{"title": "Stimulus Encoding by Multidimensional Receptive Fields in Single Cells and Cell Populations in V1 of Awake Monkey", "book": "Advances in Neural Information Processing Systems", "page_first": 377, "page_last": 384, "abstract": null, "full_text": "STIMULUS ENCODING BY \n\nMUL TIDIMENSIONAL RECEPTIVE FIELDS \nIN SINGLE CELLS AND CELL POPULATIONS \n\nIN VI OF A WAKE MONKEY \n\nEdward  Stern \n\nCenter for  Neural Computation \nand Department of Neurobiology \n\nLife Sciences Institute \nHebrew University \nJerusalem, Israel \n\nEilon  Vaadia \n\nCenter for Neural Computation \n\nand Physiology Department \nHadassah Medical School \n\nHebrew University \nJerusalem,  Israel \n\nABSTRACT \n\nAd  Aertsen \n\nInstitut fur  Neuroinfonnatik \nRuhr-Universitat-Bochum \n\nBochum, Gennany \n\nShaul  Hochstein \n\nCenter for  Neural Computation \nand Department of Neurobiology, \n\nLife Sciences Institute \nHebrew University \nJerusalem, Israel \n\nin \n\ntemporal \n\nshowed  different \n\nMultiple  single  neuron  responses  were  recorded \nfrom  a  single  electrode  in  VI  of  alert,  behaving \nmonkeys.  Drifting  sinusoidal  gratings  were \npresented \nthe  cells'  overlapping  receptive \nfields,  and  the  stimulus  was  varied  along  several \nvisual  dimensions.  The  degree  of  dimensional \nseparability  was  calculated  for  a  large  population \nof  neurons,  and  found  to  be  a  continuum.  Several \ncells \nresponse \ndependencies  to  variation  of  different  stimulus \ndimensions, \ntuning  of  the  modulated \nfiring  was  not  necessarily  the  same  as  that  of  the \nmean  firing  rate.  We  describe  a  multidimensional \nreceptive  field,  and  use  simultaneously  recorded \nresponses  to  compute  a  multi-neuron  receptive \nfield,  describing \ninformation  processing \ncapabilities  of  a  group  of  cells.  Using  dynamic \ncorrelation \nseveral \nfor  multidimensional \ncomputational  schemes \nspatiotemporal  tuning  for  groups  of  cells.  The \nimplications  for  neuronal  coding  of  stimuli  are \ndiscussed. \n\nanalysis,  we  propose \n\ni.e. \n\nthe \n\nthe \n\n377 \n\n\f378 \n\nStern, Aensen, Vaadia,  and  Hochstein \n\nINTRODUCTION \n\nThe  receptive  field  is  perhaps  the  most  useful  concept  for  understanding  neuronal \ninformation  processing. The  ideal  definition  of the  receptive  field  is  that set of stimuli \nwhich  cause  a  change  in  the  neuron's  firing  properties.  However, as  with  many  such \nconcepts, the use of the receptive field  in describing the behavior of sensory neurons  falls \nshort of the  ideal.  The classical  method  for  describing  the  receptive  field  has  been  to \nmeasure the  \"tuning curve\"  i.e.  the response of the  neuron  as a  function  of the  value of \none  dimension  of the  stimulus.  This  presents a  problem  because  the  sensory  world  is \nmultidimensional;  For  example,  even  a  simple  visual  stimulus,  such  as  a  patch  of a \nsinusoidal  grating,  may  vary  in  location,  orientation,  spatial  frequency,  temporal \nfrequency,  movement direction and speed, phase, contrast, color, etc. Does  the tuning to \none dimension remain constant when other dimensions are  varied? i.e. are the dimensions \nlinearly separable?  It is not unreasonable to expect inseparability:  Consider an oriented, \nspatially discrete receptive  field.  The excitation generated by passing a bar  through  the \nreceptive field will of course change  with orientation. However, the shape of this  tuning \ncurve will  depend upon the bar width, related  to the spatial frequency. This effect has not \nbeen  studied quantitatively,  however.  If  interactions  among  dimensions exist, do  they \naccount for a  large portion of the cell's response variance?  Are there discrete populations \nof cells, with  some  cells showing interactions among dimensions and  others not? These \nquestion have  clear implications  for the problem of neural coding. \n\nRelated to the question of dimensional  separability is  that of stimulus encoding:  Given \nthat  the  receptive  field  is  multidimensional  in  nature,  how  can  the  cell  maximize  the \namount  of stimulus  information  it encodes?  Does  the  neuron  use  a  single  code  to \nrepresent  all  the  stimulus  dimensions?  It is  possible  that  interactions  lead  to  greater \nuncertainty  in  stimulus  identification.  Does  the small  number of visual  cortical cells \nencode all  the  possible combinations of stimuli  using only spike rate  as the dependent \nvariable?  We  present  data  indicating  that  more  information  is  indeed  present  in  the \nneuronal response, and propose a new approach for  its utilization. \n\nThe final  problem  that we address is  the following:  Clearly, many cells participate in  the \nstimulus encoding  process.  Arriving at a  valid  concept of a  multidimensional receptive \nfield,  can  we  generalize  this  concept  to  more  than  one cell  introducing  the  notion  of a \nmulti-cellular receptive field? \n\nMETHODS \n\nDrifting sinusoidal gratings were presented for  500 msec to the central  10 degrees of the \nvisual  field  of  monkeys  performing  a  fixation  task.  The  gratings  were  varied  in \norientation, spatial frequency,temporal  frequency,  and movement direction.  We recorded \nfrom  up to  3 cells simultaneously  with a single electrode in  the monkey's primary  visual \ncortex  (VI).  The  cells described  in  this  study  were  well  separated,  using  a  template(cid:173)\nmatching  procedure.  The  responses of the  neurons  were  plotted  as  Peri-Stimulus Time \nHistograms (PSTHs) and  their parameters quantified (Abeles,  1982), and offline Fourier \nanalysis  and  time-dependent  crosscorrelation  analysis  (Aertsen  et  ai,  1989)  were \nperformed. \n\n\fStimulus Encoding by  Multidimensional Receptive  Fields  in Single Cells  and Cell  Populations \n\n379 \n\nRESULTS \n\nRecording  the  responses of visual  cortical  neurons  to stimuli  varied  over a  number of \ndimensions, we found  that in some cases, the tuning curve to one dimension depended on \nthe value of another dimension. Figure  lA shows the spatial-frequency tuning curve of a \nsingle  cell  measured  at  2  different stimulus  orientations.  When  the  orientation  of the \nstimulus is  72  degrees,  the  peak  response  is  at a spatial  frequency  of 4.5  cycles/degree \n(cpd), while at an orientation of216 degrees, the spatial frequency of peak response is 2.3 \ncpd.  If  the  responses  to  different  visual  dimensions  were  truly  linearly  separable,  the \ntuning  curve  to  any  single  dimension  would  have  the  same  shape  and,  in  particular, \nposition of peak, despite any  variations in  other dimensions. If the tuning curves are not \nparallel, then  interactions must exist between dimensions. Clearly,  this is an example of \na cell whose responses are  not linearly separable.  In order to quantify  the  inseparability \nphenomenon,  analyses  of variance  were  performed,  using  spike  rate  as  the  dependent \nvariable, and  the  visual  dimensions of the  stimuli as  the  independent variables. We then \nmeasured  the  amount  of  interaction  as  a  percentage  of  the total  between-conditions \n\nA. \nSpatial  Frequency \nTuning  Dependence  upon \nOrientation \n\nB.  Interaction effects between \nstimulus dimensions: \nPercentage or total variance \n\n30'.....-------------. \n\n25 \n\n<1)  0.9 \n~ 0.8 \nbO O.7 \ns:: \n'C  0.6 \nu:: \n\"0 0.5 \n~ 0.4 \nE 0.3 a 0.2 \n\ns::  0.1 \n\nO~--~~~~n---P-~~~ \n0.1 \n10 \n\n1 \n\nSpatial Frequency (cpd) \n\n!\u00a31I11~  1I11~  II \n\noooooo~ \n_ \n, \n\n- - - - - -\n\n~  \\I\"') \n, \n\"'\" \n\n1 \n1\"\"'11 \n\n% of non-residual variance \n\nN \nI \n_ \n\nf\"\"I \n' \nN \n\n110 \n, \n\nIt/') \n\n__  ORl=72  -6- ORl=216 \nnfac=45 \nnfac=34 \n\nFigure  1:  Dimensional  Inseparability  or Visual  Cortical Neurons.  A: \nAn example or dimensionsional inseparability in  the response or a single \ncell;  B:  Histogram  or dimensional  inseparability  as  a  percentage  or \n\ntotal response variance. \n\n\f380 \n\nStern,  Aertsen,  Vaadia,  and Hochstein \n\nvariance divided by the residuals. The resulting histogram for 69 cells is shown in Figure \nlB.  Although  there  are  several  cells  with  non-significant  interactions,  i.e.  linearly \nseparable  dimensions,  this  is  not  the  majority  of cells.  The  amount  of dimensional \ninseparability  seems  to  be  a continuum.  We  suggest  that  separability  is  a significant \nvariable in  the coding capability of the  neurons,  which  must be  taken  into account when \nmodeling the representation of sensory information by cortical neural networks. \n\nWe  found  that  the  time course of the  response was  not always constant, but  varied with \nstimulus parameters. Cortical cell  responses  may  have  components which  are sustained \n(constant  over  time),  transient  (with  a  peak  near  stimulus  onset  and/or  offset),  or \nmodulated (varying with  the stimulus period). For example, Figure 2 shows the responses \nof a single neuron  in  VI  to 50 stimuli, varying in orientation and spatial frequency.  Each \nresponse is plotted as a PSTH,  and  the stippled bar under the PSTH  indicates the time of \n\nOrientation \n\n-\n\nliM  !  f.ll  !!u  \u2022  D.I \n\nDD~DD \n4.5 D  [:j Eaij tJ D \nD~EJijjG5D \n23DG!5~GjD \nD~[MjE5E:5 \n1.5  G:J [;J CiIIJ ~ c:::J \nEj~~~E:::J \nO.8D~~~D \nDG5~tJD \n04oEJt5DCj \n\n!  U .. t  p.i  !  u .s  lI!.t  !  I.t J  I!.'  !  i.4 J \n\n11m.,  f  Iq  lip  \u2022  B.'  Ill.'  f  1.'1 \n\n.... t \n\nI  1.1 I  Ft.2 \n\n!  1.0 I  p.i \n\n:  u! \n\nII \u00b7' \n\n!  U \n\nI  flU  t  f.4  I  117.1  \u2022  f .1 I  11'\" \n\nFigure  2:  Spatial  Frequency/Orientation  Tuning  of  Responses \n\nof  VI  Cell \n\n\fStimulus Encoding by  Multidimensional Receptive  Fields in Single Cells  and Cell  Populations \n\n381 \n\nthe stimulus presentation (500 msec). The numbers beneath each PSTH are the firing rate \naveraged  over  the  response  time.  and  the  standard  deviations  of  the  response  over \nrepetitions of the stimulus (in  this case 40).  Clearly. the cell  is  orientation selective, and \nthe  neuronal  response  is  also  tuned  to  spatial  frequency.  The  stimulus  eliciting  the \nhighest  firing  rate  is  ORI=252  degrees;  SF=3.2  cycles/degree  (cpd).  However,  when \nlooking at the responses to lower spatial  frequencies,  we see a modulation  in  the PSTH. \nThe modulation,  when  present, has 2 peaks, corresponding to  the temporal  frequency of \nthe stimulus grating (4  cycles/second). Therefore, although the response rate of the cell is \nlower at low  spatial  frequencies  than  for other stimuli, the spike train  carries additional \ninformation about another stimulus dimension. \n\nIf the visual  neuron  is  considered as a  linear system, the predicted response  to a drifting \nsinusoidal grating would be a (rectified) sinusoid of the same (temporal) frequency as that \nof the stimulus, i.e.  a modulated  response (Enroth-Cugell  & Robson,  1966;  Hochstein & \nShapley,  1976;  Spitzer &  Hochstein.  1988).  However,  as  seen  in  Figure  2,  in  some \nstimulus  regimes  the  cell's  response  deviates  from  linearity.  We  conclude  that  the \nlinearity  or  nonlinearity  of the  response  is  dependent  upon  the  stimulus  conditions \n(Spitzer & Hochstein,  1985).  A modulated response is one that would  be  expected from \nsimple  cells,  while  the  sustained  response  seen  at  higher  spatial  frequencies  is  that \nexpected  from  complex  cells.  Our data  therefore  suggest  that the  simple/complex  cell \ncategorization is not complete. \n\nA further example of response time-course dependence on stimulus parameters is seen in \nFigure  3A.  In  this  case,  the  stimulus  was  varied  in  spatial  frequency  and  temporal \nfrequency,  while other dimensions  were  held  constant.  Again,  as  spatial  frequency  is \nraised. the modulation of the PSTH gives way to a more sustained response.  Funhennore, \nas  temporal  frequency  is  raised.  both  the  sustained  and  the  modulated  responses  are \nreplaced  by  a  single  transient response.  When  present,  the  frequency  of the modulation \nfollows  that of the temporal  frequency  of the  stimulus. Fourier analysis of the response \nhistograms  (Figure  3B)  reveals  that  the  DC  and  fundamental  component  (FC)  are  not \ntuned  to  the  same  stimulus  values  (arrows  indicating  peaks).  We  propose  that  this \ninformation  may  be  available  to  the  cell  readout,  enabling  the  single  cell  to  encode \nmultiple stimulus dimensions  simultaneously. \n\nThus, a complete description  of the receptive field  must be multidimensional  in  nature. \nFurthermore,  in  light  of the  evidence  that  the  spike  train  is  not  constant,  one  of the \ndimensions which must be used  to display the receptive field  must be time. \n\nFigure 4  shows one  method of displaying a  multidimensional  response  map,  with  time \nalong  the abscissa (in  10  msec  bins)  and orientation along  the ordinate.  In  the top two \nfigures,  the  z  axis,  represented  in  gray-scale, is  the  number of counts (spikes)  per bin. \nTherefore,  each  line  is  a  PSTH,  with  counts  (bin  height)  coded  by  shading.  In  this \nexample. cell 2 (upper picture) is tuned to orientation, with peaks at 90 and 270 degrees. \nThe cell  is only slightly direction selective, as represented by  the  fact  that the 2 areas of \nhigh activity are similarly shaded. However, there is a transient peak at270 degrees which \n\n\f382 \n\nStern, Aertsen, Vaadia,  and Hochstein \n\nSpatial  Frequency (cpd) \n\n0.6 \n\n0.11 \n\n1.1 \n\n1.5 \n\n2.1 \n\n,.0  ! 4.21  p..  !'\" 1 III\"  !  I.e 1 p.l  !  I.S 1 111.1  ! 1.11 \n\nlb  DG:J~G:J~ \nRCJ~~~~ \n\" .4  :  1.51  pi.,  ! m.s  /II.!  \u2022\u2022.\u2022  lIZ.'  ! n.I  Fi.S  !  is.1 \nC:W~~CitJ~ \nI \n~  2  UJ~CWJ[MJ~ \n\nIII\"! \"'I ~i.I  !  tl.S  pu  ! 14.1  p.1  ! IU  \".S  !  14.1 \n\npi \u2022\u2022  \u2022  D.C  [fT.'  ! 1M  FO.I  ! IS!  tl.O  !  1 .1 IA.'  !  1M \n\nA. \n\nB. \n\n2 \n\nnonnalized values \n\n1 \n\no \n\n1 \n\n1.1 \n\n0.8 \n\n0.6 \n\nSF (cpd) \n\n16 \n\nTF (cycles/second) \n\nFigure  3:  A.  TF/SF  Tuning  of  response  of  VI  cell. \n\nB.  Tuning  of  DC  and  FC  of  response  to  stimulus  parameters. \n\nis absent at 90 degrees. The middle  picture. representing a simultaneously recorded cell \nshows a different pattern of activity. The orientation  tuning of this cell is similar to  that \nof cell 2, but it has  slIonger directional selectivity. (towards 90 degrees).  In this case, the \nlIansient  is  also  at  90  degrees.  The  bottom  picture shows  the  joint activity  of these  2 \ncells. Rather than  each line being a PSTH, each  line is  a Joint PSTH  (JPSTH;  Aertsen et \nal.  1989). This histogram  represents the time-dependent correlated activity of a pair of \ncells.  It  is  equivalent  to  sliding  a  window  across  a  spike  lIain  of one  neuron  and \n\n\f250 \n200 \n150 \n\\00 \n50 \no \n\n60 \n50 \n40 \n30 \n20 \n10 \no \n\ncell 3 \n\n324 \n\n-III t \n.\u00a7  108 -S \n\n~ 216 \nQ,I :s \n\n0 \n\nI: \n... \n.~ \n=> \n\ncell 2,3  coincidence \n\n324 \n\n216 \n\n108 \n\no \n\no \n\n250 \n\n500 \n\nStimulus Encoding by  Multidimensional Receptive  Fields in Single  Cells  and Cell  Populations \n\n383 \n\ncell 2 \n\ncounts/bin \n\n324 \n\n216 \n\n108 \n\no \n\n750 \n\n1000 \nSF=4.S cpd \n\ntime (msec) \nFigure 4:  Response Maps. \nTop, Middle: Single-cell Multidimensional Receptive Fields; \nBottom:  Multi-Cell Multidimensional Receptive Field \n\nasking  when  a  spike  from  another  neuron  falls  within  the  window.  The  size  of the \nwindow can be varied; here we  used 2 msec.  Therefore, we are asking when these cells \nfire within 2 msec of each other, and  how  this is connected to  the stimulus.  The z axis is \nnow coincidences per bin. We may  consider this the logical AND activity of these cells; \nif there  is  a cell  receiving  infonnation  from  both of these neurons,  this  is  the  receptive \nfield  which  would  describe  its  input.  Clearly.  it  is  different  from  the  each  of the  2 \nindividual  cells.  In  our results.  it  is  more  narrowly  tuned.  and  the  tuning  can  not  be \npredicted from  the  individual  components.  We emphasize that  this is  the  \"raw\" JPSTH. \nwhich  is  not corrected  for stimulus effects. common input. or normalized. This is because \nwe  want  a  measure  comparable  to  the  PSTHs  themselves,  to  compare  a  multi-unit \n\n\f384 \n\nStern, Aertsen,  Vaadia,  and Hochstein \n\nreceptive field  to its single unit components. In  this case, however, a significant (p<O.01; \nPalm  et  ai,  1988)  \"mono-directional\"  interaction  is  present.  For  a  more  complete \ndescription of the receptive field,  this type of figure, shown here for one spatial frequency \nonly, can  be  shown for  all  spatial  frequencies as  \"slices\"  along a  fourth  axis.  However, \nspace  limitations  prevent  us  from  presenting  this  multidimensional  aspect  of  the \nmulticellular receptive field. \n\nCONCLUSIONS \n\nWe  have  shown  that  interactions  among  stimulus dimensions  account  for  a  significant \nproponion of the  response  variance of V 1 cells.  The variance of the  interactions  itself \nmay  be a  useful  parameter when  considering  a population response,  as  the amount and \nlocation of the dimensional  inseparability  varies among cells.  We have  also shown that \ndifferent temporal  characteristics of the spike trains can be  tuned to different dimensions, \nand  add  to  the encoding capabilities of the  cell  in  a neurobioiogically realistic  manner. \nFinally, we use these results  to generate multidimensional receptive fields, for single cells \nand small groups of cells. We emphasize that this can be generalized to larger populations \nof cells, and  to compute the population responses of cells that may  be meaningful for the \ncone x as a biological neuronal  network. \n\nAcknowledgements \n\nWe  thank  Israel  Nelken,  Hagai  Bergman,  Volodya  Yakovlev,  Moshe  Abeles,  Peter \nHillman, Roben  Shapley and  Valentino Braitenberg for helpful discussions.  This study \nwas supponed by grants from  the  U.S.-Israel Bi-National Science Foundation (BSF) and \nthe Israel Academy of Sciences. \n\nReferences \n\n1.  Abeles,  M.  Quantification,  Smoothing,  and  Confidence  Limits  for  Single  Units' \nHistograms  1. Neurosci . Melhods 5  ,317-325,1982. \n\n2.  Aertsen,  A.M.H.J.,  Gerstein,  G.  L.,  Habib,  M.K.,  and  Palm,  G.  Dynamics  of \nNeuronal  Firing  Correlation: Modulation of \"Effective Connectivity\" 1. Neurophysio151 \n(5),900-917,  1989. \n\n3.  Enroth-CugeU,  C.  and  Robson,  J.G.  The  Contrast  Sensitivity  of Retinal  Ganglion \nCells of the  Call Physiol.  Lond 187,  517-552,1966. \n\n4.  Hochstein,  S.  and  Shapley,  R.  M. Linear and  Nonlinear  Spatial  Subunits  in  Y Cat \nRetinal Ganglion  Cells 1 Physiol.  Lond 262,  265-284,  1976. \n\n5.  Palm, G., Aensen, A.M.H.J.  and  Gerstein,  G.L.  On  the  Significance of Correlations \nAmong  Neuronal  Spike Trains Bioi. Cybern. 59,  1-11,  1988. \n\n6.  Spitzer,  H.  and  Hochstein, S.  Simple and Complex-Cell Response  Dependencies on \nStimulation Parameters 1.Neurophysiol  53,1244-1265,1985. \n\n7.  Spitzer,  H.  and  Hochstein,  S.  Complex  Cell  Receptive  Field  Models  Prog.  in \nNeurobiology,  31  ,285-309,  1988. \n\n\f", "award": [], "sourceid": 639, "authors": [{"given_name": "Edward", "family_name": "Stern", "institution": null}, {"given_name": "Ad", "family_name": "Aertsen", "institution": null}, {"given_name": "Eilon", "family_name": "Vaadia", "institution": null}, {"given_name": "Shaul", "family_name": "Hochstein", "institution": null}]}