can be tuned to detect moving edges of contrast.  &lt;br /&gt;
 &lt;br /&gt;
This clearly distinguished two different neuronal pathways (L1 and L2) as responsible for different parts of  vision,  by selectively disabling each one separately and quantifying the different changes in edge detection.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2011&lt;br /&gt;
|doi=10.1016/j.neuron.2011.05.023&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8912</id>
		<title>Defining the Computational Structure of the Motion Detector in Drosophila</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8912"/>
		<updated>2012-12-15T22:51:49Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Deﬁning the Computational Structure of the Motion Detector in Drosophila&lt;br /&gt;
|authors=Damon A. Clark, Limor Bursztyn, Mark A. Horowitz, Mark J. Schnitzer, Thomas R. Clandinin&lt;br /&gt;
|url=http://www.cell.com/neuron/retrieve/pii/S0896627311004417&lt;br /&gt;
|tags=Drosophila, Reichardt detector, vision, motion&lt;br /&gt;
|summary=This paper tests the hypothesis that information about motion is extracted from shifting intensity patterns  on the back of the retina.  It shows that a Reichardt-detector model can closely match the neuronal response to visual inputs, and identifies two specific pathways that may carry out pieces of the related computation.  &lt;br /&gt;
&lt;br /&gt;
These two pathways (via laminar cells L1 and L2) are shown to respond differently to light vs. dark moving edges, and it is shown they both carry out part of the idealized computation described by a Reichardt detector.  A theoretical model is proposed that would be tuneable to match observed responses closely (possibly changing over time).  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
These experiments probe the structure and possible component parts of the part of motion detection in Drosophila that responds to moving edges like a Reichardt detector.  While no specific physical components have been identified as carrying out the individual steps of the Reichardt detector algorithm, this work tests the hypothesis that two pathways map to specific subsets of the overall Reichardt computation. &lt;br /&gt;
&lt;br /&gt;
Directional selectivity of flies is observed in response to light and dark edges in intensity patterns, the traditional input used to characterize Reichardt detection.  Responses to &amp;quot;phi&amp;quot; and &amp;quot;reverse phi&amp;quot; stimuli are also observed: changes in contrast in the same direction or in opposite direction.  Reverse phi is related to an illusion: it causes the observer to turn in the opposite direction that the spatial sequence of contrast change would -- into rather than away from an edge.  As it is also observed in animals other than flies, this suggests some overlap in analysis for future study.&lt;br /&gt;
&lt;br /&gt;
In this experiment the flies studied are conscious and held in place suspended just above a ball, which floats at low friction in an airstream.  The fly can move its legs to 'walk' along the ball, and the rotation of the ball captures its motion.  While in this setup, the flies are shown three screens, ahead and to the left and right; shown the image of a rotationg virtual cylinder with periodic patterns. &lt;br /&gt;
&lt;br /&gt;
First the response of wild-type Drosophila's Reichart correlation is characterized, by showing them two bars side by side, with a randomized range of contrast changes and time delays between successive images.  They are also shown rotating cylinders with a fixed periodic square wave.&lt;br /&gt;
Genetically modified Drosophila missing either the L1 or L2 pathway are then bred and tested with the same system.   &lt;br /&gt;
&lt;br /&gt;
Various tests of the L1 and L2 terminals are carried out to see whether each of them responded to both light and dark stimuli in isolation, and to both increases and decreases in intensity.  The response of flies to both phi and reverse phi stimuli are noted and compared to motion sensing in other species. &lt;br /&gt;
&lt;br /&gt;
To understand the role and function of edge selectivity in the L1 and L2 pathways, flies with only one or the other are shown a variety of inputs to find differential responses: including light-light, dark-dark, and phi and revers-phi stimuli.  &lt;br /&gt;
&lt;br /&gt;
It is a point of contemporary debate whether all four possible unit computations of the Reichardt detector are carried out: dark-dark, dark-light, light-dark, light-light.  Drosophila are shown not only the four combinations of dark and light bars, but also phi and reverse-phi stimuli.  Reverse phi stimuli are predicted to produce the opposite response of phi stimuli if all four computations are possible. &lt;br /&gt;
&lt;br /&gt;
A numerical model is developed to match observed edge preferences and responses, with parameters weighting the individual computations of the Reichardt detector to fit observations.&lt;br /&gt;
&lt;br /&gt;
Finally, the implications of two distinct pathways within each Reichardt detector process, for fly motion detection and for understanding other observations of fly neuron responses, are analyzed.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The fly response to randomly generated bars roughly matches that of an ideal Reichardt correlator.&lt;br /&gt;
&lt;br /&gt;
Losing L1 reduces response to only the light edges; losing L2 reduces response to only dark edges.  To distinguish edge detection from overall changes in light level, an equiluminant stimulus is developed where light and dark edges move in opposite directions at equal speeds, at once.  Control flies move only slightly; those without L1 turn towards the dark edge, those without L2 turned towards the light.  &lt;br /&gt;
&lt;br /&gt;
This strongly suggests that L1 and L2 pathways are tied to the ability to detect motion of light and dark edges, respectively.  However both L1 and L2 are found to respond similarly to light and dark flashes, and to respond to the motion of both light and dark edges.   They also respond highly linearly to changes in contrast - either increases or decreases.  In contrast to contemporary work that suggested L2 terminals respond to decreases and not increases in brightness, this is shown to be linear quite uniformly across the spectrum of stimulus intensity.&lt;br /&gt;
&lt;br /&gt;
As reverse phi stimuli produce the response predicted by a full Reichardt detector, the authors concluded that all four unit compoutations are carried out.  This did not entirely settle the question for other researchers however.  Reverse phi stimuli had another interesting property: they produced different complementary responses in flies missing L1 or L2 pathways. &lt;br /&gt;
&lt;br /&gt;
To understand this better, a numerical model is designed for an array of Reichardt detectors, with responses to phi and reverse-phi inputs tuned by weighting the four different unit multiplications in the detector.  Weighting phi stimuli equally while weighting reverse-stimuli differentially is enough to reproduce the edge-selction seen in L1 and L2 pathways.  &lt;br /&gt;
&lt;br /&gt;
As reverse phi responses are observed in many species other than Drosophila, the analysis and model presented at the end of this study are of potential interest to studies of edge and motion detection in other creatures.&lt;br /&gt;
&lt;br /&gt;
; Notes for future and contemporary researchers&lt;br /&gt;
The idea of half-wave rectification of the signal at each input has often been proposed since it is not known how sign-correct multiplication of inputs could be implemented.  Rectification may happen elsewhere in the neural circuit, however.  These experiments demonstrate that the L1 and L2 cells do not themselves carry out such rectification.   &lt;br /&gt;
&lt;br /&gt;
The authors tackle the ongoing debate between &amp;quot;two-computation&amp;quot; and &amp;quot;four-computation&amp;quot; models of a Reichardt detector, which are related to ideas about whether the fly visual system is organized into ON and OFF pathways or simply detecting light v. dark edges.  They conclude from their work that the fly visual system is not organized into ON / OFF pathways -- that is, that L1  transmits information about more than just increases in contrast, and L2 transmits information about more than just decreases.  This is in contrast to Joesch and Eichner.&amp;lt;ref&amp;gt;see [[Internal Structure of the Fly Elementary Motion Detector]], published in the same issue of Neuron, 2011.&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
A few time dependencies are noted related to the laminar cells, as pointers to future study.  The flies studied remember the last image they had seen for at least 1 second for the purposes of future reactions.  L1 and L2 terminals show different kinetics in respond to prolonged stimuli.  And previous work suggests that electrical changes in the cell membrane potential would last for 50-100ms, in contrast to the Ca responses in axonal terminals that last for seconds.  This could indicate adaptation of the synapse, or processing within the axon.  &lt;br /&gt;
&lt;br /&gt;
Reverse phi is proposed as more than an illusion - but as a specific sort of motion captured by neurons, with functional use.  In humans for instance, reverse phi shares properties with motion aftereffects, and may contribute to perception of moving edges of a specific polarity.  Edge-detecting cells are a fundamental unit of visual computation, and this work suggests edge-polarity detection is as well.  &lt;br /&gt;
&lt;br /&gt;
Finally, as demonstrated most concisely in the numerical model presented, edge selectivity can be characterized by selective weighting of L1 and L2 pathways.  Furthermore, this study may only have captured a subset of the actual computations carried out.  Other cells may be involved as well - L4 cells may have a significant role to play.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
|relevance=&lt;br /&gt;
Changes in light and shadow over time and space are shown to be detected by a system that closely parallels a simple Reichardt detector  (or Hassenstein-Reichardt correlator).  A model for such a detector is proposed that can be tuned to detect moving edges of contrast.  &lt;br /&gt;
 &lt;br /&gt;
This clearly distinguished two different neuronal pathways (L1 and L2) as responsible for different parts of  vision,  by selectively disabling each one separately and quantifying the different changes in edge detection.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2011&lt;br /&gt;
|doi=10.1016/j.neuron.2011.05.023&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8911</id>
		<title>Defining the Computational Structure of the Motion Detector in Drosophila</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Defining_the_Computational_Structure_of_the_Motion_Detector_in_Drosophila&amp;diff=8911"/>
		<updated>2012-12-15T22:08:42Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Deﬁning the Computational Structure of the Motion Detector in Drosophila&lt;br /&gt;
|authors=Damon A. Clark, Limor Bursztyn, Mark A. Horowitz, Mark J. Schnitzer, Thomas R. Clandinin&lt;br /&gt;
|url=http://www.cell.com/neuron/retrieve/pii/S0896627311004417&lt;br /&gt;
|summary=This paper tests the hypothesis that information about motion is extracted from shifting intensity patterns  on the back of the retina.  It shows that a Reichardt-detector model can closely match the neuronal response to visual inputs, and identifies two specific pathways that may carry out pieces of the related computation.  &lt;br /&gt;
&lt;br /&gt;
These two pathways (via laminar cells L1 and L2) are shown to respond differently to light vs. dark moving edges, and it is shown they both carry out part of the idealized computation described by a Reichardt detector.  A theoretical model is proposed that would be tuneable to match observed responses closely (possibly changing over time).  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
These experiments probe the structure and possible component parts of the part of motion detection in Drosophila that responds to moving edges like a Reichardt detector.  While no specific physical components have been identified as carrying out the individual steps of the Reichardt detector algorithm, this work tests the hypothesis that two pathways map to specific subsets of the overall Reichardt computation. &lt;br /&gt;
&lt;br /&gt;
Directional selectivity of flies is observed in response to light and dark edges in intensity patterns, the traditional input used to characterize Reichardt detection.  Responses to &amp;quot;phi&amp;quot; and &amp;quot;reverse phi&amp;quot; stimuli are also observed: changes in contrast in the same direction or in opposite direction.  Reverse phi is related to an illusion: it causes the observer to turn in the opposite direction that the spatial sequence of contrast change would -- into rather than away from an edge.  As it is also observed in animals other than flies, this suggests some overlap in analysis for future study.&lt;br /&gt;
&lt;br /&gt;
In this experiment the flies studied were conscious and held in place suspended just above a ball, which floats at low friction in an airstream.  The fly can move its legs to 'walk' along the ball, and the rotation of the ball captures its motion.  While in this setup, the flies are shown three screens, ahead and to the left and right; shown the image of a rotationg virtual cylinder with periodic patterns. &lt;br /&gt;
&lt;br /&gt;
First the response of wild-type Drosophila's Reichard correlation was characterized, by showing them two bars side by side, with a randomized range of contrast changes and time delays between successive images.  They were also shown rotating cylinders with a fixed periodic square wave.&lt;br /&gt;
Genetically modified Drosophila missing either the L1 or L2 pathway were then bred and tested with the same system.   &lt;br /&gt;
&lt;br /&gt;
A numerical model is developed that matches observed edge preferences and responses.&lt;br /&gt;
&lt;br /&gt;
The implications for sensitivity of the model and observed cells to the &amp;quot;reverse phi&amp;quot; illusion is noted and compared to motion sensing in other species. &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The fly response to randomly generated bars roughly matched that of an ideal Reichardt correlator.&lt;br /&gt;
&lt;br /&gt;
Losing L1 reduced response to only the light edges; losing L2 reduced response to only dark edges.  To distinguish edge detection from overall changes in light level, an equiluminant stimulus was developed where light and dark edges moved in opposite directions at equal speeds, at once.  Control flies moved only slightly; those without L1 turned towards the dark edge, those without L2 turned towards the light.  &lt;br /&gt;
&lt;br /&gt;
This strongly suggested that L1 and L2 pathways were tied to the ability to detect motion of light and dark edges, respectively.  However both L1 and L2 were found to respond similarly to light and dark flashes, and to respond to the motion of both light and dark edges. &lt;br /&gt;
&lt;br /&gt;
The observed response and model are also noted for its sensitivity to &amp;quot;reverse phi&amp;quot; stimulus, an illusion that is responded to by many species other than Drosophila.  The analysis and model presented in this paper are therefore of potential interest to studies of edge detection in other creatures.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
|relevance=Changes in light and shadow over time and space were shown to be detected by a system that closely parallels a simple Reichardt detector  (or Hassenstein-Reichardt correlator).  A model for such a detector is proposed that can be tuned to detect moving edges of contrast.  &lt;br /&gt;
 &lt;br /&gt;
This clearly distinguished two different neuronal pathways (L1 and L2) as responsible for different parts of  vision,  by selectively disabling each one separately and quantifying the different changes in edge detection.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2011&lt;br /&gt;
|doi=10.1016/j.neuron.2011.05.023&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Selective_Transmission_of_Single_Photon_Responses_by_Saturation_at_the_Rod-to-Rod_Bipolar_Synapse&amp;diff=8910</id>
		<title>Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Selective_Transmission_of_Single_Photon_Responses_by_Saturation_at_the_Rod-to-Rod_Bipolar_Synapse&amp;diff=8910"/>
		<updated>2012-12-15T21:40:32Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse&lt;br /&gt;
|authors=Alapakkam P. Sampath, Fred Rieke&lt;br /&gt;
|url=http://www.cns.nyu.edu/csh/csh04/Articles/Sampath2004.pdf&lt;br /&gt;
|tags=single photon response, rods, mouse&lt;br /&gt;
|summary=Rod cells work remarkably well in the dark.  One of the observed facets of this is a threshold-like nonlinear response of the retina to signals from each rod before combining them.  This series of experiments probes the mechanisms of that nonlinearity in mouse rods and comes up with a model that explains it in part in terms of synapse saturation, then explores that model in detail to see how well it matches observations.  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
A few mechanisms for nonlinear response to rod signals had been considered, but not explored in detail.  Evidence for and against saturation at central nervous system synapses has been debated in different contexts, with some contemporary work suggesting some synapses are saturated at a single action potential but not otherwise.  And more than one mechanisms is implicated in saturation.&lt;br /&gt;
&lt;br /&gt;
This experiment aimed to identify whether saturation occured in rod transmission, and if so which mechanisms were involved, and whether this sufficed to account for the overall nonlinear response to rod signals in the mouse retina.   Some reasons to focus on the rod-to-rod bipolar synapse include: &lt;br /&gt;
* Rods are known to continuously release transmitter in the dark, slwoing down when hyperpolarized by light.&lt;br /&gt;
* Receptor activity leads to closing nonselective cation channels through some sort of signal cascade, which could provide another source of saturation.&lt;br /&gt;
* The ribbon-type synapses between rods and rod biploars involve small graded changes in voltage.&lt;br /&gt;
&lt;br /&gt;
The light response of mouse rod bipolars was known to have a supralinear dependence on the strength of a flash, coming from the transfer of signal from rod to rod bipolar cell.  This was investigated to see whether it was an intrinsic feature of the synapse or due to feedback from horizontal or amacrine cells.  &lt;br /&gt;
&lt;br /&gt;
Both voltage-clamped and perforated-patch methods were used to study and record signals from rod bipolar cells.  The nonlinearity of the cell's response was estimated by the Hill exponent of the best fit to the flash strangth-response relation.&lt;br /&gt;
&lt;br /&gt;
In one experiment, they were observed while subject to a range of flash intensities, both with and without suppressing the activity of nearby amacrine and horizontal cells. &lt;br /&gt;
&lt;br /&gt;
In the dark, the rod bipolar transduction cascade was found to operate near saturation.   But what was being saturated?  Various tests for saturation were carried out : adding G protein; reducing the number of available receptors or stimulating them. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
Most of the nonlinearity was accounted for by the effects of saturating the rod-to-rod bipolar synapse, rather than competing theories about feedback from nearby horizontal or amacrine cells. &lt;br /&gt;
&lt;br /&gt;
Saturation was found to make the rod current insensitive to small changes in transmitter concentration around the rod.  But what was saturated in the dark? &lt;br /&gt;
&lt;br /&gt;
* Adding G protein had little effect on the cascadee.  It was more sensitive to decreases in G protein activity (as is produced by light).  &lt;br /&gt;
* Increasing receptor activity with APC increased its nonlinearity.   Decreasing receptor activity with LY341495 decreased its nonlinearity.   Since thse both unbind slowly, their influence on the response suggests the receptors themselves are not strongly saturated; this happens downstream. &lt;br /&gt;
* Few transduction channels (&amp;lt;2 per rod) were found to be open, as estimated by single channel current and dark current fluctuations. &lt;br /&gt;
&lt;br /&gt;
This saturation is in the G protein cascade that couples receptors to channels in rod bipolar dendrites, with little or no saturation of presynaptic or postsynaptic receptors.  In the dark, 2 or fewer bipolar transduction channels are observed to be open at each synapse, compared to 30 at the peak of a single-photon response.&lt;br /&gt;
&lt;br /&gt;
Two specific models are proposed, one produced by saturation directly at the transduction channels; the other produced in another component of the transduction cascade.  Both could happen, but the results suggest they account for most of the nonlinearity.  &lt;br /&gt;
&lt;br /&gt;
Rods are known to be specialized for detecting single photons; this analysis highlights that the specialization may extend to specialized transfer of signals to rod bipolar cells.&lt;br /&gt;
&lt;br /&gt;
== Key references ==&lt;br /&gt;
* [[Responses of retinal rods to single photons]].  D.A. Baylor, T.D. Lamb, K.-W. Yau, Journal of Physiology (1979)&lt;br /&gt;
* [[Nonlinear signal transfer from mouse rods to bipolar cells and implications for visual sensitivity]].&lt;br /&gt;
G.D. Field, F. Rieke, Neuron 34 (2002)&lt;br /&gt;
|relevance=This work probed the mechanism of nonlinear responses of mouse rods in darkness, indicating that synapose saturation is the source of nonlinearity and suggesting where to look for the details of the saturation mechanism.  &lt;br /&gt;
&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2004/02/05&lt;br /&gt;
|doi=10.1016/S0896-6273(04)00005-4&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8904</id>
		<title>Energy, Quanta, and Vision</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8904"/>
		<updated>2012-12-15T20:35:33Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Energy, Quanta, and Vision&lt;br /&gt;
|authors=Selig Hecht, Simon Shlaer, Maurice Henri Pirenne&lt;br /&gt;
|tags=vision quanta light eye&lt;br /&gt;
|summary= The authors note that there have been many studies of the visual threshold of the human eye, many improving on those before.   This paper includes a survey and history of experiments in the area, notes some inadequacies in past work and opportunity for improvement, and lays out and implements a new technique for measuring visual sensitivity.  Their practical noise-reduction is somewhat better than previous experiments, and they add a widely useful statistical technique that allows for a much stronger signal to be extracted from the intrinsically noisy data of observation.  &lt;br /&gt;
&lt;br /&gt;
The result is both a new and lower upper bound on the visual threshold, and a useful exercise in statistical data analysis.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The question of the fundamental sensitivity of the human eye is a long-standing one, and had been tested sporadically for decades.  This experiment reduced noise in a few ways, and analyzed the results assuming detection and observation of light would follow a Poisson distribution.&lt;br /&gt;
&lt;br /&gt;
;Noise reduction and measurement:&lt;br /&gt;
* Subjects were adapted to the dark for 40 minutes, &lt;br /&gt;
* Light was focused on an area in the retina's peripheral vision (where light response is optimal)&lt;br /&gt;
* Light was flashed at 510nm, a wavelength we are particularly sensitive to&lt;br /&gt;
* Flashes of 1 ms and a spot size smaller than 10 arcminutes were chosen.  A set of diaphragms and filters were used to vary the spot size and brightness without moving the rest of the setup.  The flashes were generated using a circular shutter with a tiny hole cut in it, rotating so quickly that at any give moment it lets light through for 0.001 s of a revolution&lt;br /&gt;
* All light was carefully passed through an equal thickness of glass for uniform illumination, with entrance and exist slits both 1.2mm wide, corresponding to the desired bandwidth of the beam.  &lt;br /&gt;
* A red light was provided to help fixate the eye so it did not jitter.  &lt;br /&gt;
&lt;br /&gt;
Measurements were taken with this apparatus over the course of two years and seven subjects.  Each of a series of intensities was presented many times, with the frequency of seeing a flash determined for each intensity, and calculating the associated number of quanta sent to the eye. &lt;br /&gt;
&lt;br /&gt;
This and the rest of the experiment assume that observer response is intrinsically probabilistic.  The participants in the study were trained to say they had seen a light only if they were sure, to minimize false positives.  A threshold was defined as the intensity which could be seen with a 60% frequency.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
;Light intensity and absorption&lt;br /&gt;
One of the more careful aspects of this paper is its analysis of reflection and absorption of light by the eye, and the estimated portion of light that reaches the retina.  &lt;br /&gt;
&lt;br /&gt;
The details of the filter and the light source were calibrated (more han once, to ensure constancy) so as to estimate the energy density sent to the pupil.  This was varied over the course of the experiment, and used as a gauge of how many quanta of light had potentially been absorbed by the eye.   &lt;br /&gt;
&lt;br /&gt;
Based on the absorption analysis, the number of quanta ''absorbed'' by the eye can be estimated from the total light intensity.  &lt;br /&gt;
&lt;br /&gt;
This suggested a value lower than any found in previous experiments.  So an additional statistical  model is used to cross-check the result, based on the Poisson distribution of light emitted in any one flash.  &lt;br /&gt;
&lt;br /&gt;
The probability of a given flash being observed is then assumed to be the probability that more than a hidden threshhold of quanta are detected by the eye.  In this version of the model it is primarily the signal  that varies -- whenever the signal passes some threshold, it is assumed to be seen.  However it is noted that human variability combines with the signal variability in this case and is not a significant factor in the analysis. &lt;br /&gt;
&lt;br /&gt;
The threshold estimated by this was compared to that estimated by calculating the % of total photons absorbed by the eye.  &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
Contemporary studies were used to estimate that 50% of light is transmitted through the cornea, and an upper limit of 20% of impinging light absorbed by retinal pigments (visual purple).  The latter is estimated anew in this paper based on data from frog retinas and pigment density.   Earlier work by Hecht provided data on scoptopic luminosity at the retina and the optimal frequency for detection.   This would mean a total absorption of 10% of incoming photons.&lt;br /&gt;
&lt;br /&gt;
The total energy density at the cornea is 54-148 quanta of light, which maps to 5-14 quanta absorbed by rods.  This is over a field of ~500 rods, suggesting that no rod absorbs more than one.&lt;br /&gt;
&lt;br /&gt;
For the statistical comparison, it is noted that the absolute threshold for vision seems to be small - 5 to 8 quanta.  And that this statistical estimate is easier to see when the total number of detections is small.  Variation in the biological capacity of the participants doesn't effect this analysis much.  So the agreement between this estimate and the energy-absorption estimate is significant.&lt;br /&gt;
&lt;br /&gt;
This suggests that, while in the past it has been assumed that light stimulus is constant and the observer variable, the primary factor in light detection is the variability of the signal.&lt;br /&gt;
&lt;br /&gt;
Future experiment is needed to determine whether there are differential threshold at some level of intensity, separate from the absolute threshold, for which a small number of events determines the differentiation.  Moreover, this is simply an upper bound, and the bound used to identify the number of photons absorbed by the retina is noted to seem high by a factor of 2.   The paper did not dwell on the training of the observers (most of whom were also co-authors).  However later studies would make a point of training people differently to note uncertainty differently than they note definite non-observation of light - a variation that lowers the threshold further.&lt;br /&gt;
|relevance=This paper has become a canonical reference for any discussion about how sensitive the human eye is to individual quanta of light.  While it was not the first to ask the question and carry out experiments to measure how small a signal was needed to stimulate the eye, it used a simple and universal technique, was careful in its error analysis, and compared its work cleanly with those of past attempts to measure the visual threshold.  Previous estimates of the visual threshhold were on the order of 20 quanta of light; this work used statistical analysis to reduce that to 5-7. &lt;br /&gt;
|journal=The Journal of General Physiology&lt;br /&gt;
|pub_date=1942&lt;br /&gt;
|subject=Biology&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Odor_Representations_in_Olfactory_Cortex:_Distributed_Rate_Coding_and_Decorrelated_Population_Activity&amp;diff=8902</id>
		<title>Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Odor_Representations_in_Olfactory_Cortex:_Distributed_Rate_Coding_and_Decorrelated_Population_Activity&amp;diff=8902"/>
		<updated>2012-12-15T19:49:38Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity&lt;br /&gt;
|authors=Keiji Miura, Zachary F. Mainen, Naoshige Uchida&lt;br /&gt;
|url=http://www.sciencedirect.com/science/article/pii/S0896627312003893&lt;br /&gt;
|tags=olfaction, coding&lt;br /&gt;
|summary=This paper addresses the question of how neuronal spikes in the olfactory cortex guide sensory decisions in the rat.  It starts from the observation that a single sniff generally suffices for precise odor discrimination,  yet the mechanism involved and the sources of noise in behavioral responses are not fully understood.  As the coding of odor information in the olfactory cortex is less well-known than that in the olfactory bulb, the authors measure the output of ensembles of 5-15 neurons in the olfactory cortex of 8 trained rats, and analyze the statistics of their responses to different odors.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
Rodents often engage in active sampling, taking rapid sniffs while exploring.  This suggests that each sniff suffices to give a snapshot of odors.  This experiment aims to understand better what happens to encode sensory information over the timescale of a single sniff, and how it is transformed on the way to the brain to influence behavior. &lt;br /&gt;
&lt;br /&gt;
Neural ensemble activity is measured in the anterior piriform cortex [aPC] of rats performing odor categorization, and principal components of the activity are identified.  These cortex ensembles show very low noise correlation, suggesting that it has a very well-defined reprsentation of odor identity.  An optimal theoretical linear decoder tested against these inputs could discriminate odors as well as mice are observed to, with only 100 neurons.  However the rat aPC has 10,000 times as many; possible implications of this variance are discussed as motivation for further study.&lt;br /&gt;
&lt;br /&gt;
Six odors were tested and an ensemble of neurons in the aPC recorded.  &lt;br /&gt;
Both latency and peak timing of aPC responses were measured, as were spike counts.  &lt;br /&gt;
&lt;br /&gt;
A number of theoretical decoders were used to map the observed latencies and spike counts to odor classification.  &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
Each sniff was seen to trigger a transient spike linked closely to the onset of inhalation.  Odor stimulation stimulated a broad ensemble of neurons, with fairly little directional selectivity.   45% of all neurons were stimulated by one of the odors, but each odor triggered only 16%; so the neurons were fairly selective.&lt;br /&gt;
&lt;br /&gt;
The theoretical decoder that worked significantly better than all others relied on spike counts, and was hardly improved with the addition of the other data.  So this seems to be the most likely candidate of those tested to related to actual encoding odor information.  &lt;br /&gt;
&lt;br /&gt;
Information provided by spike counts could account for the rapid discrimination of odors.&lt;br /&gt;
On the other hand, this decoder worked much more effectively than the rodents in practice, so some other part of the whole system is missing from the model.  Choice probability analysis suggests individual aPC neurons are very weakly correlated if at all.  This was true regardless of the distance between neurons or the similarity of their odor tuning.&lt;br /&gt;
&lt;br /&gt;
Further study is needed to understand a few points:&lt;br /&gt;
* Why might the olfactory bulb and cortex use different odor coding strategies? The codex is much larger and could afford to use a more widely-distributed code, which could also enable memory creation.  &lt;br /&gt;
* How does olfactory information switch from temporal coding to rate coding?&lt;br /&gt;
* What limits behavioral accuracy, which seems to be lower than a good linear decoder might do with only 100 neurons? &lt;br /&gt;
* Can second and further sniffs not significantly improve decoding?  This remains controversial.  Rate information seems to peak 100ms from the onset of the first sniff. But in this experiment little improvement in decoding was observed with multiple sniffs. &lt;br /&gt;
&lt;br /&gt;
|relevance=This paper suggests that odors generate characteristic transient bursts immediately after a sniff, and that the identity of an odor is more closely related to properties of those bursts such as the burst spike count than to spikes over an entire sniff cycle or to their timing.  It also suggests the olfactory bulb and cortex code odors differently, and have a higher theoretical accuracy in odor discrimination than has been observed in rat behavior.&lt;br /&gt;
|journal=Neuron&lt;br /&gt;
|pub_date=2012/06/21&lt;br /&gt;
|doi=10.1016/j.neuron.2012.04.021&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8901</id>
		<title>Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8901"/>
		<updated>2012-12-15T19:25:21Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio&lt;br /&gt;
|authors=J Haag, W Denk, A Borst&lt;br /&gt;
|url=http://adsabs.harvard.edu/abs/2004PNAS..10116333H&lt;br /&gt;
|tags=vision algorithms&lt;br /&gt;
|summary=It has been theorized that fly vision might switch from relying on Reichardt detectors to relying on some other mechanism such as gradient detectors in high signal-to-noise regimes.  This paper summarizes two experiments probing those regimes and testing different parts of the fly vision chain, and finds no evidence for any mechanism other than Reichardt detectors.  &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
Gradient detectors are still considered a competing mechanism to Reichardt detectors in high signal-to-noise regimes.  And in order to work with elementary responses, experiments often work at the opposite end of the signal spectrum, aiming for the smallest signal that elicits a measurable response.  As a result few experiments have been carried out to test whether markers of gradient detection can be observed in fly motion vision under any circumstances.&lt;br /&gt;
&lt;br /&gt;
This paper describes two experiments to evaluate the hypothesis that gradient detectors are not part of the fly motion pathways at all. Both study direction selectivity in flies, the canonical test for fly motion vision.  &lt;br /&gt;
&lt;br /&gt;
One experiment tested for the dependence of optimal stimulus 'velocity' (the actual velocity of the pattern used as a stimulus) on the wavelength of the pattern.  This is expected to be directly correlated in the Reichardt detector case, and relatively uncorrelated in the gradient detector case.  It was simply measured by looking at neuron spikes of the motion-sensitive neuron H1.  This test was repeated over a wide range of mean luminance and of stimulus contrast (roughly 2 magnitudes in each case).&lt;br /&gt;
&lt;br /&gt;
The second more complex experiment improved on a traditional experiment to show Reichardt detection: observing the local modulations in signal along a dendrite as a pattern moves past it.  In the Reichardt case this is expected to move synchronous with the pattern, and to be phase-shifted along different parts of the dendrite.  However this was always previously done with 1-photon imaging, which has a side-effect of false positives that limits how small overall noise could be in such an experiment (and so limits the maximum pattern contrast).   This is addressed here by using 2-photon microscopy with luminescent Calcium markers, a technique that allows very high signal without false-positive noise.  Neurons of both vertical and horizontal systems were observed.&lt;br /&gt;
&lt;br /&gt;
These experiments benefitted from a clear understanding of fly biology, and did not measure conscious motion detection, but neuron-level detection within the lobula plate.  The flies had their heads opened and trachea and air sacs removed so that the lobula plate could be imaged directly from above; those subject to the higher SNR-requirement two-photon microscopy also had their proboscis and gut removed.  Images were taken with a 64x64 pixel camera and transformed from fuorescence changes into projected DC + AC signal. &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
Results at all signal levels matched what would be expected of Reichardt detectors, and while there were some variations in response at different levels of signal intensity, no hallmarks of gradient detection were seen.&lt;br /&gt;
&lt;br /&gt;
This held true up to pattern contrasts of ~90% and luminance of 200cd/m^2, close to broad daylight.  Additionally, the total variation in [Ca2+] at the dendritic fringe increased with increasing contrast, the opposite of what might be expected with a gradient detector.&lt;br /&gt;
&lt;br /&gt;
This demonstrated that Reichardt detectors seem to model the mechanism of direction selectivity in fly neurons of the lobular plate, up to fairly high contrast and illumination levels, close to the maximum that flies are thought to distinguish.  While it cannot rule out the possibility of a mechanism like a gradient detector in use in the visual system, this is a strong indication that gradient detectors are not needed for effective motion detection. &lt;br /&gt;
&lt;br /&gt;
Three outstanding questions are noted as remaining support the idea that something other than Reichardt detectors, perhaps gradient detection, is involved in some regimes.  One is theoretical: a naive analysis suggests that gradient detectors would be the simplest, and perhaps most efficient, detection scheme.  If this is not true in any regime, where does the simple model fail?  And a few experimental results are also unexplained: &lt;br /&gt;
* Reichardt detectors have a quadratic relationship between signal amplitude and stimulus contrast.  But this becomes contrast-independent slightly above 10% contrast, in Drosophila, Musca, and others.   &lt;br /&gt;
* Humans perceive low-contrast gratings to be slower than high-contrast gratings. &lt;br /&gt;
* Srinivasan (1991) notes free-flying honey bees moving through a tunnel can detect actual image velocity, not just pattern wavelength. &lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* [[:File:Reichardt-forever.pdf|Visual summary]] (presentation form, pdf)&lt;br /&gt;
* M. V. Srinivasan, M. Lehrer, W. H. Kirchner, S. W. Zhang (1991) Visual Neuroscience 6. &lt;br /&gt;
|relevance=This is a concise demonstration that a Reichardt-detector process, or something very close to it, continues to be the dominant way gradients and edges are detected in fly vision, even in environments with low noise.  &lt;br /&gt;
&lt;br /&gt;
Historically, gradient detection has been a top contender for a mechanism for vision in low-noise environments, because of their theoretical simplicity and high precision.  This experiment tried two unrelated methods of finding indications of gradient detection in fly vision, removing much more noise from their method and increasing the signal dramatically beyond previous experiments; but without success.&lt;br /&gt;
|journal=PNAS&lt;br /&gt;
|pub_date=2004/11/01&lt;br /&gt;
|doi=10.1073/pnas.0407368101&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Unitary_response_of_mouse_olfactory_receptor_neurons&amp;diff=8900</id>
		<title>Unitary response of mouse olfactory receptor neurons</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Unitary_response_of_mouse_olfactory_receptor_neurons&amp;diff=8900"/>
		<updated>2012-12-15T18:54:18Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Unitary response of mouse olfactory receptor neurons&lt;br /&gt;
|authors=Yair Ben-Chaim a,1 , Melody M. Cheng b , and King-Wai Yau a,1&lt;br /&gt;
|url=http://www.pnas.org/content/108/2/822&lt;br /&gt;
|tags=olfaction mouse&lt;br /&gt;
|summary=This paper studies the response of mouse olfactory receptor neurons [ORNs] to a variety of odorants, and notes that the response is relatively uniform in amplitude and kinetics, unchanging across different neurons and different odors (hence 'elementary' or 'unitary' - responding to the entire experience of a novel smell as a single smelling-event).  The experiment involved followed earlier work by Yau and others on frog ORNs, showing that the same results hold for mice and so possibly for other mammals.  &lt;br /&gt;
&lt;br /&gt;
The olfactory response similar for different clusters of odorants  it had little amplification, triggering transduction through only just single molecular complex.  Successful response required only O(10) successful binding events.  Both traits are similar to the results found for frog ORNs in the earlier work. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The primary goal was to check the similarity between responses of mouse and frog ORNs to address the question of whether the properties of olfactory response in mammals might have similar traits.  Existing methodology was repeated with mouse cells: short bursts of odorants, varying either the concentration in bursts of fixed length or the length of bursts of fixed concentration.  &lt;br /&gt;
&lt;br /&gt;
The method used carried out a quantal analysis on results, assuming there was a minimum unitary response, and a Poisson distribution of individual responses.  The suction-pipette method was used to measure membrane currents.  As there are 1000 species of OR cells, a mixture of five odorants was used instead of two.&lt;br /&gt;
&lt;br /&gt;
Temperature effects were also studied - the most detailed experiment was run at room temperature, as the cells did not last as long at higher temperatures, but macroscopic analysis of cell behavior at 35 C was evaluated for differences.  &lt;br /&gt;
&lt;br /&gt;
The threshold number of binding events to trigger an action potential to the brain was measured, to provide a bound on the sensitivity threshold for olfaction.   &lt;br /&gt;
 &lt;br /&gt;
Finally, additional experiments were carried out to test the dependence of the concentration of G proteins on output signal strength.  Cells from adult mice that expressed half of the normal level of G protein involved in odorant activation were compared with those from mice with normal expression.  &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The overall process of olfaction in mouse ORNs seems to match that observed in frog ORNs. &lt;br /&gt;
The unitary response was the same across odorants and cells, even though the odorants varied in efficacy and each cell had different conditions and receptors.  &lt;br /&gt;
&lt;br /&gt;
The unitary response of neurons from mice with less of the needed G protein was also the same.  This adds evidence to the theory that there is little or no amplification cascade involving those proteins, which would otherwise have a nonlinear response varying with their density.  &lt;br /&gt;
&lt;br /&gt;
The total number of receptor bindings needed to signal the brain was estimated at 20-25 unitary events, increasing slightly at lower (room) temperature.  This is comparable to the 35 events predicted as a threshold upper bound for frog ORNs. &lt;br /&gt;
&lt;br /&gt;
Some parts of this analysis differed significantly from the frog ORN study.  A completely Ca2+-free solution was used, which avoids negative feedback and adaptation, but also enhances receptor current via an inward Cl- current.  &lt;br /&gt;
&lt;br /&gt;
Further study is needed on the olfactory threshold at consciousness.  &lt;br /&gt;
It is hypothesized that it may require only one or a few ORNs are needed to trigger perception.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]] . V Bhandawat, J Reisert, K-W Yau, Science (2005)&lt;br /&gt;
* [[Signaling by olfactory receptor neurons near threshold]]. V Bhandaat, J Reisert, K-W Yau, PNAS (2010)&lt;br /&gt;
* [[The electrochemical basis of odor transduction in vertebrate olfactory cilia]].  SJ Kleene, Chem Senses (2008)&lt;br /&gt;
&lt;br /&gt;
|relevance=This paper replicates the results of [[Elementary Response of Olfactory Receptor Neurons to Odorants|Bhandawat, Reisert, and Yau]] (which used frog ORNs) with mouse ORNs.  It confirms the low amplification of smells at the single-neuron level, and provides a first upper bound on the number of odorant-binding events needed to trigger a signal in an ORN.&lt;br /&gt;
|journal=PNAS&lt;br /&gt;
|pub_date=2011/01/11&lt;br /&gt;
|doi=10.1073/pnas.1017983108&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Forces_between_clustered_stereocilia_minimize_friction_in_the_ear_on_a_subnanometre_scale&amp;diff=8899</id>
		<title>Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Forces_between_clustered_stereocilia_minimize_friction_in_the_ear_on_a_subnanometre_scale&amp;diff=8899"/>
		<updated>2012-12-15T16:34:31Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale&lt;br /&gt;
|authors=Andrei S. Kozlov, Johannes Baumgart, Thomas Risler, Corstiaen P. C. Versteegh,  A. J. Hudspeth&lt;br /&gt;
|url=http://www.ncbi.nlm.nih.gov/pmc/articles/PMC3150833/pdf/nihms313088.pdf&lt;br /&gt;
|tags=hearing, acoustics, biophysics&lt;br /&gt;
|summary=As hair bundles move, viscous friction between stereocilia and the surrounding liquid poses a physical challenge to the ear’s high sensitivity and sharp frequency selectivity. This letter proposes that some of that energy is used for frequency-selective sound amplification, through fluid–structure interaction between the liquid within the hair bundle and the stereocilia. &lt;br /&gt;
&lt;br /&gt;
A dynamic model is proposed to simulate hair bundles in a viscous environment, to see what large and small scale insights could be gained.  Finite-element analysis, a submodel of hydrodynamic forces, stochastic simulation, and models of interferometric measurement all aimed to simulate both a hair bundle in natural conditions and what might be observed in an experiment involving it.&lt;br /&gt;
&lt;br /&gt;
Forces between stereocilia are estimated, and the results suggest that the closeness of stereocilia reduces drag between them, supporting a sliding but not a squeezing mode.  Tip links may couple mechanotransduction to this low-friction sliding mode, with motion between neighboring stereocilia of less than 1nm when the hair bundle moves the larger distance [O(10nm)]needed to stimulate its channels.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
&lt;br /&gt;
On the one hand, the length scale of viscous fluids inside the ear exceeds the distance between any two stereocilia.  On the other, we know stereocilia slide past one another easily, and that the ear has sharp frequency selectivity.   &lt;br /&gt;
&lt;br /&gt;
The goal of this paper was to identify some counterintuitive properties of a hair-bundle in viscous medium and probe the molecular-level interactions of cilia with one another and with the fluid.  &lt;br /&gt;
&lt;br /&gt;
A model was designed around a bullfrog hair bundle in a viscous methylcellulose solution.  It was constructed to make it easy to change the properties of the stereocilia, with a fixed set of properties of the solution.  An initial model focused on three parameters:  pivotal stiffness, drag, and inetrial mass.  &lt;br /&gt;
This model allowed calculation of the coherence of motion of the entire bundle.&lt;br /&gt;
&lt;br /&gt;
Finally, an experiment was devised to test the theory that the magnitude of relative bundle motion depends on a balance between hydrodynamic and elastic forces, with a small relative motion varying from the highly coherent Brownian motion of the bundle.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
Top connectors were added with high stiffness (20mN/m), strongly increasing coherence and reducing drag.  These were then replaced with tip links oriented obliquely on the stereocilia, with a stiffness of 1mN/m.  This increased drag significantly.  Including both connectors and tip links led to  a model closer to observation: a drag coefficient that is not much dependent on frequency, and an overall bundle stiffness similar to that observed.&lt;br /&gt;
&lt;br /&gt;
In the physical experiment, combination frequencies were observed in a hair bundle when it was stimulated at two different frequencies at once; something that disappeared once tip links were disrupted enzymatically.  Similarly, another hair bundle in a viscous solution similar to the model was shown to gain significant drag when its top connectors were removed.   &lt;br /&gt;
|relevance=This work provides a detailed model of how hair bundles in the mammalian ear interact with the surrounding fluid, and can stimulate mechanotransduction with motion of less than 1 nm.   This model provides a quantitative understanding of how mechanotransduction can work, and describes ways that the structure of hair bundles can minimize viscous friction, resolving a potential confusion.&lt;br /&gt;
&lt;br /&gt;
This suggests further models along these lines may be helpful&lt;br /&gt;
|journal=Nature&lt;br /&gt;
|pub_date=2011/06/16&lt;br /&gt;
|doi=10.1038/nature10073&lt;br /&gt;
|subject=Biology&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8898</id>
		<title>Motility-associated hair-bundle motion in mammalian outer hair cells</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8898"/>
		<updated>2012-12-15T16:05:13Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Motility-associated hair-bundle motion in mammalian outer hair cells&lt;br /&gt;
|authors=Shuping Jia, David Z He&lt;br /&gt;
|url=http://courses.washington.edu/pbio525/Paper%20PDFs/Jia%202006%20Nat%20Neuro.pdf&lt;br /&gt;
|tags=hearing, cochlea, somatic motility&lt;br /&gt;
|summary=Mammalian hearing depends on mechanical feedback in he cochlea.  The outer hair cells (OHCs) function as the key elements in this feedback loop.   Both somatic motility and &amp;quot;active movement&amp;quot; of hair bundles are considered possible sources of motion-driven cochlear ampliﬁcation.  Active movement is known to be the source of such amplification in non-mammals, where somatic motility does not occur.   This experiment distinguishes which drives movement in part of the mammalian cochlea. &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The goal is to distinguish between somatic motility and other active movement of hair bundles in the mammalian cochlea, focusing in part on past studies of gerbils and rats which linked hair bundle movement to active movement for gerbil inner hair cells (IHCs), and rat OHCs. &lt;br /&gt;
&lt;br /&gt;
To gain precision in measurement, cochlea from four groups of subjects were studied: Adult and neonatal gerbils, he latter of which have mechanotransduction but no OHC motility yet; and both wild and prestin-knockout mice, the latter of which have normal hair bundles and mechanotransducer function, but no OHC somatic motility at all.&lt;br /&gt;
&lt;br /&gt;
Somatic motility was measured by applying a voltage across a bundle and looking for voltage-evoked motion.  Mechanotransducer currents were also measured.  To fully separate the functions of the two different source of motion, streptomycin was used as an inhibitor - it entirely blocks mechanotransducer channels and elimiates spontaneous bundle motion.  &lt;br /&gt;
&lt;br /&gt;
Hair motion was measured by looking at the magnified image of bundles at 1260x magnification, in which regime they looked like bright V-shaped lines and movement could be measured at up to 1200 Hz and down to 5nm.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
The OHCs showed bundle movement with peak responses of up to 830 nm. The movement was insensitive to manipulations that block mechanotransduction.  Adjacent OHCs were found to move in tandem with a target OHC when somatic motility was applied; a linkage which disappeared when the target OHC lost its turgor pressure.  This suggests the motion resulted from something like rotation of its reticular lamina, a feature of somatic motility.&lt;br /&gt;
&lt;br /&gt;
Finally, movement was entirely absent in neonatal OHCs and prestin-knockout OHCs. This strongly suggests that bundle movement originated in somatic motility for these specieis, and that it plays a central role in cochlear amplification in mammals.&lt;br /&gt;
&lt;br /&gt;
Sharp extracellular potential changes would be needed to drive OHCs at high frequency.  There is evidence that the organ of Corti could provide that drive, and theoretical models of OHC piezoelectric properties suggest ways their frequency response might be increased, addressing one outstanding concern with this theory.&lt;br /&gt;
&lt;br /&gt;
Finally, OHC motility can also stimulate freestanding IHC cilia, leading to their motion as well - formerly attributed to mechanotransduction.  Further study is needed to determine the source of IHC motion.&lt;br /&gt;
|relevance=This study distinguishes between two potential sources of hair-bundle motion: the reclosing of mechanotransduction channels and somatic electromotility.  Previous analyses had mainly demonstrated the possibility of either (including the possible presence of mechanotransduction-driven motion in IHCs of gerbils). &lt;br /&gt;
&lt;br /&gt;
It demonstrate conclusively that such motion is due predominantly to electromotility in the OHCs of some gerbils and mice.  It also suggests ways in which this motion in OHCs might excite IHCs and stimulate observed motion there as well, including possibly the observed motion of gerbil IHCs, which would make electromotility the primary mechanism for cochlear amplification in mammals.  This indicates  avenues for future research.&lt;br /&gt;
|journal=Nature Neuroscience&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=doi:10.1038/nn1509&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Essential_Nonlinearities_in_Hearing&amp;diff=8897</id>
		<title>Essential Nonlinearities in Hearing</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Essential_Nonlinearities_in_Hearing&amp;diff=8897"/>
		<updated>2012-12-15T15:43:27Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Essential Nonlinearities in Hearing&lt;br /&gt;
|authors=V. M. Eguíluz, M. Ospeck, Y. Choe, A. J. Hudspeth, M. O. Magnasco&lt;br /&gt;
|url=http://arxiv.org/pdf/nlin.CD/0005042.pdf&lt;br /&gt;
|tags=hearing, Hopf bifurcation, resonance&lt;br /&gt;
|summary=This paper demonstrates that three nonlinearities observed in human hearing can be predicted when the state of the hearing system is modeled by a dynamical system near a fixed point that has a Hopf bifurcation.  Recent observations of these three non-linearities are characterized.  A simple model of a system with such a bifurcation is developed, and shown to account for those non-linearities.  An analysis of  physical evidence about hair cells suggests ways in which they might operate in such a regime, and potential evolutionary advantages.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
Starting with the observation of three nonlinearities in human hearing, the authors aim to identify a model that can occur simply and accounts for all of them.  &lt;br /&gt;
&lt;br /&gt;
The three nonlinearities:&lt;br /&gt;
* Dynamic range compression: some sort of active tuning provides highly tuned responses to sounds despite damping across a very broad range.&lt;br /&gt;
*  The sharpness of mechanical tuning: no audible sound is so soft that the cochlear response is linear.   This cannot be accounted for by membrane rigidity or basic fluid mechanics, as the nonlinearity depends on the  ionic gradient.  &lt;br /&gt;
* The perception of missing harmonic tones has been tied to a nonlinearity in psychoacoustics.  Again, for this tone combination, no audible sound is too faint to drop back into a linear regime where those combination tones are not heard.&lt;br /&gt;
&lt;br /&gt;
A Hopf bifurcation at a fixed point in a dynamical system can be a very sensitive point around which to measure input.   Nonlinearities are expected, including compression, sharp tuning for small inputs, and broad tuning for large inputs.  &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
A model of a dynamical system is presented with a Hopf bifurcation, and shown to map to a resonance frequency at which infinitely sharp tuning is oberved.  An analytically computable instance of the model is developed as a homogenous osscillator, showing the three features described, and noting that they are observed independent of model parameters. &lt;br /&gt;
&lt;br /&gt;
The question of how the cochlea might keep itself near this state remains open.   It is proposed that individual hair cells themselves act at a Hopf bifurcation.  This could account for their electrical resonance.  Similarly, the otoacoustic emissions could be generated similar to the way combination tones are generated in psychoacoustic experiments.  &lt;br /&gt;
&lt;br /&gt;
The model chosen has parameters - including the Ca2+ binding kinetics and the number of hairs in a bundle - which support a locus of Hopf bifurcations with frequencies across the range of human hearing, and realistic given current observations.  A full numerical exploration by of the model by V. M. Eguíluz is awaiting publication.  &lt;br /&gt;
&lt;br /&gt;
== Key References ==&lt;br /&gt;
* M. A. Ruggero, et al.  J. Acoust. Soc. Am. 101, 2151 (1997)&lt;br /&gt;
* J.L. Goldstein, J. Acoust. Soc. Am. 41, 676 (1967)&lt;br /&gt;
* A.J. Hudspeth, Curr. Opin. Neurobiol. 7, 480 (1997)&lt;br /&gt;
|relevance=This is the first unified proposal of a single underlying mechanism that would account for three nonlinear responses of human hearing: dynamic range compression, sharp tuning, and the amplitude of combination tones. It suggests a mathematical model and identifies some experimental data suggesting there may be physical controls that map to tuning the parameters of such a model.&lt;br /&gt;
|journal=Physical Review Letters&lt;br /&gt;
|pub_date=2000/05/29&lt;br /&gt;
|doi=10.1103/PhysRevLett.84.5232&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=How_the_ear%27s_works_work&amp;diff=8896</id>
		<title>How the ear's works work</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=How_the_ear%27s_works_work&amp;diff=8896"/>
		<updated>2012-12-15T15:21:21Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=How the ear's works work&lt;br /&gt;
|authors=A. J. Hudspeth&lt;br /&gt;
|url=http://www.nature.com/nature/journal/v341/n6241/abs/341397a0.html&lt;br /&gt;
|tags=hearing, acoustics&lt;br /&gt;
|summary=This paper reviews the known physical origins of hearing and equilibrium in vertebrates, focusing on the results of studies in the 1970s and 80s particularly on the role of hair bundles in converting sound into electrical potential in the nervous system.  The contemporary understanding of structural details of the ear are summarized, including the structure of hair cells and mechanoreceptive hair bundles, transduction channels, adaptation to a range of frequencies, and the possibilities for direct mechanoelectrical transduction, driven directly by hair motion without secondary messengers.  &lt;br /&gt;
&lt;br /&gt;
Particular attention is paid to mechanisms for transduction and frequency tuning, areas of active research and study at the time.  Both positive and negative discoveries are covered, noting areas where further research is needed.  Some new micrographs and figures from the author's work are included to tie the review together.  Over 100 related papers are cited and synthesized into the review, most by other authors. &lt;br /&gt;
&lt;br /&gt;
== Overview of contemporary results ==&lt;br /&gt;
&lt;br /&gt;
;Hair cell structure and use&lt;br /&gt;
Hair cells are essential to the proper function of the ear, and similar structures are found in all vertebrates.  Hair bundles in the ear can detect tiny motions and respond to vibrations over 100,000 times a second.  It is noted that this mechanism is widely used across the animal kingdom and for a variety of sensory purposes even within the ear, with hair bundles in the cupula itself (sensitive to angular acceleration in three directions), in the organ of Corti (sensitive to sound), and in the otolithic organs (sensitive to linear horizontal and vertical acceleration).  &lt;br /&gt;
&lt;br /&gt;
The chain of  events in hearing is summarized, from displacement of the eardrum to the bones of the middle ear, to piston-like stimulation and angular acceleration of the cochlea, deflecting the cupula and flexing the basilar membrane up and down, which in turn  stimulates hair bundles in the organ of Corti.  Similar effects driven by acceleration stimulate hair cells in the otolithic membrane. &lt;br /&gt;
&lt;br /&gt;
Variations in the structure of hair bundles and individual hair cells:  Each is used as a strain gauge, opening ion channels when stimulated.  And they are very precisely located within the ear: the numer of stereocilia in a hair bundle, and their length and diameter and spacing, are completely determined by their place along the basilar membrane.   Within a stereocilium, actin filaments are cross-linked by fimbrin, greatly increasing their stiffness.&lt;br /&gt;
&lt;br /&gt;
Unresolved questions about hair growth and structure: how are the dimensions of hair bundles determined?  Can they regenerate in humans, as they do in lower vertebrates? &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
; Mechanoelectrical transduction&lt;br /&gt;
The electrical signals that convert sound into neuronal impulses are driven by opening and closing transduction channels.  These seem to be opened and closed directly by the mechanical motion of hair cells, though again the specific mechanism is a subject of open research.  The mechanism acting through some sort of elastic gating springs.  The specific transduction channels have not been isolated, but their responses have been characterized in many ways, in humans and other vertebrates.&lt;br /&gt;
&lt;br /&gt;
A deflection of a hair bundle by only 0.003 degrees - 0.3nm - leads to electrical response.   This seems to suggest a lot of noise from Brownian motion, which is expected (and observed via inteferometry) to have an rms amplitude of 2nm.  &lt;br /&gt;
&lt;br /&gt;
Most transduction current involves K+passing through transduction channels.  Some chemicals known to be toxic to the ear can enter and obstruct the channels.  There is O(1) channel per stereocilium, making them relatively difficult to see in dissection.  One potential way of locating them is through the attraction of Ca2+ to them. &lt;br /&gt;
&lt;br /&gt;
Individual bundles seem to contain elements that act as [gating] springs, whose tension controls the opening and closing of these channels.  These springs seem to absorb 50% of the force applied to bundles.  They have been difficult to locate.  However there are small strands that connect every stereocilium to the side of the longest attached process, called 'tip links' which could be those springs.&lt;br /&gt;
&lt;br /&gt;
Unresolved questions: the location and shape of transduction channels and the sites triggering transduction are not precisely known.   How could tip links be tested for demonstration that they act as springs?  Perhaps showing that they are elongated during excitement and shortened on inhibition of channels, or finding a way to remove them while measuring changes in hearing. &lt;br /&gt;
&lt;br /&gt;
; Frequency tuning&lt;br /&gt;
Frequency tuning and adaptation happens through both physical resonance - with longer hairs responding to lower frequencies - and through a separate ion channel which enables electrical resonance and damping. Adaptation involves loosening of gating spring tension.  Ca2+ may work as a second messenger in adaptation here as it does in photoreceptors.&lt;br /&gt;
&lt;br /&gt;
The physical structure of each bundle tunes it to a specific frequency, around which it may be able to distinguish sound from noise very well.  An electrical tuning and resonance is also predicted, via Ca2+-sensitive K+ channels.  &lt;br /&gt;
&lt;br /&gt;
There is evidence of active tuning by the ear as well, with cells exerting force on their surrounding and parts of the ear vibrating and emitting acoustic wavelengths to improve tuning.  Similar active tuning and emission is observed in birds and amphibians as well as mammals.  The hair bundle may collectively play a role in active tuning as well.&lt;br /&gt;
&lt;br /&gt;
Unresolved questions: it is not known how cells get tuned to an electrical resonant frequency, or how hair bundles generate force.&lt;br /&gt;
&lt;br /&gt;
; Need for speed&lt;br /&gt;
Good arguments can be made for hearing requiring very fast response to changing stimuli.  And hearing is clearly responsive to high-frequency sound.  This provides a reason for direct transduction (which is faster than any intermediated mechanism), and is needed for active echo-location such as bats use.  This may rquire gating speeds of up to 3 microseconds.  These speeds are fast compared to the diffusion timescale for transduction channels.  However direct opening of a gate or channel could speed up the process dramatically with its mechanical energy.&lt;br /&gt;
|relevance=This review article summarized the state of understanding of the internals of the vertebrate ear in 1989, particularly the role played by hair cells, summarizing some of the clearest and most unchanging data about it.  It remains current as of 2012.&lt;br /&gt;
|journal=Nature&lt;br /&gt;
|pub_date=1989/10/05&lt;br /&gt;
|doi=10.1038/341397a0&lt;br /&gt;
|subject=Biology&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8895</id>
		<title>Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Fly_motion_vision_is_based_on_Reichardt_detectors_regardless_of_the_signal-to-noise_ratio&amp;diff=8895"/>
		<updated>2012-12-15T14:27:00Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio&lt;br /&gt;
|authors=J Haag, W Denk, A Borst&lt;br /&gt;
|url=http://adsabs.harvard.edu/abs/2004PNAS..10116333H&lt;br /&gt;
|tags=vision algorithms&lt;br /&gt;
|summary=It has been theorized that fly vision might switch from relying on Reichardt detectors to relying on some other mechanism such as gradient detectors in high signal-to-noise regimes.  This paper summarizes two experiments probing those regimes and testing different parts of the fly vision chain, and finds no evidence for any mechanism other than Reichardt detectors.  &lt;br /&gt;
&lt;br /&gt;
Extra steps were taken to reduce background noise and to increase sources of signal.  One experiment was relatively casual: increasing the intensity of light in a standard test of vision.  The other was more exacting, and used two-photon excitation microscopy to get a strong signal from optical receptors (using luminescent markers on Calcium channels to see activity at the fringe of the neurons) with very low noise.  This experiment dug deeply into a specific level of fly neurology: the flies studied were eviscerated and had their proboscis removed to minimize neuronal firing from their gut (and each good for only 1 hr of experimentation); what was measured was direct response by the visual part of their neuronal plate to signals shined into their eyes.&lt;br /&gt;
&lt;br /&gt;
Results at all signal levels matched what would be expected of Reichardt detectors, and while there were some variations in response at different levels of signal intensity, no hallmarks of gradient detection were seen.&lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* [[:File:Reichardt-forever.pdf|Visual summary]] (presentation form, pdf)&lt;br /&gt;
&lt;br /&gt;
|relevance=This is a concise demonstration that a Reichardt-detector process, or something very close to it, continues to be the dominant way gradients and edges are detected in fly vision, even in environments with low noise.  &lt;br /&gt;
&lt;br /&gt;
Historically, gradient detection has been a top contender for a mechanism for vision in low-noise environments, because of their theoretical simplicity and high precision.  This experiment tried two unrelated methods of finding indications of gradient detection in fly vision, removing much more noise from their method and increasing the signal dramatically beyond previous experiments; but without success.&lt;br /&gt;
|journal=PNAS&lt;br /&gt;
|pub_date=2004/11/01&lt;br /&gt;
|doi=10.1073/pnas.0407368101&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=File:Reichardt-forever.pdf&amp;diff=8894</id>
		<title>File:Reichardt-forever.pdf</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=File:Reichardt-forever.pdf&amp;diff=8894"/>
		<updated>2012-12-15T14:26:04Z</updated>

		<summary type="html">&lt;p&gt;Sj: A summary of Haag, Denk, and Borst's  2004 paper, Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio.&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;A summary of Haag, Denk, and Borst's  2004 paper, [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]].&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Unitary_response_of_mouse_olfactory_receptor_neurons&amp;diff=8893</id>
		<title>Unitary response of mouse olfactory receptor neurons</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Unitary_response_of_mouse_olfactory_receptor_neurons&amp;diff=8893"/>
		<updated>2012-12-15T14:24:15Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Unitary response of mouse olfactory receptor neurons&lt;br /&gt;
|authors=Yair Ben-Chaim a,1 , Melody M. Cheng b , and King-Wai Yau a,1&lt;br /&gt;
|url=http://www.pnas.org/content/108/2/822&lt;br /&gt;
|tags=olfaction mouse&lt;br /&gt;
|summary=This paper studies the response of mouse olfactory receptor neurons [ORNs] to a variety of odorants, and notes that the response is relatively uniform in amplitude and kinetics, unchanging across different neurons and different odors (hence 'elementary' or 'unitary' - responding to the entire experience of a novel smell as a single smelling-event).  The experiment involved followed earlier work by Yau and others on frog ORNs, showing that the same results hold for mice and so possibly for other mammals.  &lt;br /&gt;
&lt;br /&gt;
The olfactory response similar for different clusters of odorants  it had little amplification, triggering transduction through only just single molecular complex.  Successful response required only O(10) successful binding events.  Both traits are similar to the results found for frog ORNs in the earlier work. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
The primary goal was to check the similarity between responses of mouse and frog ORNs to address the question of whether the properties of olfactory response in mammals might have similar traits.  Existing methodology was repeated with mouse cells: short bursts of odorants, varying either the concentration in bursts of fixed length or the length of bursts of fixed concentration.  &lt;br /&gt;
&lt;br /&gt;
The method used carried out a quantal analysis on results, assuming there was a minimum unitary response, and a Poisson distribution of individual responses.  The suction-pipette method was used to measure membrane currents.  As there are 1000 species of OR cells, a mixture of five odorants was used instead of two.&lt;br /&gt;
&lt;br /&gt;
Temperature effects were also studied - the most detailed experiment was run at room temperature, as the cells did not last as long at higher temperatures, but macroscopic analysis of cell behavior at 35 C was evaluated for differences.  &lt;br /&gt;
&lt;br /&gt;
The threshold number of binding events to trigger an action potential to the brain was measured, to provide a bound on the sensitivity threshold for olfaction.   &lt;br /&gt;
 &lt;br /&gt;
Finally, additional experiments were carried out to test the dependence of the concentration of G proteins on output signal strength.  Cells from adult mice that expressed half of the normal level of G protein involved in odorant activation were compared with those from mice with normal expression.  &lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The overall process of olfaction in mouse ORNs seems to match that observed in frog ORNs. &lt;br /&gt;
The unitary response was the same across odorants and cells, even though the odorants varied in efficacy and each cell had different conditions and receptors.  &lt;br /&gt;
&lt;br /&gt;
The unitary response of neurons from mice with less of the needed G protein was also the same.  This adds evidence to the theory that there is little or no amplification cascade involving those proteins, which would otherwise have a nonlinear response varying with their density.  &lt;br /&gt;
&lt;br /&gt;
The total number of receptor bindings needed to signal the brain was estimated at 20-25 unitary events, increasing slightly at lower (room) temperature.  This is comparable to the 35 events predicted as a threshold upper bound for frog ORNs. &lt;br /&gt;
&lt;br /&gt;
Some parts of this analysis differed significantly from the frog ORN study.  A completely Ca2+-free solution was used, which avoids negative feedback and adaptation, but also enhances receptor current via an inward Cl- current.  &lt;br /&gt;
&lt;br /&gt;
Further study is needed on the olfactory threshold at consciousness.  &lt;br /&gt;
It is hypothesized that it may require only one or a few ORNs are needed to trigger perception.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]] . V Bhandawat, J Reisert, K-W Yau, Science (2005)&lt;br /&gt;
* [[Signaling by olfactory receptor neurons near threshold]]. V Bhandaat, J Reisert, K-W Yau, PNAS (2010)&lt;br /&gt;
* [[The electrochemical basis of odor transduction in vertebrate olfactory cilia]].  SJ Kleene, Chem Senses (2008)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&lt;br /&gt;
|relevance=This paper replicates the results of [[Elementary Response of Olfactory Receptor Neurons to Odorants|Bhandawat, Reisert, and Yau]] (which used frog ORNs) with mouse ORNs.  It confirms the low amplification of smells at the single-neuron level, and provides a first upper bound on the number of odorant-binding events needed to trigger a signal in an ORN.&lt;br /&gt;
|journal=PNAS&lt;br /&gt;
|pub_date=2011/01/11&lt;br /&gt;
|doi=10.1073/pnas.1017983108&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8892</id>
		<title>Elementary Response of Olfactory Receptor Neurons to Odorants</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8892"/>
		<updated>2012-12-15T14:15:32Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Elementary Response of Olfactory Receptor Neurons to Odorants&lt;br /&gt;
|authors=Vikas Bhandawat, Johannes Reisert, King-Wai Yau&lt;br /&gt;
|url=http://www.sciencemag.org/content/308/5730/1931.long&lt;br /&gt;
|tags=olfaction, GTP, transduction&lt;br /&gt;
|summary=This paper describes experiments testing the response of frogs' olfactory neurons to odors, to see how they amplify the signal of an odor.  This is compared to the visual amplification of single photons (through a phototransduction cascade).  The two mechanisms are shown to be quite different at the level of individual neurons.  The frog response is estimated for two odorants with very different response efficiencies, and the statistics of the results interpreted to give insight into the underlying process.&lt;br /&gt;
&lt;br /&gt;
Questions about how to maintain olfactory sensitivity under the observed model are raised, and some theoretical explanations are proposed that involve synthesis across many neurons, but without related experiment. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
This experiment aimed to probe the relation between responses of frog olfactory receptors to odor stimuli, and the intensity and duration of those stimuli.  Working from knowledge of the specific proteins and cation channels involved in olfactory reception, the authors set out to develop a technique to stimulate isolated olfactory neurons of a frog, in Ringer solution (to stimulate a physical environment), while measuring resulting membrane currents.  &lt;br /&gt;
&lt;br /&gt;
This method assumed that there was some smallest quantum of response to odor detection, and that any observed response was some combination of these elementary (or 'unitary') units of response.  This followed quantal analysis originally developed by Castillo and Katz in 1954.  To do this required avoiding non-linear variations away from those simplest responses.  &lt;br /&gt;
&lt;br /&gt;
Olfactory adaptation was minimized: cells were known to adapt in the presence of Ca2+, leading to a non-linear dose-response relation.  The experiment minimized this concentration, while confirming its impact on the results by repeating its tests in solutions with different concentrations of Ca2+ (replaced in low-Ca solutions with Mg2+) : tests were run with cells in regular Ringer solution, 20μM Ca2+, and 100nM Ca2+ solution.&lt;br /&gt;
&lt;br /&gt;
Two odorants that ORNs were known to resopnd to very differently (acetophenone and cineole) were used to get a sense of response variation across different regimes of odorant binding and saturation.  the dwell-time of the two odorants different by roughly a magnitude.  The results were analyzed to see how long the receptor-odorant complexes lasted, and what could be understood about the activation of G proteins during the process.  This was compared to the better known process of rhodopsin amplification cascade in which photoisomerized rhodopsin triggers a cascade of transducins before being shutoff by phosphorylation.&lt;br /&gt;
&lt;br /&gt;
Concentration of odorants was varied both by using increasingly long pulses of low concentration, and by using increasingly intense pulses of fixed concentration odors, with similar results.&lt;br /&gt;
&lt;br /&gt;
The unitary amplitude for a given response was measured as the transient peak of the response, assuming a Poisson distribution.  Membrane currents were measured using the suction-pipette method.  Where appropriate observations matched well to a least-squares fit to the Hill equation, which applies to such situations where cooperative binding is expected.  &lt;br /&gt;
&lt;br /&gt;
Quantal analysis and linear extrapolation from lower-concentration solutions allows the estimate of the unitary response in normal Ringer solution, even though the macroscopic response is nonlinear.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The unitary current stimulated by each and the overall response kinetics were similar for both odorants across five different cells.  This unit of response varied primarily with the concentration of Ca2+ in the solution, and was consistent across different cells, though it is expected that every cell has different binding receptor.   &lt;br /&gt;
&lt;br /&gt;
A simple check for whether a quantal / unitary response is detected is the linearity of the relationship between concentration and response.  If many different binding events start to overlap spatially, transduction effects would not be linear, so the observed response would be supralinear.  And indeed in low-Ca2+ environments a linear response was seen, at both 100nM and 20μM Ca2+, up to a certain odorant concentration.  The unitary current in Ringer solution is estimated to be roughly 0.03pA, 100 times smaller than previously measured by Menini, et al.&lt;br /&gt;
&lt;br /&gt;
The response was analyzed for possible amplification cascades involved in converting those stimuli to signals from GTP-binding [G] proteins.  The dwell-time of odorants was found to be quite small, under 1ms.  Moreover the response time to odors was fast and steady: the linear increase in total response to a pulse of fixed molarity but different duration had a projected time-intercept of 0, indicating that some response was taking place very soon after the odor was released.&lt;br /&gt;
&lt;br /&gt;
Each bound odorant seemed to have a low probability of activating a single G protein, which in turn has a low probability of activating more than one adenylyl cyclase molecule.  This is projected from the overall linearity of response across a wide range of odor saturations.  Even when all receptors were expected to be bound to cineole, the highly effective odorant, the total response amplitude continued to increase linearly with pulse duration.  &lt;br /&gt;
&lt;br /&gt;
These results were compared to known response patterns of optical neurons to light at low levels of stimulation.  In contrast, rod phototransduction acts through photoisomerized rhodopsin activating a transducin cascade.  This experiment suggests that such a mechanism may not exist for olfaction, and that the odorant-receptor complexes may generally be too short lived to trigger any mechanisms that might exist.  Moreover, each receptor, once activated, did not seem to be inactivated for at least 100ms.&lt;br /&gt;
&lt;br /&gt;
Some further understanding of the workings of receptors once they bind to an odorant are needed.  The authors suggest that they may integrate responses when an odorant binds to them repeatedly without being phosphorylated.  Moreover, the glomerulus in the olfactory bulb of the frog can integrate signals from all ORNs, perhaps separately integrating them for each receptor.&lt;br /&gt;
&lt;br /&gt;
Unlike with photons, each odorant can go on to bind many times at the same site or at different sites.   And unlike with an eye of fixed size, which is difficult to modify within the structure of its host, the surface area of olfactory epithelium can readily be expanded.  This could have a proportional improvement in olfactory sensitivity.&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
== References ==&lt;br /&gt;
* Measurement process:  [[Quantal Components of the End-Plate Potential]]. Castillo and Katz, [http://jp.physoc.org/content/124/3/560.full.pdf+html?ijkey=6ff0ca7eede96a5d444b7154dd088b836af7997f&amp;amp;keytype2=tf_ipsecsha Journal of Physiology] (1954)&lt;br /&gt;
* S. J. Kleene, Neuroscience 66, 1001 (1995)&lt;br /&gt;
|relevance=This is a study of low-level components of one olfactory system that suggest the sorts of sensory models which may be studied in further experiments.  It provides a benchmark for similar work in other animals and at other levels in the frog.  &lt;br /&gt;
&lt;br /&gt;
The unitary response of individual ORNs was calculated to be 100x smaller than previously reported. (0.03 pA)&lt;br /&gt;
|journal=Science&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=10.1126/science.1109886&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8891</id>
		<title>Elementary Response of Olfactory Receptor Neurons to Odorants</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8891"/>
		<updated>2012-12-15T14:07:42Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Elementary Response of Olfactory Receptor Neurons to Odorants&lt;br /&gt;
|authors=Vikas Bhandawat, Johannes Reisert, King-Wai Yau&lt;br /&gt;
|url=http://www.sciencemag.org/content/308/5730/1931.long&lt;br /&gt;
|tags=olfaction, GTP, transduction&lt;br /&gt;
|summary=This paper describes experiments testing the response of frogs' olfactory neurons to odors, to see how they amplify the signal of an odor.  This is compared to the visual amplification of single photons (through a phototransduction cascade).  The two mechanisms are shown to be quite different at the level of individual neurons.  The frog response is estimated for two odorants with very different response efficiencies, and the statistics of the results interpreted to give insight into the underlying process.&lt;br /&gt;
&lt;br /&gt;
Questions about how to maintain olfactory sensitivity under the observed model are raised, and some theoretical explanations are proposed that involve synthesis across many neurons, but without related experiment. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
This experiment aimed to probe the relation between responses of frog olfactory receptors to odor stimuli, and the intensity and duration of those stimuli.  Working from knowledge of the specific proteins and cation channels involved in olfactory reception, the authors set out to develop a technique to stimulate isolated olfactory neurons of a frog, in Ringer solution (to stimulate a physical environment), while measuring resulting membrane currents.  &lt;br /&gt;
&lt;br /&gt;
This method assumed that there was some smallest quantum of response to odor detection, and that any observed response was some combination of these elementary (or 'unitary') units of response.  This followed quantal analysis originally developed by Castillo and Katz in 1954.  To do this required avoiding non-linear variations away from those simplest responses.  &lt;br /&gt;
&lt;br /&gt;
Olfactory adaptation was minimized: cells were known to adapt in the presence of Ca2+, leading to a non-linear dose-response relation.  The experiment minimized this concentration, while confirming its impact on the results by repeating its tests in solutions with different concentrations of Ca2+ (replaced in low-Ca solutions with Mg2+) : tests were run with cells in regular Ringer solution, 20μM Ca2+, and 100nM Ca2+ solution.&lt;br /&gt;
&lt;br /&gt;
Two odorants that ORNs were known to resopnd to very differently (acetophenone and cineole) were used to get a sense of response variation across different regimes of odorant binding and saturation.  the dwell-time of the two odorants different by roughly a magnitude.  The results were analyzed to see how long the receptor-odorant complexes lasted, and what could be understood about the activation of G proteins during the process.  This was compared to the better known process of rhodopsin amplification cascade in which photoisomerized rhodopsin triggers a cascade of transducins before being shutoff by phosphorylation.&lt;br /&gt;
&lt;br /&gt;
The unitary amplitude for a given response was measured as the transient peak of the response, assuming a Poisson distribution.  Membrane currents were measured using the suction-pipette method.  Where appropriate observations matched well to a least-squares fit to the Hill equation, which applies to such situations where cooperative binding is expected.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The unitary current stimulated by each and the overall response kinetics were similar for both odorants across five different cells.  This unit of response varied primarily with the concentration of Ca2+ in the solution, and was consistent across different cells, though it is expected that every cell has different binding receptor.  &lt;br /&gt;
&lt;br /&gt;
A simple check for whether a quantal / unitary response is detected is the linearity of the relationship between concentration and response.  If many different binding events start to overlap spatially, transduction effects would not be linear, so the observed response would be supralinear.  And indeed in low-Ca2+ environments a linear response was seen, at both 100nM and 20μM Ca2+, up to a certain odorant concentration.  Concentration was varied both by using increasingly long pulses of low concentration, and by using increasingly intense pulses of fixed concentration odors, with similar results.&lt;br /&gt;
&lt;br /&gt;
The response was analyzed for possible amplification cascades involved in converting those stimuli to signals from GTP-binding [G] proteins.  The dwell-time of odorants was found to be quite small, under 1ms.  Moreover the response time to odors was fast and steady: the linear increase in total response to a pulse of fixed molarity but different duration had a projected time-intercept of 0, indicating that some response was taking place very soon after the odor was released.&lt;br /&gt;
&lt;br /&gt;
Each bound odorant seemed to have a low probability of activating a single G protein, which in turn has a low probability of activating more than one adenylyl cyclase molecule.  This is projected from the overall linearity of response across a wide range of odor saturations.  Even when all receptors were expected to be bound to cineole, the highly effective odorant, the total response amplitude continued to increase linearly with pulse duration.  &lt;br /&gt;
&lt;br /&gt;
These results were compared to known response patterns of optical neurons to light at low levels of stimulation.  In contrast, rod phototransduction acts through photoisomerized rhodopsin activating a transducin cascade.  This experiment suggests that such a mechanism may not exist for olfaction, and that the odorant-receptor complexes may generally be too short lived to trigger any mechanisms that might exist.  Moreover, each receptor, once activated, did not seem to be inactivated for at least 100ms.&lt;br /&gt;
&lt;br /&gt;
Some further understanding of the workings of receptors once they bind to an odorant are needed.  The authors suggest that they may integrate responses when an odorant binds to them repeatedly without being phosphorylated.  Moreover, the glomerulus in the olfactory bulb of the frog can integrate signals from all ORNs, perhaps separately integrating them for each receptor.&lt;br /&gt;
&lt;br /&gt;
Unlike with photons, each odorant can go on to bind many times at the same site or at different sites.   And unlike with an eye of fixed size, which is difficult to modify within the structure of its host, the surface area of olfactory epithelium can readily be expanded.  This could have a proportional improvement in olfactory sensitivity.&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
== References ==&lt;br /&gt;
* Measurement process:  [[Quantal Components of the End-Plate Potential]]. Castillo and Katz, [http://jp.physoc.org/content/124/3/560.full.pdf+html?ijkey=6ff0ca7eede96a5d444b7154dd088b836af7997f&amp;amp;keytype2=tf_ipsecsha Journal of Physiology] (1954)&lt;br /&gt;
* S. J. Kleene, Neuroscience 66, 1001 (1995)&lt;br /&gt;
|relevance=This is a study of low-level components of one olfactory system that suggest the sorts of sensory models which may be studied in further experiments.  It provides a benchmark for similar work in other animals and at other levels in the frog.&lt;br /&gt;
|journal=Science&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=10.1126/science.1109886&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8890</id>
		<title>Elementary Response of Olfactory Receptor Neurons to Odorants</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8890"/>
		<updated>2012-12-15T14:05:28Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Elementary Response of Olfactory Receptor Neurons to Odorants&lt;br /&gt;
|authors=Vikas Bhandawat, Johannes Reisert, King-Wai Yau&lt;br /&gt;
|url=http://www.sciencemag.org/content/308/5730/1931.long&lt;br /&gt;
|tags=olfaction, GTP, transduction&lt;br /&gt;
|summary=This paper describes experiments testing the response of frogs' olfactory neurons to odors, to see how they amplify the signal of an odor.  This is compared to the visual amplification of single photons (through a phototransduction cascade).  The two mechanisms are shown to be quite different at the level of individual neurons.  The frog response is estimated for two odorants with very different response efficiencies, and the statistics of the results interpreted to give insight into the underlying process.&lt;br /&gt;
&lt;br /&gt;
Questions about how to maintain olfactory sensitivity under the observed model are raised, and some theoretical explanations are proposed that involve synthesis across many neurons, but without related experiment. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
This experiment aimed to probe the relation between responses of frog olfactory receptors to odor stimuli, and the intensity and duration of those stimuli.  Working from knowledge of the specific proteins and cation channels involved in olfactory reception, the authors set out to develop a technique to stimulate isolated olfactory neurons of a frog, in Ringer solution (to stimulate a physical environment), while measuring resulting membrane currents.  &lt;br /&gt;
&lt;br /&gt;
This method assumed that there was some smallest quantum of response to odor detection, and that any observed response was some combination of these elementary (or 'unitary') units of response.  This followed quantal analysis originally developed by Castillo and Katz in 1954.  To do this required avoiding non-linear variations away from those simplest responses.  &lt;br /&gt;
&lt;br /&gt;
Olfactory adaptation was minimized: cells were known to adapt in the presence of Ca2+, leading to a non-linear dose-response relation.  The experiment minimized this concentration, while confirming its impact on the results by repeating its tests in solutions with different concentrations of Ca2+ (replaced in low-Ca solutions with Mg2+) : tests were run with cells in regular Ringer solution, 20μM Ca2+, and 100nM Ca2+ solution.&lt;br /&gt;
&lt;br /&gt;
Two odorants that ORNs were known to resopnd to very differently (acetophenone and cineole) were used to get a sense of response variation across different regimes of odorant binding and saturation.  the dwell-time of the two odorants different by roughly a magnitude.  The results were analyzed to see how long the receptor-odorant complexes lasted, and what could be understood about the activation of G proteins during the process.  This was compared to the better known process of rhodopsin amplification cascade in which photoisomerized rhodopsin triggers a cascade of transducins before being shutoff by phosphorylation.&lt;br /&gt;
&lt;br /&gt;
The unitary amplitude for a given response was measured as the transient peak of the response, assuming a Poisson distribution.  Membrane currents were measured using the suction-pipette method.  Observations were matched to a least-squares fit to the Hill equation, which applies to such situations where cooperative binding is expected.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The unitary current stimulated by each and the overall response kinetics were similar for both odorants across five different cells.  This unit of response varied primarily with the concentration of Ca2+ in the solution, and was consistent across different cells, though it is expected that every cell has different binding receptor.  &lt;br /&gt;
&lt;br /&gt;
A simple check for whether a quantal / unitary response is detected is the linearity of the relationship between concentration and response.  If many different binding events start to overlap spatially, transduction effects would not be linear, so the observed response would be supralinear.  And indeed in low-Ca2+ environments a linear response was seen, at both 100nM and 20μM Ca2+, up to a certain odorant concentration.  Concentration was varied both by using increasingly long pulses of low concentration, and by using increasingly intense pulses of fixed concentration odors, with similar results.&lt;br /&gt;
&lt;br /&gt;
The response was analyzed for possible amplification cascades involved in converting those stimuli to signals from GTP-binding [G] proteins.  The dwell-time of odorants was found to be quite small, under 1ms.  Moreover the response time to odors was fast and steady: the linear increase in total response to a pulse of fixed molarity but different duration had a projected time-intercept of 0, indicating that some response was taking place very soon after the odor was released.&lt;br /&gt;
&lt;br /&gt;
Each bound odorant seemed to have a low probability of activating a single G protein, which in turn has a low probability of activating more than one adenylyl cyclase molecule.  This is projected from the overall linearity of response across a wide range of odor saturations.  Even when all receptors were expected to be bound to cineole, the highly effective odorant, the total response amplitude continued to increase linearly with pulse duration.  &lt;br /&gt;
&lt;br /&gt;
These results were compared to known response patterns of optical neurons to light at low levels of stimulation.  In contrast, rod phototransduction acts through photoisomerized rhodopsin activating a transducin cascade.  This experiment suggests that such a mechanism may not exist for olfaction, and that the odorant-receptor complexes may generally be too short lived to trigger any mechanisms that might exist.  Moreover, each receptor, once activated, did not seem to be inactivated for at least 100ms.&lt;br /&gt;
&lt;br /&gt;
Some further understanding of the workings of receptors once they bind to an odorant are needed.  The authors suggest that they may integrate responses when an odorant binds to them repeatedly without being phosphorylated.  Moreover, the glomerulus in the olfactory bulb of the frog can integrate signals from all ORNs, perhaps separately integrating them for each receptor.&lt;br /&gt;
&lt;br /&gt;
Unlike with photons, each odorant can go on to bind many times at the same site or at different sites.   And unlike with an eye of fixed size, which is difficult to modify within the structure of its host, the surface area of olfactory epithelium can readily be expanded.  This could have a proportional improvement in olfactory sensitivity.&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
== References ==&lt;br /&gt;
* Measurement process:  [[Quantal Components of the End-Plate Potential]]. Castillo and Katz, [http://jp.physoc.org/content/124/3/560.full.pdf+html?ijkey=6ff0ca7eede96a5d444b7154dd088b836af7997f&amp;amp;keytype2=tf_ipsecsha Journal of Physiology] (1954)&lt;br /&gt;
* S. J. Kleene, Neuroscience 66, 1001 (1995)&lt;br /&gt;
|relevance=This is a study of low-level components of one olfactory system that suggest the sorts of sensory models which may be studied in further experiments.  It provides a benchmark for similar work in other animals and at other levels in the frog.&lt;br /&gt;
|journal=Science&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=10.1126/science.1109886&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8889</id>
		<title>Elementary Response of Olfactory Receptor Neurons to Odorants</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8889"/>
		<updated>2012-12-15T13:48:27Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Elementary Response of Olfactory Receptor Neurons to Odorants&lt;br /&gt;
|authors=Vikas Bhandawat, Johannes Reisert, King-Wai Yau&lt;br /&gt;
|url=http://www.sciencemag.org/content/308/5730/1931.long&lt;br /&gt;
|tags=olfaction, GTP, transduction&lt;br /&gt;
|summary=This paper describes experiments testing the response of frogs' olfactory neurons to odors, to see how they amplify the signal of an odor.  This is compared to the visual amplification of single photons (through a phototransduction cascade).  The two mechanisms are shown to be quite different at the level of individual neurons.  The frog response is estimated for two odorants with very different response efficiencies, and the statistics of the results interpreted to give insight into the underlying process.&lt;br /&gt;
&lt;br /&gt;
Questions about how to maintain olfactory sensitivity under the observed model are raised, and some theoretical explanations are proposed that involve synthesis across many neurons, but without related experiment. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
This experiment aimed to probe the relation between responses of frog olfactory receptors to odor stimuli, and the intensity and duration of those stimuli.  Working from knowledge of the specific proteins and cation channels involved in olfactory reception, the authors set out to develop a technique to stimulate isolated olfactory neurons of a frog, in Ringer solution (to stimulate a physical environment), while measuring resulting membrane currents.  &lt;br /&gt;
&lt;br /&gt;
This method assumed that there was some smallest quantum of response to odor detection, and that any observed response was some combination of these elementary (or 'unitary') units of response.  This followed quantal analysis originally developed by Castillo and Katz in 1954.  To do this required avoiding non-linear variations away from those simplest responses.  &lt;br /&gt;
&lt;br /&gt;
Olfactory adaptation was minimized: cells were known to adapt in the presence of Ca2+, leading to a non-linear dose-response relation.  The experiment minimized this concentration, while confirming its impact on the results by repeating its tests in solutions with different concentrations of Ca2+ (replaced in low-Ca solutions with Mg2+) : tests were run with cells in regular Ringer solution, 20μM Ca2+, and 100nM Ca2+ solution.&lt;br /&gt;
&lt;br /&gt;
Two odorants that ORNs were known to resopnd to very differently (acetophenone and cineole) were used to get a sense of response variation across different regimes of odorant binding and saturation.  the dwell-time of the two odorants different by roughly a magnitude.  The results were analyzed to see how long the receptor-odorant complexes lasted, and what could be understood about the activation of G proteins during the process.  This was compared to the better known process of rhodopsin amplification cascade in which photoisomerized rhodopsin triggers a cascade of transducins before being shutoff by phosphorylation.&lt;br /&gt;
&lt;br /&gt;
The unitary amplitude for a given response was measured as the transient peak of the response, assuming a Poisson distribution.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The unitary current stimulated by each and the overall response kinetics were similar for both odorants across five different cells.  This unit of response varied primarily with the concentration of Ca2+ in the solution, and was consistent across different cells, though it is expected that every cell has different binding receptor.  &lt;br /&gt;
&lt;br /&gt;
A simple check for whether a quantal / unitary response is detected is the linearity of the relationship between concentration and response.  If many different binding events start to overlap spatially, transduction effects would not be linear, so the observed response would be supralinear.  And indeed in low-Ca2+ environments a linear response was seen, at both 100nM and 20μM Ca2+, up to a certain odorant concentration.  Concentration was varied both by using increasingly long pulses of low concentration, and by using increasingly intense pulses of fixed concentration odors, with similar results.&lt;br /&gt;
&lt;br /&gt;
The response was analyzed for possible amplification cascades involved in converting those stimuli to signals from GTP-binding [G] proteins.  The dwell-time of odorants was found to be quite small, under 1ms.  Moreover the response time to odors was fast and steady: the linear increase in total response to a pulse of fixed molarity but different duration had a projected time-intercept of 0, indicating that some response was taking place very soon after the odor was released.&lt;br /&gt;
&lt;br /&gt;
Each bound odorant seemed to have a low probability of activating a single G protein, which in turn has a low probability of activating more than one adenylyl cyclase molecule.  This is projected from the overall linearity of response across a wide range of odor saturations.  Even when all receptors were expected to be bound to cineole, the highly effective odorant, the total response amplitude continued to increase linearly with pulse duration.  &lt;br /&gt;
&lt;br /&gt;
These results were compared to known response patterns of optical neurons to light at low levels of stimulation.  In contrast, rod phototransduction acts through photoisomerized rhodopsin activating a transducin cascade.  This experiment suggests that such a mechanism may not exist for olfaction, and that the odorant-receptor complexes may generally be too short lived to trigger any mechanisms that might exist.  Moreover, each receptor, once activated, did not seem to be inactivated for at least 100ms.&lt;br /&gt;
&lt;br /&gt;
Some further understanding of the workings of receptors once they bind to an odorant are needed.  The authors suggest that they may integrate responses when an odorant binds to them repeatedly without being phosphorylated.  Moreover, the glomerulus in the olfactory bulb of the frog can integrate signals from all ORNs, perhaps separately integrating them for each receptor.&lt;br /&gt;
&lt;br /&gt;
Unlike with photons, each odorant can go on to bind many times at the same site or at different sites.   And unlike with an eye of fixed size, which is difficult to modify within the structure of its host, the surface area of olfactory epithelium can readily be expanded.  This could have a proportional improvement in olfactory sensitivity.&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
== References ==&lt;br /&gt;
* Measurement process:  [[Quantal Components of the End-Plate Potential]]. Castillo and Katz, [http://jp.physoc.org/content/124/3/560.full.pdf+html?ijkey=6ff0ca7eede96a5d444b7154dd088b836af7997f&amp;amp;keytype2=tf_ipsecsha Journal of Physiology] (1954)&lt;br /&gt;
* S. J. Kleene, Neuroscience 66, 1001 (1995)&lt;br /&gt;
|relevance=This is a study of low-level components of one olfactory system that suggest the sorts of sensory models which may be studied in further experiments.  It provides a benchmark for similar work in other animals and at other levels in the frog.&lt;br /&gt;
|journal=Science&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=10.1126/science.1109886&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8888</id>
		<title>Elementary Response of Olfactory Receptor Neurons to Odorants</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8888"/>
		<updated>2012-12-15T13:44:32Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Elementary Response of Olfactory Receptor Neurons to Odorants&lt;br /&gt;
|authors=Vikas Bhandawat, Johannes Reisert, King-Wai Yau&lt;br /&gt;
|url=http://www.sciencemag.org/content/308/5730/1931.long&lt;br /&gt;
|tags=olfaction, GTP, transduction&lt;br /&gt;
|summary=This paper describes experiments testing the response of frogs' olfactory neurons to odors, to see how they amplify the signal of an odor.  This is compared to the visual amplification of single photons (through a phototransduction cascade).  The two mechanisms are shown to be quite different at the level of individual neurons.  The frog response is estimated for two odorants with very different response efficiencies, and the statistics of the results interpreted to give insight into the underlying process.&lt;br /&gt;
&lt;br /&gt;
Questions about how to maintain olfactory sensitivity under the observed model are raised, and some theoretical explanations are proposed that involve synthesis across many neurons, but without related experiment. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
This experiment aimed to probe the relation between responses of frog olfactory receptors to odor stimuli, and the intensity and duration of those stimuli.  Working from knowledge of the specific proteins and cation channels involved in olfactory reception, the authors set out to develop a technique to stimulate isolated olfactory neurons of a frog, in Ringer solution (to stimulate a physical environment), while measuring resulting membrane currents.  &lt;br /&gt;
&lt;br /&gt;
This method assumed that there was some smallest quantum of response to odor detection, and that any observed response was some combination of these elementary (or 'unitary') units of response.  This followed quantal analysis originally developed by Castillo and Katz in 1954.  To do this required avoiding non-linear variations away from those simplest responses.  &lt;br /&gt;
&lt;br /&gt;
Olfactory adaptation was minimized: cells were known to adapt in the presence of Ca2+, leading to a non-linear dose-response relation.  The experiment minimized this concentration, while confirming its impact on the results by repeating its tests in solutions with different concentrations of Ca2+ (replaced in low-Ca solutions with Mg2+) : tests were run with cells in regular Ringer solution, 20μM Ca2+, and 100nM Ca2+ solution.&lt;br /&gt;
&lt;br /&gt;
Two odorants that ORNs were known to resopnd to very differently (acetophenone and cineole) were used to get a sense of response variation across different regimes of odorant binding and saturation.  the dwell-time of the two odorants different by roughly a magnitude.  The results were analyzed to see how long the receptor-odorant complexes lasted, and what could be understood about the activation of G proteins during the process.  This was compared to the better known process of rhodopsin amplification cascade in which photoisomerized rhodopsin triggers a cascade of transducins before being shutoff by phosphorylation.&lt;br /&gt;
&lt;br /&gt;
The unitary amplitude for a given response was measured as the transient peak of the response, assuming a Poisson distribution.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The unitary current stimulated by each and the overall response kinetics were similar for both odorants across five different cells.  This unit of response varied primarily with the concentration of Ca2+ in the solutino, and was consistent across different cells, though it is expected that every cell has different binding receptor.  &lt;br /&gt;
&lt;br /&gt;
A simple check for whether a quantal / unitary response is detected is the linearity of the relationship between concentration and response.  If many different binding events start to overlap spatially, transduction effects would not be linear, so the observed response would be supralinear.  And indeed in low-Ca2+ environments a linear response was seen, at both 100nM and 20μM Ca2+, up to a certain odorant concentration.  Concentration was varied both by using increasingly long pulses of low concentration, and by using increasingly intense pulses of fixed concentration odors, with similar results.&lt;br /&gt;
&lt;br /&gt;
The response was analyzed for possible amplification cascades involved in converting those stimuli to signals from GTP-binding [G] proteins.  The dwell-time of odorants was found to be quite small, under 1ms.  Moreover the response time to odors was fast and steady: the linear increase in total response to a pulse of fixed molarity but different duration had a projected time-intercept of 0, indicating that some response was taking place very soon after the odor was released.&lt;br /&gt;
&lt;br /&gt;
Each bound odorant seemed to have a low probability of activating a single G protein, which in turn has a low probability of activating more than one adenylyl cyclase molecule.  This is projected from the overall linearity of response across a wide range of odor saturations.  Even when all receptors were expected to be bound to cineole, the highly effective odorant, the total response amplitude continued to increase linearly with pulse duration.  &lt;br /&gt;
&lt;br /&gt;
These results were compared to known response patterns of optical neurons to light at low levels of stimulation.  In contrast, rod phototransduction acts through photoisomerized rhodopsin activating a transducin cascade.  This experiment suggests that such a mechanism may not exist for olfaction, and that the odorant-receptor complexes may generally be too short lived to trigger any mechanisms that might exist.  Moreover, each receptor, once activated, did not seem to be inactivated for at least 100ms.&lt;br /&gt;
&lt;br /&gt;
Some further understanding of the workings of receptors once they bind to an odorant are needed.  The authors suggest that they may integrate responses when an odorant binds to them repeatedly without being phosphorylated.  Moreover, the glomerulus in the olfactory bulb of the frog can integrate signals from all ORNs, perhaps separately integrating them for each receptor.&lt;br /&gt;
&lt;br /&gt;
Unlike with photons, each odorant can go on to bind many times at the same site or at different sites.   And unlike with an eye of fixed size, which is difficult to modify within the structure of its host, the surface area of olfactory epithelium can readily be expanded.  This could have a proportional improvement in olfactory sensitivity.&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
== References ==&lt;br /&gt;
* Measurement process:  [[Quantal Components of the End-Plate Potential]]. Castillo and Katz, [http://jp.physoc.org/content/124/3/560.full.pdf+html?ijkey=6ff0ca7eede96a5d444b7154dd088b836af7997f&amp;amp;keytype2=tf_ipsecsha Journal of Physiology] (1954)&lt;br /&gt;
* S. J. Kleene, Neuroscience 66, 1001 (1995)&lt;br /&gt;
|relevance=This is a study of low-level components of one olfactory system that suggest the sorts of sensory models which may be studied in further experiments.  It provides a benchmark for similar work in other animals and at other levels in the frog.&lt;br /&gt;
|journal=Science&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=10.1126/science.1109886&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8887</id>
		<title>Elementary Response of Olfactory Receptor Neurons to Odorants</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Elementary_Response_of_Olfactory_Receptor_Neurons_to_Odorants&amp;diff=8887"/>
		<updated>2012-12-15T13:40:03Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Elementary Response of Olfactory Receptor Neurons to Odorants&lt;br /&gt;
|authors=Vikas Bhandawat, Johannes Reisert, King-Wai Yau&lt;br /&gt;
|url=http://www.sciencemag.org/content/308/5730/1931.long&lt;br /&gt;
|tags=olfaction, GTP, transduction&lt;br /&gt;
|summary=This paper describes experiments testing the response of frogs' olfactory neurons to odors, to see how they amplify the signal of an odor.  This is compared to the visual amplification of single photons (through a phototransduction cascade).  The two mechanisms are shown to be quite different at the level of individual neurons.  The frog response is estimated for two odorants with very different response efficiencies, and the statistics of the results interpreted to give insight into the underlying process.&lt;br /&gt;
&lt;br /&gt;
Questions about how to maintain olfactory sensitivity under the observed model are raised, and some theoretical explanations are proposed that involve synthesis across many neurons, but without related experiment. &lt;br /&gt;
&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
This experiment aimed to probe the relation between responses of frog olfactory receptors to odor stimuli, and the intensity and duration of those stimuli.  Working from knowledge of the specific proteins and cation channels involved in olfactory reception, the authors set out to develop a technique to stimulate isolated olfactory neurons of a frog, in Ringer solution (to stimulate a physical environment), while measuring resulting membrane currents.  &lt;br /&gt;
&lt;br /&gt;
This method assumed that there was some smallest quantum of response to odor detection, and that any observed response was some combination of these elementary (or 'unitary') units of response.  This followed quantal analysis originally developed by Castillo and Katz in 1954.  To do this required avoiding olfactory adaptation - cells were known to have a non-linear dose-response relation in the presence of external Ca2+, which leads to such adaptation.  So the experiment minimized this concentration, while confirming its impact on the results by repeating its tests in solutions with different concentrations of Ca2+ (replaced in low-Ca solutions with Mg2+) : tests were run with cells in regular Ringer solution, 20μM Ca2+, and 100nM Ca2+ solution.&lt;br /&gt;
&lt;br /&gt;
Two odorants that ORNs were known to resopnd to very differently (acetophenone and cineole) were used to get a sense of response variation across different regimes of odorant binding and saturation.  the dwell-time of the two odorants different by roughly a magnitude.  The results were analyzed to see how long the receptor-odorant complexes lasted, and what could be understood about the activation of G proteins during the process.  This was compared to the better known process of rhodopsin amplification cascade in which photoisomerized rhodopsin triggers a cascade of transducins before being shutoff by phosphorylation.&lt;br /&gt;
&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
&lt;br /&gt;
The unitary current stimulated by each and the overall response kinetics were similar for both odorants across five different cells.  This unit of response varied primarily with the concentration of Ca2+ in the solutino, and was consistent across different cells, though it is expected that every cell has different binding receptor.  &lt;br /&gt;
&lt;br /&gt;
A simple check for whether a quantal / unitary response is detected is the linearity of the relationship between concentration and response.  If many different binding events start to overlap spatially, transduction effects would not be linear, so the observed response would be supralinear.  And indeed in low-Ca2+ environments a linear response was seen, at both 100nM and 20μM Ca2+, up to a certain odorant concentration.  Concentration was varied both by using increasingly long pulses of low concentration, and by using increasingly intense pulses of fixed concentration odors, with similar results.&lt;br /&gt;
&lt;br /&gt;
The response was analyzed for possible amplification cascades involved in converting those stimuli to signals from GTP-binding [G] proteins.  The dwell-time of odorants was found to be quite small, under 1ms.  Moreover the response time to odors was fast and steady: the linear increase in total response to a pulse of fixed molarity but different duration had a projected time-intercept of 0, indicating that some response was taking place very soon after the odor was released.&lt;br /&gt;
&lt;br /&gt;
Each bound odorant seemed to have a low probability of activating a single G protein, which in turn has a low probability of activating more than one adenylyl cyclase molecule.  This is projected from the overall linearity of response across a wide range of odor saturations.  Even when all receptors were expected to be bound to cineole, the highly effective odorant, the total response amplitude continued to increase linearly with pulse duration.  &lt;br /&gt;
&lt;br /&gt;
These results were compared to known response patterns of optical neurons to light at low levels of stimulation.  In contrast, rod phototransduction acts through photoisomerized rhodopsin activating a transducin cascade.  This experiment suggests that such a mechanism may not exist for olfaction, and that the odorant-receptor complexes may generally be too short lived to trigger any mechanisms that might exist.  Moreover, each receptor, once activated, did not seem to be inactivated for at least 100ms.&lt;br /&gt;
&lt;br /&gt;
Some further understanding of the workings of receptors once they bind to an odorant are needed.  The authors suggest that they may integrate responses when an odorant binds to them repeatedly without being phosphorylated.  Moreover, the glomerulus in the olfactory bulb of the frog can integrate signals from all ORNs, perhaps separately integrating them for each receptor.&lt;br /&gt;
&lt;br /&gt;
Unlike with photons, each odorant can go on to bind many times at the same site or at different sites.   And unlike with an eye of fixed size, which is difficult to modify within the structure of its host, the surface area of olfactory epithelium can readily be expanded.  This could have a proportional improvement in olfactory sensitivity.&lt;br /&gt;
&lt;br /&gt;
 &lt;br /&gt;
== References ==&lt;br /&gt;
* Measurement process:  [[Quantal Components of the End-Plate Potential]]. Castillo and Katz, [http://jp.physoc.org/content/124/3/560.full.pdf+html?ijkey=6ff0ca7eede96a5d444b7154dd088b836af7997f&amp;amp;keytype2=tf_ipsecsha Journal of Physiology] (1954)&lt;br /&gt;
* S. J. Kleene, Neuroscience 66, 1001 (1995)&lt;br /&gt;
|relevance=This is a study of low-level components of one olfactory system that suggest the sorts of sensory models which may be studied in further experiments.  It provides a benchmark for similar work in other animals and at other levels in the frog.&lt;br /&gt;
|journal=Science&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=10.1126/science.1109886&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8885</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8885"/>
		<updated>2012-12-15T01:30:16Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA, USA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein; I try to keep [[user:Benjamin Mako Hill|Mako]]'s article updates in check.&lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
{| style=&amp;quot;font-size:100%;&amp;quot; width=&amp;quot;100%&amp;quot; cellpadding=0 cellspacing=0&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work]]&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]]&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
|} &lt;br /&gt;
{| style=&amp;quot;font-size:80%;&amp;quot; width=&amp;quot;100%&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;38%&amp;quot;|&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
|width=&amp;quot;4%&amp;quot;| &amp;amp;nbsp;&lt;br /&gt;
|valign=&amp;quot;top&amp;quot; width=&amp;quot;58%&amp;quot;|&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
|}&lt;br /&gt;
&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8884</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8884"/>
		<updated>2012-12-15T01:24:00Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA, USA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein; I try to keep [[user:Benjamin Mako Hill|Mako]]'s article updates in check.&lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work]]&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]]&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8883</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8883"/>
		<updated>2012-12-15T01:23:35Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein; I try to keep Mako's article updates in check.&lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work]]&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]]&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8882</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8882"/>
		<updated>2012-12-15T01:23:08Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein; you can find me most easily on [[user:sj|Wikipedia]].  I try to keep Mako's article updates in check...&lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work]]&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants]]&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User:Sj&amp;diff=8881</id>
		<title>User:Sj</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User:Sj&amp;diff=8881"/>
		<updated>2012-12-15T01:22:51Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{User&lt;br /&gt;
|name=Sam Klein&lt;br /&gt;
|location=Harvard, Cambridge, MA&lt;br /&gt;
}}&lt;br /&gt;
I'm Sam Klein; you can find me most easily on [[user:sj|Wikipedia]].  I try to keep Mako's article updates in check...&lt;br /&gt;
&lt;br /&gt;
Papers I'm reading currently:&lt;br /&gt;
* [[Energy, Quanta, and Vision]]&lt;br /&gt;
* [[How the ear's works work&lt;br /&gt;
* [[Elementary Response of Olfactory Receptor Neurons to Odorants&lt;br /&gt;
* [[Deﬁning the Computational Structure of the Motion Detector in Drosophila]]&lt;br /&gt;
&lt;br /&gt;
* [[Segregation of object and background motion in the retina]]&lt;br /&gt;
* [[Motility-associated hair-bundle motion in mammalian outer hair cells]]‎&lt;br /&gt;
* [[Forces between clustered stereocilia minimize friction in the ear on a subnanometre scale]]&lt;br /&gt;
* [[Mechanisms Regulating Variability of the Single Photon Responses of Mammalian Rod Photoreceptors]]&lt;br /&gt;
* [[Selective Transmission of Single Photon Responses by Saturation at the Rod-to-Rod Bipolar Synapse]]&lt;br /&gt;
&lt;br /&gt;
* [[Essential Nonlinearities in Hearing]] &lt;br /&gt;
* [[Unitary response of mouse olfactory receptor neurons]]&lt;br /&gt;
* [[Internal Structure of the Fly Elementary Motion Detector]]&lt;br /&gt;
* [[Odor Representations in Olfactory Cortex: Distributed Rate Coding and Decorrelated Population Activity]]‎&lt;br /&gt;
* [[Fly motion vision is based on Reichardt detectors regardless of the signal-to-noise ratio]]&lt;br /&gt;
&lt;br /&gt;
Interested in:&lt;br /&gt;
* [[Material Selection for Direct Posterior Restoratives]]&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=User_talk:Mike_Linksvayer&amp;diff=8880</id>
		<title>User talk:Mike Linksvayer</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=User_talk:Mike_Linksvayer&amp;diff=8880"/>
		<updated>2012-12-15T01:17:55Z</updated>

		<summary type="html">&lt;p&gt;Sj: /* Summaries wanted */ new section&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Thanks, Mike, for all your contributions to the site--online and off! [[User:Jodi.a.schneider|Jodi.a.schneider]] 00:25, 7 October 2009 (UTC)&lt;br /&gt;
&lt;br /&gt;
== Summaries wanted ==&lt;br /&gt;
&lt;br /&gt;
That's such a brilliant aspect of AcaWiki that it should be its own siebar link with a dedicated form/template/extension written to make it simple to use. &lt;br /&gt;
&lt;br /&gt;
This is something we could easily ask everyone to fill ou - a few quick requests for summaries; with and without bounties.  The bounties could be fun things like &amp;quot;I will find and upload X in exchange&amp;quot; (where X could be summaries of great PD or free papers, to be thematic), or donations to an AcaWiki fund, or amazon giftcards...  [[User:Sj|Sj]] 02:17, 15 December 2012 (CET)&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8878</id>
		<title>Energy, Quanta, and Vision</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Energy,_Quanta,_and_Vision&amp;diff=8878"/>
		<updated>2012-12-14T22:30:10Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Energy, Quanta, and Vision&lt;br /&gt;
|authors=Selig Hecht, Simon Shlaer, Maurice Henri Pirenne&lt;br /&gt;
|tags=vision quanta light eye&lt;br /&gt;
|summary=This paper has become a canonical reference for any discussion about how sensitive the human eye is to individual quanta of light.  While it was not the first to ask the question and carry out experiments to measure how small a signal was needed to stimulate the eye, it used a simple and universal technique, was careful in its error analysis, and compared its work cleanly with those of past attempts to measure the visual threshold.  Previous estimates of the visual threshhold were on the order of 20 quanta of light; this work used statistical analysis to reduce that to 5-7.  &lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
--&amp;gt;&lt;br /&gt;
|relevance=This was a standard reference for human visual threshold analysis for decades, and the new statistical technique they used changed how future experiments would be analysed.&lt;br /&gt;
|journal=The Journal of General Physiology&lt;br /&gt;
|pub_date=1942&lt;br /&gt;
|subject=Biology&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8877</id>
		<title>Motility-associated hair-bundle motion in mammalian outer hair cells</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8877"/>
		<updated>2012-12-14T21:48:27Z</updated>

		<summary type="html">&lt;p&gt;Sj: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Motility-associated hair-bundle motion in mammalian outer hair cells&lt;br /&gt;
|authors=Shuping Jia, David Z Z He&lt;br /&gt;
|url=http://courses.washington.edu/pbio525/Paper%20PDFs/Jia%202006%20Nat%20Neuro.pdf&lt;br /&gt;
|tags=hearing, cochlea, somatic motility&lt;br /&gt;
|summary=&amp;lt;!--&lt;br /&gt;
Mammalian hearing owes its remarkable sensitivity and frequency selectivity to a local mechanical feedback process within the&lt;br /&gt;
cochlea. Cochlear outer hair cells (OHCs) function as the key elements in the feedback loop in which the fast somatic motility of&lt;br /&gt;
OHCs is thought to be the source of cochlear ampliﬁcation. An alternative view is that ampliﬁcation arises from active hair-bundle&lt;br /&gt;
movement, similar to that seen in nonmammalian hair cells. We measured voltage-evoked hair-bundle motions in the gerbil&lt;br /&gt;
cochlea to determine if such movements were also present in mammalian OHCs. The OHCs showed bundle movement with peak&lt;br /&gt;
responses of up to 830 nm. The movement was insensitive to manipulations that would normally block mechanotransduction in&lt;br /&gt;
the stereocilia, and it was absent in neonatal OHCs and prestin-knockout OHCs. These ﬁndings suggest that the bundle movement&lt;br /&gt;
originated in somatic motility and that somatic motility has a central role in cochlear ampliﬁcation in mammals.&lt;br /&gt;
--&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
--&amp;gt;&lt;br /&gt;
|relevance=This study distinguishes between two potential sources of hair-bundle motion: the reclosing of mechanotransduction channels and somatic electromotility.  Previous analyses had mainly demonstrated the possibility of either (including the possible presence of mechanotransduction-driven motion in IHCs of gerbils). &lt;br /&gt;
&lt;br /&gt;
It demonstrate conclusively that such motion is due predominantly to electromotility in the OHCs of some gerbils and mice.  It also suggests ways in which this motion in OHCs might excite IHCs and stimulate observed motion there as well, including possibly the observed motion of gerbil IHCs, which would make electromotility the primary mechanism for cochlear amplification in mammals.  This indicates  avenues for future research.&lt;br /&gt;
|journal=Nature Neuroscience&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=doi:10.1038/nn1509&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8876</id>
		<title>Motility-associated hair-bundle motion in mammalian outer hair cells</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Motility-associated_hair-bundle_motion_in_mammalian_outer_hair_cells&amp;diff=8876"/>
		<updated>2012-12-14T21:14:38Z</updated>

		<summary type="html">&lt;p&gt;Sj: Created page with &amp;quot;{{Summary |title=Motility-associated hair-bundle motion in mammalian outer hair cells |authors=Shuping Jia, David Z Z He |url=http://courses.washington.edu/pbio525/Paper%20PDFs/J...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Motility-associated hair-bundle motion in mammalian outer hair cells&lt;br /&gt;
|authors=Shuping Jia, David Z Z He&lt;br /&gt;
|url=http://courses.washington.edu/pbio525/Paper%20PDFs/Jia%202006%20Nat%20Neuro.pdf&lt;br /&gt;
|tags=hearing, cochlea, somatic motility&lt;br /&gt;
|summary=&amp;lt;!--&lt;br /&gt;
Mammalian hearing owes its remarkable sensitivity and frequency selectivity to a local mechanical feedback process within the&lt;br /&gt;
cochlea. Cochlear outer hair cells (OHCs) function as the key elements in the feedback loop in which the fast somatic motility of&lt;br /&gt;
OHCs is thought to be the source of cochlear ampliﬁcation. An alternative view is that ampliﬁcation arises from active hair-bundle&lt;br /&gt;
movement, similar to that seen in nonmammalian hair cells. We measured voltage-evoked hair-bundle motions in the gerbil&lt;br /&gt;
cochlea to determine if such movements were also present in mammalian OHCs. The OHCs showed bundle movement with peak&lt;br /&gt;
responses of up to 830 nm. The movement was insensitive to manipulations that would normally block mechanotransduction in&lt;br /&gt;
the stereocilia, and it was absent in neonatal OHCs and prestin-knockout OHCs. These ﬁndings suggest that the bundle movement&lt;br /&gt;
originated in somatic motility and that somatic motility has a central role in cochlear ampliﬁcation in mammals.&lt;br /&gt;
--&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
--&amp;gt;&lt;br /&gt;
|journal=Nature Neuroscience&lt;br /&gt;
|pub_date=2005/06/24&lt;br /&gt;
|doi=doi:10.1038/nn1509&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
	<entry>
		<id>https://acawiki.org/index.php?title=Segregation_of_object_and_background_motion_in_the_retina&amp;diff=8875</id>
		<title>Segregation of object and background motion in the retina</title>
		<link rel="alternate" type="text/html" href="https://acawiki.org/index.php?title=Segregation_of_object_and_background_motion_in_the_retina&amp;diff=8875"/>
		<updated>2012-12-14T21:10:03Z</updated>

		<summary type="html">&lt;p&gt;Sj: Created page with &amp;quot;{{Summary |title=Segregation of object and background motion in the retina |authors=Bence P. Ölveczky, Stephen A. Baccus, Markus Meister |url=http://www.oeb.harvard.edu/faculty/...&amp;quot;&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;{{Summary&lt;br /&gt;
|title=Segregation of object and background motion in the retina&lt;br /&gt;
|authors=Bence P. Ölveczky, Stephen A. Baccus, Markus Meister&lt;br /&gt;
|url=http://www.oeb.harvard.edu/faculty/olveczky/docs/Nature.pdf&lt;br /&gt;
|tags=vision, retina, background, object discrimination&lt;br /&gt;
|summary=&amp;lt;!--&lt;br /&gt;
An important task in vision is to detect objects moving within a stationary scene. During normal viewing this is complicated&lt;br /&gt;
by the presence of eye movements that continually scan the image across the retina, even during ﬁxation. To detect moving&lt;br /&gt;
objects, the brain must distinguish local motion within the scene from the global retinal image drift due to ﬁxational eye&lt;br /&gt;
movements. We have found that this process begins in the retina: a subset of retinal ganglion cells responds to motion in the&lt;br /&gt;
receptive ﬁeld centre, but only if the wider surround moves with a different trajectory. This selectivity for differential motion is&lt;br /&gt;
independent of direction, and can be explained by a model of retinal circuitry that invokes pooling over nonlinear interneurons. The&lt;br /&gt;
suppression by global image motion is probably mediated by polyaxonal, wide-ﬁeld amacrine cells with transient responses. We&lt;br /&gt;
show how a population of ganglion cells selective for differential motion can rapidly ﬂag moving objects, and even segregate&lt;br /&gt;
multiple moving objects.&lt;br /&gt;
--&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--&lt;br /&gt;
== Goals and Methods ==&lt;br /&gt;
== Results and Analysis ==&lt;br /&gt;
--&amp;gt;&lt;br /&gt;
|relevance=This analysis suggests that many species have cells that are specially sensitive to object motion, related to those known to carry out nonlinear spatial summation.  It presents an analysis that could be carried out in a variety of other settings to probe motion tracking and object-background distinction.&lt;br /&gt;
|journal=Nature&lt;br /&gt;
|pub_date=2003/05/22&lt;br /&gt;
|doi=10.1038/nature01652&lt;br /&gt;
|subject=Neuroscience&lt;br /&gt;
}}&lt;/div&gt;</summary>
		<author><name>Sj</name></author>
		
	</entry>
</feed>