Motion sensitivity in the nucleus of the basal optic root of the pigeon
F. Wolf-Oberhollenzer and K. Kirschfeld Max-Planck-Institut fur Biologische Kybernetik, Tubingen, Germany. 1. Single-unit responses to large-field movement (angular velocity, w = 0.25-42 degrees/s) of sine-wave gratings of different spatial wavelength (lambda = 5.2-41 degrees) and contrast have been...
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Veröffentlicht in: | Journal of neurophysiology 1994-04, Vol.71 (4), p.1559-1573 |
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creator | Wolf-Oberhollenzer, F Kirschfeld, K |
description | F. Wolf-Oberhollenzer and K. Kirschfeld
Max-Planck-Institut fur Biologische Kybernetik, Tubingen, Germany.
1. Single-unit responses to large-field movement (angular velocity, w =
0.25-42 degrees/s) of sine-wave gratings of different spatial wavelength
(lambda = 5.2-41 degrees) and contrast have been recorded in the nucleus of
the basal optic root (nBOR) of the accessory optic system (AOS) of the
pigeon. 2. The steady-state response to moving sine-wave gratings increases
with increasing contrast to reach a saturation level at 25%. 3. Generally
the steady-state responses of the cells passed through a maximum when
stimulated at various velocities. In 12 of the 15 cells tested with six
different velocities and four different spatial wavelengths, the location
of the response maximum on the velocity scale depended on the spatial
wavelength (lambda) used. That is, in these cells the response depends on
the temporal frequency (tf = w/lambda) of the stimulus and not on its
velocity alone. This is in agreement with the prediction of the theory of
motion detection according to the basic version of the correlation scheme.
4. The temporal frequency for maximal response of individual cells shifts
to higher values when the contrast of the sine-wave gratings is reduced to
5%. 5. The steady-state response of 16 of the recorded directional
selective cells (53) is modulated with the temporal frequency of the
stimulus, regardless of the phase of the grating at the beginning of its
movement. 6. In phasic-tonically responding cells, the phasic response peak
decays to the steady-state level with a time constant that becomes shorter
as the temporal frequency of the stimulus increases. 7. The basic version
of the correlation scheme includes only the time constant of one low-pass
filter. Therefore the phasic response is expected to decay to the
steady-state level with one and the same time constant, and the position of
the maximal response on the temporal frequency scale should not be
influenced by a change of pattern contrast. According to the model,
phase-dependent modulations of the steady-state response should occur only
when the spatial wavelength of the stimulus pattern is large compared with
the sampling base of the underlying detector. Consequently the results
given in points 4-6 cannot be described by a basic version of the
correlation scheme. |
doi_str_mv | 10.1152/jn.1994.71.4.1559 |
format | Article |
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Max-Planck-Institut fur Biologische Kybernetik, Tubingen, Germany.
1. Single-unit responses to large-field movement (angular velocity, w =
0.25-42 degrees/s) of sine-wave gratings of different spatial wavelength
(lambda = 5.2-41 degrees) and contrast have been recorded in the nucleus of
the basal optic root (nBOR) of the accessory optic system (AOS) of the
pigeon. 2. The steady-state response to moving sine-wave gratings increases
with increasing contrast to reach a saturation level at 25%. 3. Generally
the steady-state responses of the cells passed through a maximum when
stimulated at various velocities. In 12 of the 15 cells tested with six
different velocities and four different spatial wavelengths, the location
of the response maximum on the velocity scale depended on the spatial
wavelength (lambda) used. That is, in these cells the response depends on
the temporal frequency (tf = w/lambda) of the stimulus and not on its
velocity alone. This is in agreement with the prediction of the theory of
motion detection according to the basic version of the correlation scheme.
4. The temporal frequency for maximal response of individual cells shifts
to higher values when the contrast of the sine-wave gratings is reduced to
5%. 5. The steady-state response of 16 of the recorded directional
selective cells (53) is modulated with the temporal frequency of the
stimulus, regardless of the phase of the grating at the beginning of its
movement. 6. In phasic-tonically responding cells, the phasic response peak
decays to the steady-state level with a time constant that becomes shorter
as the temporal frequency of the stimulus increases. 7. The basic version
of the correlation scheme includes only the time constant of one low-pass
filter. Therefore the phasic response is expected to decay to the
steady-state level with one and the same time constant, and the position of
the maximal response on the temporal frequency scale should not be
influenced by a change of pattern contrast. According to the model,
phase-dependent modulations of the steady-state response should occur only
when the spatial wavelength of the stimulus pattern is large compared with
the sampling base of the underlying detector. Consequently the results
given in points 4-6 cannot be described by a basic version of the
correlation scheme.</description><identifier>ISSN: 0022-3077</identifier><identifier>EISSN: 1522-1598</identifier><identifier>DOI: 10.1152/jn.1994.71.4.1559</identifier><identifier>PMID: 8035235</identifier><language>eng</language><publisher>United States: Am Phys Soc</publisher><subject>Acceleration ; Algorithms ; Animals ; Aves ; Brain Mapping ; Columbidae - physiology ; Contrast Sensitivity - physiology ; Evoked Potentials, Visual - physiology ; Female ; Male ; Motion Perception - physiology ; Neurons - physiology ; Optic Nerve - physiology ; Orientation - physiology ; Pattern Recognition, Visual - physiology ; Photoreceptor Cells - physiology ; Space life sciences ; Visual Pathways - physiology</subject><ispartof>Journal of neurophysiology, 1994-04, Vol.71 (4), p.1559-1573</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c359t-3ddc91d98a42fbd2bbd1317994288c5a1d587016e53d455a60da9458ece699fb3</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/8035235$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Wolf-Oberhollenzer, F</creatorcontrib><creatorcontrib>Kirschfeld, K</creatorcontrib><title>Motion sensitivity in the nucleus of the basal optic root of the pigeon</title><title>Journal of neurophysiology</title><addtitle>J Neurophysiol</addtitle><description>F. Wolf-Oberhollenzer and K. Kirschfeld
Max-Planck-Institut fur Biologische Kybernetik, Tubingen, Germany.
1. Single-unit responses to large-field movement (angular velocity, w =
0.25-42 degrees/s) of sine-wave gratings of different spatial wavelength
(lambda = 5.2-41 degrees) and contrast have been recorded in the nucleus of
the basal optic root (nBOR) of the accessory optic system (AOS) of the
pigeon. 2. The steady-state response to moving sine-wave gratings increases
with increasing contrast to reach a saturation level at 25%. 3. Generally
the steady-state responses of the cells passed through a maximum when
stimulated at various velocities. In 12 of the 15 cells tested with six
different velocities and four different spatial wavelengths, the location
of the response maximum on the velocity scale depended on the spatial
wavelength (lambda) used. That is, in these cells the response depends on
the temporal frequency (tf = w/lambda) of the stimulus and not on its
velocity alone. This is in agreement with the prediction of the theory of
motion detection according to the basic version of the correlation scheme.
4. The temporal frequency for maximal response of individual cells shifts
to higher values when the contrast of the sine-wave gratings is reduced to
5%. 5. The steady-state response of 16 of the recorded directional
selective cells (53) is modulated with the temporal frequency of the
stimulus, regardless of the phase of the grating at the beginning of its
movement. 6. In phasic-tonically responding cells, the phasic response peak
decays to the steady-state level with a time constant that becomes shorter
as the temporal frequency of the stimulus increases. 7. The basic version
of the correlation scheme includes only the time constant of one low-pass
filter. Therefore the phasic response is expected to decay to the
steady-state level with one and the same time constant, and the position of
the maximal response on the temporal frequency scale should not be
influenced by a change of pattern contrast. According to the model,
phase-dependent modulations of the steady-state response should occur only
when the spatial wavelength of the stimulus pattern is large compared with
the sampling base of the underlying detector. Consequently the results
given in points 4-6 cannot be described by a basic version of the
correlation scheme.</description><subject>Acceleration</subject><subject>Algorithms</subject><subject>Animals</subject><subject>Aves</subject><subject>Brain Mapping</subject><subject>Columbidae - physiology</subject><subject>Contrast Sensitivity - physiology</subject><subject>Evoked Potentials, Visual - physiology</subject><subject>Female</subject><subject>Male</subject><subject>Motion Perception - physiology</subject><subject>Neurons - physiology</subject><subject>Optic Nerve - physiology</subject><subject>Orientation - physiology</subject><subject>Pattern Recognition, Visual - physiology</subject><subject>Photoreceptor Cells - physiology</subject><subject>Space life sciences</subject><subject>Visual Pathways - physiology</subject><issn>0022-3077</issn><issn>1522-1598</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1994</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNqFUE1PhDAQbYxmXVd_gAcTTnoCO8BAezQbXU3WeNFzU2hZumEpUtDw7wV31aOnmXlfyTxCLoEGABjebusAOI-DFII4AER-ROYjHvqAnB2TOaXjHtE0PSVnzm0ppSnScEZmjEYYRjgnq2fbGVt7TtfOdObDdINnaq8rtVf3eaV759ni-8ykk5Vnm87kXmtt94M3ZqNtfU5OClk5fXGYC_L2cP-6fPTXL6un5d3azyPknR8plXNQnMk4LDIVZpmCCNLxh5CxHCUoZCmFRGOkYkSZUCV5jEznOuG8yKIFud7nNq1977XrxM64XFeVrLXtnUgT5CFD_q8QEpYABRyFsBfmrXWu1YVoWrOT7SCAiqllsa3F1LJIQcRiann0XB3C-2yn1a_jUOvI3-z50mzKT9Nq0ZSDM7aym2GK-0v6ArlahaY</recordid><startdate>19940401</startdate><enddate>19940401</enddate><creator>Wolf-Oberhollenzer, F</creator><creator>Kirschfeld, K</creator><general>Am Phys Soc</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TK</scope><scope>7X8</scope></search><sort><creationdate>19940401</creationdate><title>Motion sensitivity in the nucleus of the basal optic root of the pigeon</title><author>Wolf-Oberhollenzer, F ; Kirschfeld, K</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c359t-3ddc91d98a42fbd2bbd1317994288c5a1d587016e53d455a60da9458ece699fb3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1994</creationdate><topic>Acceleration</topic><topic>Algorithms</topic><topic>Animals</topic><topic>Aves</topic><topic>Brain Mapping</topic><topic>Columbidae - physiology</topic><topic>Contrast Sensitivity - physiology</topic><topic>Evoked Potentials, Visual - physiology</topic><topic>Female</topic><topic>Male</topic><topic>Motion Perception - physiology</topic><topic>Neurons - physiology</topic><topic>Optic Nerve - physiology</topic><topic>Orientation - physiology</topic><topic>Pattern Recognition, Visual - physiology</topic><topic>Photoreceptor Cells - physiology</topic><topic>Space life sciences</topic><topic>Visual Pathways - physiology</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Wolf-Oberhollenzer, F</creatorcontrib><creatorcontrib>Kirschfeld, K</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>Neurosciences Abstracts</collection><collection>MEDLINE - Academic</collection><jtitle>Journal of neurophysiology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Wolf-Oberhollenzer, F</au><au>Kirschfeld, K</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Motion sensitivity in the nucleus of the basal optic root of the pigeon</atitle><jtitle>Journal of neurophysiology</jtitle><addtitle>J Neurophysiol</addtitle><date>1994-04-01</date><risdate>1994</risdate><volume>71</volume><issue>4</issue><spage>1559</spage><epage>1573</epage><pages>1559-1573</pages><issn>0022-3077</issn><eissn>1522-1598</eissn><abstract>F. Wolf-Oberhollenzer and K. Kirschfeld
Max-Planck-Institut fur Biologische Kybernetik, Tubingen, Germany.
1. Single-unit responses to large-field movement (angular velocity, w =
0.25-42 degrees/s) of sine-wave gratings of different spatial wavelength
(lambda = 5.2-41 degrees) and contrast have been recorded in the nucleus of
the basal optic root (nBOR) of the accessory optic system (AOS) of the
pigeon. 2. The steady-state response to moving sine-wave gratings increases
with increasing contrast to reach a saturation level at 25%. 3. Generally
the steady-state responses of the cells passed through a maximum when
stimulated at various velocities. In 12 of the 15 cells tested with six
different velocities and four different spatial wavelengths, the location
of the response maximum on the velocity scale depended on the spatial
wavelength (lambda) used. That is, in these cells the response depends on
the temporal frequency (tf = w/lambda) of the stimulus and not on its
velocity alone. This is in agreement with the prediction of the theory of
motion detection according to the basic version of the correlation scheme.
4. The temporal frequency for maximal response of individual cells shifts
to higher values when the contrast of the sine-wave gratings is reduced to
5%. 5. The steady-state response of 16 of the recorded directional
selective cells (53) is modulated with the temporal frequency of the
stimulus, regardless of the phase of the grating at the beginning of its
movement. 6. In phasic-tonically responding cells, the phasic response peak
decays to the steady-state level with a time constant that becomes shorter
as the temporal frequency of the stimulus increases. 7. The basic version
of the correlation scheme includes only the time constant of one low-pass
filter. Therefore the phasic response is expected to decay to the
steady-state level with one and the same time constant, and the position of
the maximal response on the temporal frequency scale should not be
influenced by a change of pattern contrast. According to the model,
phase-dependent modulations of the steady-state response should occur only
when the spatial wavelength of the stimulus pattern is large compared with
the sampling base of the underlying detector. Consequently the results
given in points 4-6 cannot be described by a basic version of the
correlation scheme.</abstract><cop>United States</cop><pub>Am Phys Soc</pub><pmid>8035235</pmid><doi>10.1152/jn.1994.71.4.1559</doi><tpages>15</tpages></addata></record> |
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subjects | Acceleration Algorithms Animals Aves Brain Mapping Columbidae - physiology Contrast Sensitivity - physiology Evoked Potentials, Visual - physiology Female Male Motion Perception - physiology Neurons - physiology Optic Nerve - physiology Orientation - physiology Pattern Recognition, Visual - physiology Photoreceptor Cells - physiology Space life sciences Visual Pathways - physiology |
title | Motion sensitivity in the nucleus of the basal optic root of the pigeon |
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