The Journal of Neuroscience, August 6, 2003, 23(18):7021-7033
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Selective Elimination of Corticogeniculate Feedback Abolishes the Electroencephalogram Dependence of Primary Visual Cortical Receptive Fields and Reduces Their Spatial Specificity
Dirk Eyding,1
Jeffrey D. Macklis,2,3,4 *
Ute Neubacher,1
Klaus Funke,1 * and
Florentin Wörgötter5 *
1Department of Neurophysiology, Ruhr University
Bochum, D-44780 Bochum, Germany, 2Department of
Neurology and Program in Neuroscience, Harvard Medical School,
3Division of Neuroscience, Children's Hospital, and
4Massachusetts General Hospital-Harvard Medical School
Center for Nervous System Repair, Massachusetts General Hospital, Boston,
Massachusetts 02115, and 5Department of Psychology,
University of Stirling, Stirling FK9 4LA, United Kingdom
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Abstract
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The role of corticogeniculate feedback in the organization, function, and
state dependence of visual responses and receptive fields (RFs) is not well
understood. We investigated the contribution of the corticogeniculate loop to
state-dependent changes of characteristics of the primary visual cortex
response by using a novel approach of eliminating corticogeniculate projection
neurons with targeted neuronal apoptosis. Experiments were performed in
anesthetized cats (N2O plus halothane) with parallel recordings of
single units from experimental (right) and control (left) hemispheres
2
weeks after induction of apoptosis. Within the experimental hemispheres,
neurons of area 17 and of the dorsal lateral geniculate nucleus (dLGN) showed
an unusually enhanced and prolonged tonic visual response during episodes of
synchronized (syn) EEG activity, whereas response levels during less
synchronized states were almost normal. In addition, dLGN cells showed a
reduced tendency for burst firing and a less regular spike interval
distribution compared with those of controls. These changes are likely
attributable to a tonic depolarization of dLGN relay neurons or, more likely,
to a decreased responsiveness of thalamic inhibitory processes to cortical
feedback. Cortical neurons also displayed an activity-dependent increase in RF
size, in contrast to an almost activity-invariant RF size of controls, a
phenomenon likely related to the elimination of collateral, intracortical
projections of layer 6 neurons. Together, these results demonstrate that
selective chronic elimination of corticogeniculate feedback results in the
loss of EEG-correlated differences of visual processing in the remaining
thalamocortical network, accompanied by a significant increase in excitability
during syn EEG, at the expense of noticeably reduced spatial receptive-field
specificity in the remaining cortical neurons.
Key words: visual cortex; corticogeniculate loop; photoactivation of chlorin e6; neuronal apoptosis; state dependence; receptive-field characteristics
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Introduction
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The spectral composition of the electroencephalogram (EEG), a signal
averaging the activity of large populations of cortical neurons, strongly
covaries with behavioral states of an animal, primarily as a result of the
activity of modulatory brainstem nuclei
(Foote et al., 1991
;
Munk et al., 1996
) (for
review, see Steriade, 1991
).
One of their prominent targets is the thalamus (for review, see
Sherman and Guillery, 2001
),
in which they influence its neuronal responses. As a consequence, during
globally synchronized (
-wave-dominated) EEG states, neurons in the
visual thalamus [dorsal lateral geniculate nucleus (dLGN)] are preferentially
in a burst mode. This mode is characterized by brief, transient,
high-frequency (phasic) responses of only a few tens of milliseconds in
duration, even to prolonged visual stimuli. The same neurons respond to the
same stimuli with long-lasting tonic responses during activated (previously
termed desynchronized,
-wave-dominated) EEG states. During this
so-called tonic transmission mode, dLGN neurons can transfer additional
information about the nature of the stimulus (e.g., its local contrast or
duration) (Sawai et al., 1988
;
Funke and Eysel, 1992
;
McClurkin et al., 1994
;
Wörgötter et al.,
1998a
; Przybyszewski et al.,
2000
). A similar pattern of activityalthough less
pronouncedis also reflected in the visual cortex
(Ikeda and Wright, 1974
;
Singer et al., 1976
;
Livingstone and Hubel,
1981
).
It has been suggested that corticogeniculate feedback plays an important
role in the perpetuation of the tonic component of dLGN relay neurons during
activated episodes (Kalil and Chase,
1970
; Funke and Eysel,
1992
; Wörgötter et
al., 1998a
). This feedback originates in layer 6 of the visual
cortex and contributes up to 40% of the total synaptic input to dLGN relay
neurons, compared with 10 -20% from the retina (for review, see
Sherman and Koch, 1986
;
Montero, 1991
). A considerable
effect of corticogeniculate feedback on dLGN tonic responses was shown by
reversibly cooling (Baker and Malpeli,
1977
; Funke and Eysel,
1992
; Wörgötter et
al., 1998a
) or irreversibly aspirating
(Kalil and Chase, 1970
;
Sillito et al., 1993
,
1994
) the visual cortex. The
temporal structure of the tonic component is also sharpened by
corticogeniculate feedback
(Wörgötter et al.,
1998a
).
Previously, it has not been possible to record visual cortical activity
while inactivating the corticogeniculate feedback projection because of the
global effect of all of the previously available inactivation procedures on
the entire cortical network, also including neurons other than the layer 6
projection neurons. In this study, we applied a novel experimental approach of
biophysical induction of neuron type-specific targeted apoptosis
(Macklis, 1993
;
Sheen and Macklis, 1995
;
Magavi et al., 2000
;
Scharff et al., 2000
;
Shin et al., 2000
;
Fricker-Gates et al., 2002
).
This leads to specific elimination of a large portion of the corticogeniculate
projection neurons, while leaving the remaining network undisturbed. We
combined this approach with electrophysiological recordings in dLGN and visual
cortex. We report here that this experimental elimination of corticogeniculate
feedback leads to a striking reduction of EEG-related cortical response
differences and a reduction of the spatial specificity of cortical receptive
fields (RFs) because of a substantial increase of thalamic and cortical visual
activity during synchronized EEG states.
 |
Materials and Methods
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Induction of apoptosis of corticogeniculate neurons in cortical layer
6. Apoptotic death of corticogeniculate feedback neurons in layer 6 of
cortical areas 17-18 was induced using methods previously described by one of
our laboratories (Macklis,
1993
; Sheen and Macklis,
1994
; Magavi et al.,
2000
; Scharff et al.,
2000
; Shin et al.,
2000
; Fricker-Gates et al.,
2002
). We directly adapted methods developed in the mouse
(Magavi et al., 2000
) for use
in the cat.
Stereotaxic injection of photoactive nanospheres. Under deep
anesthesia with a combination of ketamine (20 mg/kg) and xylazine (2 mg/kg),
cats [n = 9; five with cortical recordings; two with geniculate
recordings after apoptosis; one control experiment with cortical and
geniculate recordings but no final apoptosis (sham control); and one control
experiment with apoptosis and multisite EEG recording instead of multiunit
recording] were stabilized using standard stereotaxic methods, and
craniotomies were performed unilaterally to allow access to the dLGN. All of
the incisions were also locally anesthetized by xylocaine. Nanospheres
carrying the targeting chromophore chlorin e6 [covalently
bound to the 20 - 60 nm subfraction of rhodamine latex microspheres
(Lumafluor, New York, NY)] were stereotaxically pressure microinjected under
electrophysiological control into both dorsal layers (A and A1) of the dLGN of
one hemisphere at three to four sites (20 nl in each site;
10 injections
along each micropipette track). Positions of both the RFs and the optic disc
were recorded on a tangent screen to determine the visual-field positions of
the injection sites (Fig.
1a).

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Figure 1. Schematic illustration of the experimental approach (for details, see
Materials and Methods). a, Injection of fluorescent nanospheres
carrying chlorin e6 (depicted in gray here) into both
layers A and A1 of cat dLGN under electrophysiological control. b,
The region of cortex with retrogradely labeled neurons in layer 6 was
illuminated with deeply penetrating 674 nm light after electrophysiological
verification of the correct topographic region. c, After completion
of targeted corticogeniculate neuron apoptosis, electrophysiological
recordings were conducted in both cortex and dLGN.
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Induction of targeted apoptosis of corticogeniculate projection
neurons. After 2-3 weeks, allowing sufficient time for retrograde
transport of the photoactive targeting nanospheres, apoptosis of
corticogeniculate neurons was induced in cortical layer 6 of primary visual
cortex areas 17 and 18. The same basic surgical procedures were used as
mentioned above. Neuronal apoptosis was induced via the noninvasive,
transdural activation of chlorin e6 with 674 nm light
(region diameter, 1.9 mm; 2.7 kJ/cm2; 2.2 W/cm2)
delivered by a continuous-wave laser (Schaefter und Kirchhoff, Hamburg,
Germany) coupled to custom beam-controlling optics via a quartz fiber. Light
was applied after exposing the appropriate cortical surface representing the
same visual field position as the injection sites, as reverified by RF
mapping. After light exposure, neuronal apoptosis progressively developed over
10 -14 d (Fig.
1b).
Electrophysiology and receptive-field mapping
(Fig. 1c). We applied
conventional approaches for semiacute extracellular recording to allow RF
mapping (Wörgötter et al.,
1998b
). Initial anesthesia was provided by ketamine-xylazine, as
described above. Craniotomy provided access to the areas 17 of both
hemispheres. An additional craniotomy was performed overlying area 18 of the
control hemisphere, to allow insertion of a 0.5 mm silver-ball electrode
epidurally for EEG recording. Femoral artery cannulization enabled infusion of
alcuronium chloride (0.15 mg · kg-1 · h-1;
Alloferin 10; Hoffmann-La Roche, Basel, Switzerland), glucose, minerals, and
amino acids through the femoral artery. Endotracheal intubation enabled
artificial respiration with 70% N2O-30% O2 and 0.6%
halothane for ongoing anesthesia (halothane was increased to 2.0% during any
potentially painful preparation procedure; additional local anesthetic
xylocaine was used at pressure and incision points). Data were obtained by
single-unit recordings, using glass micropipettes in cortical areas 17-18
(n = 76 experimental neurons). Recordings in experimental and control
hemispheres were performed simultaneously in both areas 17. Visual stimuli
were presented monocularly as bright and dark bars (size, 0.2-0.8° x
3-6°; contrast [100(I - I0)/(I +
I0)], 33 and -33%, respectively, displayed on a computer
screen, controlled by standard software [Leonardo system; Lohmann Research
Equipment, Castrop-Rauxel, Germany]). Optimally sized and oriented bars were
presented at 16 evenly spaced positions along a line cross-sectioning the RF
center, in a pseudorandom sequence. The two extreme presentation positions
extended beyond the RF borders. Each stimulus was shown with a duty cycle of
350 msec presentation time and 150 msec pause. Neurons from the control and
the experimental hemispheres were stimulated in an interleaved manner, for a
total duration of 20 - 60 min, depending on the general responsiveness of the
neurons. This resulted in >75 complete stimulus sweeps for all of the
positions. We categorized the neurons into simple and complex cells on the
basis of their neuronal responses and the spatial overlap of RF subfields
responding to bright and dark stimuli. Spatial subfield separation or the
presence of only one response type was interpreted as simple, versus spatial
overlap, which was interpreted as complex. Because we investigated a trait
that affects all of the neurons [at the level of the dLGN
(Funke and Eysel, 1992
) as
well as the visual cortex (Ikeda and
Wright, 1974
)], we pooled all of the data, irrespective of neuron
type (simple or complex).
Information about the cortical layer of the neurons is based on recording
depth, because we avoided interference with the process of targeted neuronal
apoptosis by not marking the electrode tracks.
For the control recordings in the dLGN, an optimally sized dot stimulus was
flashed at a fixed position in the center of the RF (50% contrast; duty cycle,
0.8:1.2 sec), to obtain a standard peristimulus-time histogram (PSTH).
EEG analysis. The state of the EEG was determined by a
sliding-window fast Fourier transformation (time base, 5 sec; step size, 1
sec) of the EEG trace, and the calculation of the
-power ratio (power
of 1-4 Hz band/all of the bands). Previous studies have shown that changes in
the dynamics of thalamic and cortical visual responses were predominantly
correlated with changes in the spectral power of the
frequency band
(Wörgötter et al.,
1998b
; Li et al.,
1999
). Changes in the power of the
band were less
effective, probably because
activity and sleep spindles overlap in
frequency. The proportion of
-wave power was used to differentiate
between synchronized (syn) (high
-wave power ratio, >0.7),
intermediate (moderate
-wave power ratio, 0.3-0.7), and less
synchronized (less syn) (lowest
-wave power ratio, <0.3) EEG
(Wörgötter et al.,
1998b
). Finally, the states of less syn (power ratio, <0.3) and
syn (power ratio, >0.7) were taken to sort visual response data by EEG, and
data from the intermediate state were omitted. The state of less synchronized
in the anesthetized animal is the state that most closely resembles an
activated (desynchronized) EEG in awake animals.
Analysis of cortical and geniculate single unit activity. Because
of the RF-mapping procedure, cortical responses to visual stimuli can be
represented as a three-dimensional (3D) plot, as shown in
Figure 2a, with space
and time as the x- and y-axes and the level of activity as
the z-axis.

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Figure 2. Schematic illustration of the response analysis. a, 3D
representation of a cortical response with time and space on the x-
and y-axes, respectively, and neuronal activity on the
z-axis. The phasic maximum is the reference of the activity measure
andfor graphical reasonsevenly divided into 10 vertical bins.
The time axis has a resolution of 10 msec. Raw data maps were then smoothed
with a 2D Gaussian profile with a of five bins along space and time.
b, PSTH (top) obtained from the central cross-section of the 3D plot
and a contour map (bottom; 2D map) viewed along the z-axis of the 3D
plot. The calculation of the absolute width, the normalized WHH, and DHH of
the tonic response is illustrated. Reference for the latter two is the tonic
maximum (of 100 Hz in this schematic example). The lower bound for absolute
width is twice the SD (2SD) of the spontaneous activity (gray shaded area).
Activity levels above half-height of tonic maximum are shown in black, and
those below are shown with white shading.
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These raw 3D maps (bin width, 10 msec) were convoluted with an optimally
suited two-dimensional (2D) Gaussian profile for smoothing in time and space.
The Gauss had a
of 50 msec on the temporal axis and of five stimulus
positions on the space axis, thus leading to a weighted sliding average of the
map over five bins in each direction. To emphasize the temporal aspects of the
response, we calculated a PSTH from the central cross-section of the RF
including the highest activity (Fig.
2b, top). Because of the smoothing process applied to the
3D map, each bin of the PSTH includes the weighted average from a 5 x 5
matrix of the contour map. The spatial aspects of cortical responses are shown
as 2D contour maps by coding different levels of spike rate with black, white,
and gray shading as described below (Fig.
2b, bottom).
From the smoothed 3D maps, we determined the maximum of the phasic response
component, and for the tonic component, the duration as well as two measures
of the width and the mean amplitude. Two times the SD of the spontaneous
activity level (shown in gray shading in
Fig. 2b) was taken as
the minimum response level, a conventional threshold for separation of
background activity. The phasic response is the transient, high-frequency
response first after stimulus onset, whereas the tonic response is the
sustained response component afterward. The maximum of the phasic response is
the firing rate of the highest bin. To determine the parameters of the tonic
response, we first defined its temporal outline approximately by visual
inspection. This is straightforward, because the shape of the responses was
almost always very distinct (Fig.
2b, top). Within the tonic response, we determined the
tonic response maximum from the smoothed profile. The tonic maximum was then
used to more accurately define the duration of the tonic response as the
difference between those two points at which the firing rate of the neuron
crosses the half-height of the tonic maximum [duration at half-height (DHH)]
(Fig. 2b). The
normalized tonic RF width was determined as the maximal width of the tonic
response portion (again, with the temporal limits given by the duration) at
half-height of the tonic maximum [width at half-height (WHH)]
(Fig. 2b, bottom).
It has been shown that acute silencing of the corticogeniculate feedback
leads to a general depression of geniculate activity
(Kalil and Chase, 1970
;
Baker and Malpeli, 1977
;
Funke and Eysel, 1992
;
Wörgötter et al.,
1998a
). We suspected that this could also lead to a rather
nonspecific depression of cortical activity, resulting in difficulty in
interpreting absolute changes in cortical responses (e.g., attributable to an
iceberg effect, in which RFs appear narrower simply because of the downscaled
peak). To control against this, duration and normalized RF width measures were
defined in this normalized way, such that mere amplitude scaling does not
affect them. In addition, to quantify this scaling effect, the absolute tonic
RF width was determined as the maximum extension of the tonic component above
2 SDs of the spontaneous activity (Fig.
2b, bottom). The mean amplitude is the mean firing rate
at the central cross-section of the tonic component within the limits of its
duration. In a few cases, the tonic response maximum could not be determined
because of strong adaptation of the tonic response, so we defined the tonic
duration by visual inspection.
Geniculate visual responses were analyzed with the aid of peristimulus-time
histograms and interspike interval histograms. Receptive fields of pairs of
dLGN units were stimulated in an interleaved manner with spots of light of
33-50% contrast to background and 0.3-1.0° in diameter, flashed for 800
msec within the center of the RF (total sweep length, 2 sec).
Histology. After electrophysiological data collection, cats were
perfused with heparinized Ringer's solution, followed by 4% paraformaldehyde
in PBS at pH 7.4. After fixation, brains were removed and cryoprotected in 30%
sucrose. Coronal frozen sections (30 µm) of area 17, area 18, and the dLGN
were prepared. Sections were alternately prepared for fluorescence microscopy
and cresyl violet staining (Nissl stain). Sections from the regions of
targeted neuronal apoptosis and the homologous regions of the control
hemispheres were processed for immunocytochemistry using primary antibodies
directed against the mature neuronal marker NeuN (Chemicon, Temecula, CA).
Labeling for NeuN was detected both histochemically and by fluorescence, in
alternate sections: (1) to allow for quantitative neuronal counting, we used
peroxidase anti-peroxidase (Dako, Glostrup, Denmark) and Ni-enhanced
diaminobenzidine (DAB-Ni), and (2) to determine the ratio of retrogradely
labeled neurons via fluorescence of the targeting chlorin
e6 nanospheres (label ratio), we used secondary antibodies
coupled to the green fluorochrome carbocyanine (Cy2) (Jackson ImmunoResearch,
West Grove, PA).
Quantification of neuronal density in area 17-18. Quantitative
analysis was performed using modified stereological methods
(Guillery and Herrup, 1997
).
First, the baseline density of NeuN-labeled neurons was determined by manually
counting Cy2-labeled NeuN sections at high magnification in control regions
outside the regions of laser exposure. Second, we applied semiautomated
modified stereological analysis to quantify neuronal population density in
experimental versus control regions of cortical areas 17-18. We used DAB-Ni
staining for NeuN, with images acquired using a high-resolution CCD camera
(Visitron Systems, Puchheim, Germany). DAB-Ni staining provides excellent
contrast, well suited for semiautomated quantitative analysis. Regions of
interest (ROI) were defined as rectangular regions along the medial or lateral
banks of the lateral gyrus. At the sharply curved tip of the gyrus,
wedge-shaped sectors were defined with the radius of the curvature of the
gyrus. Blood vessels and other atypical structural elements were excluded from
the ROI. Matched, homologous ROIs were analyzed in control and experimental
hemispheres. Minor size differences between the matched ROIs, typically within
±5%, were corrected to the size of the ROI in the experimental
hemisphere. Neurons in the ROI were counted with a sliding-window technique.
The depth of each window (i.e., its dimension perpendicular to the cortical
surface) was 25% of the depth of the ROI; window overlap was 50%. To obtain
optimal quantification, analysis was performed starting in layer 4. We chose
the border between layers 5A and 5B as the zero reference point (ZP) for
analysis, because it is optimally identified in the cat, better than any other
layer boundary (Lund et al.,
1979
). Thus, ZP-relative depth in
Figure 3 refers to depth from
layer 5B-6 to the white matter. For semiautomatic quantitative analysis, we
applied luminance thresholds to the images. Neurons were identified as closed
contours and counted. Correction for potentially overlapping or attached
neurons was achieved by defining a standard neuronal area for neurons within
each ROI windowan assumption valid for layers 5B and 6, because these
layers are primarily composed of equally sized neurons. Objects with areas
that were an integer multiple of the standard area range were counted
multiply, and areas <50% of the standard neuronal area were excluded
(MetaMorph software; Universal Imaging Corporation, West Chester, PA).
Neuronal densities were normalized to compensate for nonspecific differences
between cortices, defining the density of the ZP window as 100%.

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Figure 3. Highly selective elimination of corticogeniculate neurons in areas 17-18 of
experimental cortex. a, Gyrus lateralis of an experimental cat 14 d
after induction of apoptosis. The red arrow indicates the center and direction
of photoactivation by incident light (1.9 mm diameter region of
photoactivation); L, lateral; V, ventral; WM, white matter. b, c,
Merged overlay of images for the rhodamine fluorochrome carried by the
targeting nanospheres (red) and immunocytochemical labeling for the mature
neuronal marker NeuN with Cy2 (green). b, High magnification image of
the blue-boxed region in a, demonstrating the highly efficient
elimination of corticogeniculate projection neurons in the experimentally
targeted region. c, High magnification image of the red-boxed region
in a, demonstrating the normal appearance of corticogeniculate
neurons in control primary visual cortex. d-f, Quantification of
corticogeniculate neuron loss by relative cell density profiles. Regions
denoted by gray and white shading represent assignment to specific cortical
layers (noted above the abscissa). d, Density profile in regions of
corticogeniculate neuron apoptosis at the tip of the gyrus and in the
homologous regions in the control hemisphere (see insets above). e,
Control region at the tip of the gyrus 3-6 mm anterior to the affected region,
within the same experimental hemisphere (see inset). f, Control
regions deep in the medial or lateral banks of the experimental hemisphere.
Note that layer 5A is relatively thicker than layers 5B-6 in these deep
regions compared with that at the tip of the gyrus, as indicated by three
sampling windows and thicker area of gray shading. Error bars in d-f
indicate SDs from the means.
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|
Histological and physiological control procedures. One sham
control experiment was performed, specifically to test our procedures for
inducing targeted neuronal apoptosis, in which all of the experimental steps
were completed except for initiation of targeted neuronal death. We found no
changes in cortical histology and no change in any electrophysiological
parameter, compared with intact controls. In two more cats, we performed
control measurements in the dLGN (n = 36 neurons) after induction of
apoptosis, to compare the effects of chronic silencing of the
corticogeniculate pathway with the previously published acute effects on
phasic and tonic response components
(Funke and Eysel, 1992
) and
temporal precision of spike intervals of dLGN light response
(Wörgötter et al.,
1998a
).
 |
Results
|
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Quantification of neuron loss in layer 6
After inducing the death of the targeted corticogeniculate neurons
(Fig. 1a,b),
histological analysis after the final recording session (c) revealed
a substantial reduction of corticogeniculate projection neurons in the
experimental regions of cortical layer 6. Because the targeting nanospheres
also contain rhodamine as a fluorescent label, we could visualize the loss of
previously labeled neurons. The substantial reduction in layer 6 neurons was
visible by routine light-microscopic inspection of individual sections, which
showed many fewer rhodamine-fluorescent corticogeniculate neurons in the
experimental regions of layer 6, compared with the control regions
(Fig. 3a-c).
To determine quantitatively the loss of the labeled neurons, we first
determined the percentage of total neurons in layer 6 that were initially
labeled by the geniculate injections, without photoactivation and initiation
of targeted neuronal death (label ratio). We then counted the total number of
neurons in layer 6 of the experimental and the appropriate control cortices to
quantify the total neuron loss (total loss ratio). From these two ratios, we
calculated how many of the labeled neurons underwent apoptosis.
The label ratio of corticogeniculate neurons, compared with all of the
NeuN-labeled neurons in control regions of experimental animals, was 45
± 3% in the densest sublayers, in agreement with previous studies
(McCourt et al., 1986
;
Katz, 1987
). Thus, it is
reasonable to assume that almost every LGN projecting neuron was actually
labeled within the cortical region corresponding to the injection site. As
shown in Figure 3d,
the quantitative evaluation of the total loss of neurons in experimental
regions was 27 ± 4% in the bin with the highest loss. This bin
anatomically matched the sublayers with the densest label. Thus, 60 ±
9% (0.27/0.45) of labeled corticogeniculate neurons were eliminated in the
targeted regions. ANOVA demonstrated highly significant effects of hemisphere
(p < 0.001) and depth (p < 0.001), and no interaction
between depth and hemisphere (p = 0.15).
In both of the control regions immediately adjacent to the experimental
regions (Fig. 3e), and
in deep control regions (f), quantification of the density of layer 6
neurons was uniform with complete overlap of the density profiles,
demonstrating no loss of neurons in the controls. Together, these results
indicate that targeted induction of corticogeniculate neuron death was quite
efficient and occurred only in the appropriate highly localized region of
layer 6 in visual cortex. (See Discussion for additional details.)
We will now first discuss the effect of targeted apoptosis on the cortical
network and later compare it with responses from dLGN neurons recorded after
having applied the same experimental protocol.
Consequences of layer 6 neuron loss on cortical responses
We recorded the responses of 76 individual cortical neurons. It is known
from previous studies that the spatial-response
(Wörgötter et al.,
1998b
) andto an even greater extentthe
temporal-response (Ikeda and Wright,
1974
; Livingstone and Hubel,
1981
) properties of cortical neurons are significantly different
during different EEG states, and there is evidence that corticogeniculate
influences are involved in this (Funke and
Eysel, 1992
;
Wörgötter et al.,
1998a
). Our approach took advantage of this predictable dependence
of cortical response properties on EEG states. In the following, we will base
our analysis on the direct comparison of the responses from simultaneous
recordings in the control and experimental cortex during different EEG
states.
We found that elimination of corticogeniculate neurons had striking effects
on cortical response properties, abolishing the normal dependence on EEG
state. In control cortex with intact corticogeniculate feedback circuitry,
longer and more pronounced tonic responses occurred during less synchronized
EEG states, compared with shorter, more phasic responses during synchronized
EEG (
-wave-dominated EEG). No significant differences were found
between simple (experimental hemisphere, 25; control, 22 subfields) and
complex (experimental, 52; control, 27 subfields) cells, neither regarding the
EEG-dependent differences in the control hemispheres nor its abolishment in
the experimental hemispheres, respectively. Therefore, the results will be
pooled for these two populations throughout the paper. This highly
reproducible variation in responses between less synchronized and synchronized
EEG states is represented graphically for four cortical neurons in control
cortex (Fig. 4a-d).
The diagrams show PSTHs of the activity of the control neurons at the central
cross-section of their receptive fields, as described in Materials and
Methods. The right side (Fig.
4e-h) shows four simultaneously recorded neurons from the
experimental cortex with targeted elimination of corticogeniculate neurons
(each row shows pairs of simultaneously recorded neurons). In contrast to
responses of neurons in control cortex, tonic responses in experimental cortex
during synchronized EEG were significantly increased; in some cases, they even
exceeded responses observed during less synchronized EEG, in duration and/or
amplitude (Fig
4e,f,h). Bins within the tonic response exceeding
half-height of the tonic response maximum are labeled by the white area, which
delineates half-height of the tonic response and its duration according to the
half-height amplitude threshold.

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Figure 4. State dependence of tonic visual responses in control and experimental
hemispheres. Four representative neurons are depicted from control
(a-d) and experimental (e-h) hemispheres. The PSTHs show the
activity of each cortical neuron along the central cross-section of its
receptive fields as demonstrated in Figure
2. a-d, As expected, responses in control hemispheres are
longer and more pronounced during less synchronized EEG. e-h, The
situation is reversed in the experimental hemispheres, in which responses are
stronger and have a longer duration during synchronized EEG. White boxes label
the part of the tonic response that exceeds half-height of maximum. Twenty
second-long EEG traces above the PSTHs show the typical EEG pattern during
those episodes of spike activity collected in the corresponding PSTHs. To the
left of e-h, coordinates are indicating the visuotopic location of
the RF of the respective neuron (box), in relation to the RF location of the
original nanosphere injection sites (gray dots) and the center of the region
of targeted corticogeniculate neuron apoptosis (X), within the visual
field (axes in degrees of visual angle; HM, horizontal meridian; VM, vertical
meridian). Cell types: complex (a), complex (b), simple
(c), simple (d), simple (e), simple (f),
complex (g), and complex (h).
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Not only the amplitude and duration of the tonic visual response but also
the spatial distribution of the activity differed between the experimental and
control hemispheres during the different states of the system. RF widths in
the experimental cortex appeared to covary with the amplitude of the response
and were often wider with a high-amplitude response during syn episode than
during a lower amplitude response in the less syn state. In contrast, in
control cortex, no such covariation between amplitude and RF width could be
observed. The RFs appeared to be equally wide or even narrower during the less
syn episodes, despite the higher amplitudes. To more clearly demonstrate this
effect, we replotted in Figure
5 the same data that are shown in
Figure 4 (except for
Fig. 4d because of
missing tonic response) by showing 2D RF plots with normalized RF widths,
which reflect WHH (areas filled in black) of the tonic response amplitude
maximum (Fig. 2). This measure
was chosen, because it is insensitive to mere scaling (iceberg) effects and
was therefore also used for statistical quantification
(Fig. 6). This representation
shows that tonic RFs in control cortex were typically substantially narrower
(early part) during less synchronized EEG than during synchronized EEG
(a-c), in spite of the fact that the tonic amplitude was typically
higher during the less syn state. In contrast, the normalized tonic RF widths
in the experimental cortex showed a similar width during both EEG states
(d and f), even wider RFs during less syn episodes
(e), or, because of a very large amplitude difference, still wider
RFs during syn episodes (g). In summary, these results suggest that,
in normal cortex, there exists a normalizing mechanism that keeps the size of
the receptive fields relatively constant. This mechanism appears to be
impaired during chronic elimination of the dLGN projecting layer 6 neurons,
most likely because of their collateral projection to layer 4.

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Figure 5. Examples of cortical receptive-field maps with activity scaling normalized
to the activity level at width at half-height of tonic response. Those
examples of Figure 4 with
sufficiently strong tonic responses are shown as 2D contour plots (only
d is omitted). Shown in black is the area that had higher activity
than one-half of the tonic maximum, which is depicted in absolute firing rate
below the plots. WHH and DHH can be directly seen in this representation. max,
Maximum of tonic response.
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Figure 6. Quantitative analysis of response properties of experimental and control
primary visual cortex. Responses of experimental (open squares) and control
(filled squares) neuron samples are depicted during both synchronized and less
synchronized EEG states, with regard to their duration (a),
phasic-response (b) and tonic-response (c) amplitude
(ampl.), tonic receptive-field width (e), and normalized (norm.)
tonic receptive-field width (f). Logarithmic scatter plots show
values obtained during less synchronized EEG, plotted against those observed
during synchronized EEG. Enlarged dots depict the mean values for experimental
(open) and control (filled) data. Histograms in the top right corners show the
distributions of the data points (open bars, experimental; filled bars,
control) with respect to the diagonal. This indicates the relative deviation
( ) from an EEG-independent behavior. The inset histograms at the bottom
right of each panel show mean values and SEs of the distributions; large
values are indicative of strongly EEG-dependent behavior; significance was
evaluated by a one-sample Student's t test (mean against = 0)
and U test between hemispheres. One hundred twenty-six
receptive-field on and off subfields were analyzed; tonic receptive-field
width could be reliably measured in 61 of these subfields. The differences in
a, c, and f are highly significant; p < 0.001.
In d, the ratio (value of less syn episodes divided by values of syn
episodes) of absolute (abs.) tonic RF width is plotted against the
corresponding amplitude ratio, to compare the covariation of RF width and
amplitude. Regression lines for the samples of data from experimental (solid
line) and control (dotted line) hemisphere are added.
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Statistical analysis
Quantitative statistical analysis confirmed the qualitative observations
(Fig. 6, Tables
1 and
2). The previous qualitative
analysis suggested that responses in experimental cortex increased in both
tonic amplitude and duration, particularly during synchronized EEG, and that
tonic receptive fields scaled with amplitude.
Figure 6 presents this
quantitative analysis graphically, first with scatter plots of the raw data
and their mean values (large dots). Histograms in the top right corner of each
panel and their means (small insets) demonstrate the elimination of
EEG-dependent behavior of cortical responses in the experimental hemisphere
(Fig. 6a,c, open
bars). Responses were only of 7 ± 7% longer
(Fig. 6a) and 6
± 5% higher (c) amplitude during less syn than during syn.
This elimination of EEG-dependent behavior was primarily attributable to a
significantly increased response duration
(Fig. 6a) and
amplitude (c) during synchronized EEG, compared with the control
cortex (right shift of the large white dot only along the x-axis
compared with the black dot). Because the change during less syn episodes
appeared negligible, we calculated the shift only along the x-axis,
which corresponds to an increase in duration of 64 ± 10% and an
increase in amplitude of 77 ± 14% during syn episodes in the
experimental hemispheres compared with the control cortices.
This was in sharp contrast to control cortices, in which the duration and
amplitude of tonic responses were typically enhanced during the less
synchronized EEG state [Fig.
6a,c, black bars, corresponding to 62 ± 12% longer
duration (a) and 34 ± 8% higher amplitude (c)],
consistent with previous reports (Ikeda
and Wright, 1974
; Livingstone
and Hubel, 1981
). Phasic responses were similar under both
synchronized and less synchronized conditions
(Fig. 6b).
From the examples above, we expected a change in the relation between
response amplitude and RF width in the experimental cortices. Statistical
analysis demonstrated that covariation of receptive-field width and amplitude
occurred only in experimental hemispheres, whereas RF width remained
independent of the response amplitude in controls. This overall result is
depicted more completely and with more detail in the next figure panels. For
statistical analysis, we measured receptive-field widths (absolute and
normalized; see Materials and Methods) during the tonic responses. This was
possible only for a subset of neurons, in which the receptive fields were
sufficiently smooth. The covariation of absolute RF width and response
amplitude was analyzed in Figure
6d by plotting the less syn/syn ratio of the absolute RF
widths against the ratio of the corresponding response amplitudes. In cases of
a covariation, one would expect most data points to lie in the concordant
quadrants (both ratios below or above 1 of the plot). We found exactly this
result in the experimental cortex. Significantly more of the data points in
Fig. 6d are in the
concordant quadrants (31/38;
2 = 15.1; p < 0.001),
demonstrating that RF widths scaled directly with amplitude. In control
cortex, however, the observed amplitude increase during less synchronized EEG
(Fig. 6c) was not
typically accompanied by an increase in receptive field width; receptive
fields in control cortex typically remained narrow. Therefore, the majority of
data points in the controls lie in the discordant quadrant at the bottom right
(15/23), although not significantly (
2 = 2.1; p <
0.2). Only for much higher amplitudes during less syn compared with syn
episodes (large values on the x-axis) did RF width tend to increase
as well. In spite of these few cases, the linear regression still had a much
lower slope in the control hemisphere (0.31 ± 0.15; stippled line) than
in experimental cortices (0.60 ± 0.13). Moreover, only for the
experimental hemispheres, there is a significant correlation (nonparametric
according to Spearman, r = 0.65; p < 0.001), which is not
found in the control cortices (r = 0.35; p = 0.10). Such
exceptions were rare (as shown in Fig.
6e), and they did not affect the mean of the
absolute tonic RF widths, which did not differ between the different states in
either experimental (-5 ± 5%) or control hemispheres (+4 ± 9%).
As expected, the normalized tonic RF widths differed strongly only in the
control hemispheres; during less syn episodes, they were clearly narrower than
during syn episodes (-27 ± 4%). This difference was completely absent
in the experimental hemispheres (+3 ± 5%)
(Fig. 6f).
The insets in Figure 6, a-c and
e-f, summarize the findings: the normally observed
EEG-dependent changes in cortical-response characteristics were eliminated in
experimental cortices because of an increase in the duration (a) and
amplitude (c) of neuronal responses during synchronized EEG, whereas
their spatial selectivity was diminished simultaneously (f).
Table 1 summarizes the means
and SEM for the samples shown in Figure
6 (except for d). For tonic-response duration and
amplitude, Table 2 shows that
simple and complex cells were affected almost in the same manner, but the
increase of tonic visual activity in the lesioned hemisphere is on average
somewhat stronger in simple cells. The differences in tonic-response amplitude
and duration, however, do not differ significantly between simple and complex
cells, both in control and experimental hemispheres.
dLGN data
As a control, we also performed recordings from 36 neurons in the dLGNs of
two cats (18 pairs in experimental/control hemispheres), at or close to the
injection sites as verified by stereotaxic coordinates and visual field
positions. Similar to what was found for cortical responses, the geniculate
visual responses also showed an increase in the tonic response component
during syn episodes, leading to a loss of its normal EEG dependence
(Sawai et al., 1988
;
Funke and Eysel, 1992
)
(Fig. 7). dLGN neurons of the
control hemispheres showed the typical reduction in the tonic visual response
component when the EEG changed from a less syn
(Fig. 7c) to a more
syn (a) pattern. In contrast, dLGN neurons recorded simultaneously
from the experimental hemisphere did not show this strong reduction of the
sustained light response (Fig. 7, compare
g with e). Responses during less syn episodes
appeared similar to those observed in the intact system with respect to
duration and amplitude (Fig. 7, compare
g with c). In addition, we observed a changed
spike interval structure, predominantly a loss of the temporal precision of
distinct spike interval modes normally observed in the tonic response during
less syn episodes (Funke and
Wörgötter, 1995
;
Funke et al., 1996
). The inset
diagram of Figure 7d
shows two modes (arrows) in the interval distribution obtained from the tonic
light response during the less syn state. These modes disappear during the syn
state (Fig. 7b,
inset). In a similar manner, we found that the modes became broader or merged
to a single mode in the experimental hemispheres
(Fig. 7f,h, insets).
The broadening of these interval modes was more pronounced than after an acute
silencing of the corticogeniculate feedback
(Funke et al., 1996
;
Wörgötter et al.,
1998a
); in many cases, a complete loss of distinct modes was
evident, preventing quantification of interval mode width in some cases (see
below). In addition, we found a lower ratio of burst spikes versus single
spikes in the experimental hemispheres
(Fig. 7, compare large diagrams
of f and h with those of b and d; short
intraburst spike intervals are left of the vertical bar). Even during syn
episodes, the ratio of short versus longer spike intervals was low in the
experimental hemispheres, contrary to the normal situation in less activated
states and after acute disruption of the corticogeniculate feedback
(Wörgötter et al.,
1998a
). Mean spontaneous activity levels were somewhat higher in
the experimental hemisphere for a few cells, but on average, the difference
was not significant and cannot be the reason for the reduced ratio of burst
spikes to single spikes.

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Figure 7. Effect of chronic elimination of corticogeniculate feedback on thalamic
visual activity. Peristimulus-time histograms (top rows; a, c, e, g)
and spike interval histograms (bottom rows; b, d, f, h) showing the
temporal properties of light responses evoked in two dLGN relay cells during
different states of the system (top set, syn state; bottom set, less syn
state), one recorded from the control hemisphere (a-d) and one
simultaneously recorded from the experimental hemisphere (e-h). A
spot of light slightly larger than the receptive-field center of the dLGN
cells was flashed for the time indicated by the horizontal bar below histogram
(a). The spike interval histograms composed of bars were calculated
for the entire activity during the recording episode for spike intervals
between 1 and 30 msec. The four bins to the left of the vertical line
dissecting the diagram correspond to spike intervals usually composing a burst
(1-4 msec). The smaller inset diagrams (solid lines) show the spike interval
distribution during the tonic part of the visual response, for intervals
between 1 and 50 msec. Arrows in histogram d indicate two interval
modes, as described by Funke and Wörgötter
(1995 ). T, Time (length of
interval). i, Shown are the positions of the tracer injections (gray
dots), the center of laser application (black dot), and the area of the
receptive field of the dLGN relay cell in the experimental hemisphere
(rectangle) (the cell of the control hemisphere had an RF at a topographically
corresponding position within the contralateral visual hemifield). Visual
stimulation of the two RFs was performed in an interleaved manner. Scale in
degrees of visual angle; VM, vertical meridian; HM, horizontal meridian.
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Figure 8 summarizes the
statistical analysis of the dLGN data. The mean ratio of tonic- to
phasic-response amplitudes during the syn state clearly increases in the
experimental hemispheres and approaches values usually obtained during less
syn episodes in the control hemisphere
(Fig. 8a). The ratio
between less syn and syn states for this index is almost 1 in the experimental
hemisphere and significantly smaller than the normal ratio obtained for the
control hemispheres (Fig.
8b). For a subset of cells (n = 12 pairs in
experimental and control hemisphere) that showed at least one clear mode in
the spike interval distribution of the tonic response
(Fig. 7d, inset
diagram), we calculated the WHH of these modes. For the remaining cell pairs,
either one or both cells of a pair did not show a clear mode in the interval
distribution. In most cases, it was the cell of the experimental hemisphere
that had a broad distribution without a distinct interval mode.
Figure 8c demonstrates
that mean WHH of modes calculated for the neurons of the experimental
hemisphere is significantly broader than that of the neurons recorded from the
control hemisphere during the less syn state. The WHH for the hemisphere with
chronic elimination of corticogeniculate feedback is
50% larger than that
of the control hemisphere. For comparison, the increase in WHH of interval
modes was
25% after acute silencing of the corticogeniculate feedback
(Funke and Wörgötter,
1995
; Funke et al.,
1996
). To quantify the probability of high-frequency burst firing,
we calculated the ratio of the number of interspike intervals of <5 msec to
the number of spike intervals of
5 msec.
Figure 8d shows two
major findings: (1) the typically higher incidence for burst firing (higher
ratio) during the syn state compared with that of the less syn state as seen
in the control hemisphere is abolished in the experimental hemisphere, and (2)
the likelihood of burst firing is generally reduced in the experimental
hemisphere, with a reduction of 80% in the syn state and 65% in the less syn
state, indicating that the thalamic neurons may be tonically depolarized and
thus are not able anymore to achieve a state suitable for generating
low-threshold calcium spike-carried bursts.

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Figure 8. Statistical analysis of the temporal structure of dLGN activity.
a, Tonic/phasic ratio of light responses in control and experimental
hemispheres in relation to the two system states of syn and less syn.
b, The change of the tonic (ton.)/phasic (phas.) index with respect
to EEG state. c, The mean WHH of spike interval modes during the
tonic light response in control and experimental hemispheres. d, The
ratio of spikes included in a burst (1-4 msec spike intervals) to single
spikes (>5 msec spike intervals) in control and experimental hemispheres.
For each cell pair (number of pairs analyzed is indicated at the bottom of
histograms), one neuron was recorded from the unaffected hemisphere (control)
while the other neuron was simultaneously recorded (with interleaved visual
stimulation in the contralateral hemifield) from the experimental hemisphere.
Asterisks indicate statistically significant differences between samples
(*p < 0.05; **p < 0.01;
Student's t test). Error bars indicate SEM.
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Control experiments
Controls (sham controls) in which all of the experimental steps were
performed except for initiation of targeted neuronal death showed the
following: (1) no changes in cortical histology, compared with intact
controls, (2) specifically, no change in the number of corticogeniculate
neurons, and (3) no change in any electrophysiological parameter, compared
with intact controls in dLGN and cortex.
In one experiment with induced apoptosis of corticogeniculate projection
neurons, we made no single-unit recordings but local EEG recordings directly
above the lesioned cortex, 4 mm anterior to the lesion within the same
hemisphere (still area 17) and at a position opposite to the lesion within the
control hemisphere. The EEG was recorded via small (<0.5 mm) silver-ball
electrodes attached to the cortical surface. We made long-lasting recordings
with the cat either in the dark or a dimmed room, or during full-field flicker
stimulation. Neither the spectral power of the EEG nor the coherence of EEG
waves were found to differ for the three recording sites (data not shown). For
additional details, see Discussion.
 |
Discussion
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The combination of targeted neuronal apoptosis of corticogeniculate
projection neurons with electrophysiological recording in visual cortex and
thalamus made it possible for the first time to investigate directly whether
elimination of a large proportion of the corticogeniculate projections would
result in a loss of EEG-dependent response properties in the visual cortex
itself. The approach of inducing targeted apoptotic neuronal death was
established in mice (Macklis,
1993
; Sheen and Macklis,
1994
) but adaptation to cat neocortex was successful with regard
to labeling efficiency (McCourt et al.,
1986
; Katz, 1987
;
Sheen and Macklis, 1995
) and
efficiency of induced neuronal apoptosis
(Macklis, 1993
;
Sheen and Macklis, 1995
;
Scharff et al., 2000
) when
compared with rodent studies.
So far, the contribution of corticogeniculate feedback to state-dependent
differences at the level of the dLGN has been documented only in acute
experiments (Funke and Eysel,
1992
; Wörgötter et
al., 1998a
). It has been found that acute elimination of the
corticogeniculate feedback usually causes a decrease in geniculate visual
responsiveness during less syn episodes, whereas its effects are less
pronounced during syn states when responsiveness is already low. In strong
contrast to these previous studies, the current report demonstrates that the
chronic and highly selective elimination of this feedback circuitry leads to
an increase in neuronal activity in the visual cortex (and the dLGN), evident
primarily during states of synchronized EEG.
These results raise three major questions: (1) Why does elimination of
corticogeniculate feedback lead to the abolition of state-dependent variations
in visual responsiveness? (2) Why is there a response increase, despite the
elimination of excitatory feedback? (3) What is the reason for the
activity-dependent increase in receptive-field size in the experimental
cortex?
First, it is likely that the observed loss of state dependence is the
result of equally strong retinogeniculate signal transmission during syn and
less syn episodes, attributable to either upregulated retinal input or other
influences. The high retinogeniculate transfer ratio
(Coenen and Vendrik, 1972
)
indicates that the efficiency of the retinal synapse is already high under
normal conditions and cannot be substantially increased. This leads to tight
coupling of the relatively sharp spike interval modes in retina and dLGN
(Funke and Wörgötter,
1995
). The broadening of the interval histograms observed here
(Fig. 7) likely results from
spurious additional action potentials of nonretinal origin, assuming that the
membrane of dLGN neurons is tonically depolarized. Additional support for this
idea arises from the substantially reduced number of high-frequency bursts in
the dLGN. Normally, one finds many high-frequency bursts in dLGN responses to
visual stimuli during syn EEG (Lu et al.,
1992
) (for review, see
Sherman, 1996
). This indicates
prolonged hyperpolarization of the cell membrane, which is required to elicit
low-threshold calcium spikes (LTS) as a result of deinactivating the
responsible IT current
(Suzuki and Rogawski, 1989
;
Lu et al., 1992
). When
analyzing dLGN responses in the treated cats, we found very few bursts even
during the syn state. This suggests that the membrane potential was hardly
ever hyperpolarized long enough to enable LTS-mediated spike bursts.
Second, previous studies investigating the effects of retinal deprivation
demonstrated that the removal of excitatory input from the retina
(deafferentation) leads to increased excitability of target neurons in dLGN
and cortex (Eysel, 1979
;
Hendry and Jones, 1988
;
Kaas et al., 1990
;
Gilbert and Wiesel, 1992
;
Hendry and Miller, 1996
;
Gilbert, 1998
;
Eysel et al., 1999
). This
result has been interpreted as a compensatory reaction of the remaining
network in response to the loss of its main excitatory input
(Eysel, 1979
). Evidence exists
that this might be attributable to homeostatic mechanisms that influence the
global postsynaptic sensitivity to maintain a constant spiking output
(Frégnac, 1998
;
Turrigiano et al., 1998
). Loss
of numerous corticogeniculate synapses may elicit a compensatory
overexpression of metabotropic glutamate receptors found at the
corticogeniculate synapse (McCormick and
von Krosigk, 1992
; Rivadulla
et al., 2002
). Activation of these receptors reduces a potassium
leak current, thereby causing depolarization of the cell membrane.
Corticogeniculate inputs also target inhibitory neurons of dLGN and thalamic
reticular nucleus (TRN) (Weber et al.,
1989
; Montero,
1991
). Interestingly, both synaptic density
(Weber et al., 1989
) and
synaptic strength (Golshani et al.,
2001
) seem to be higher for cortical synapses on inhibitory
interneurons compared with dLGN relay cells. Removal of the corticogeniculate
projection would, thus, more strongly weaken the inhibitory impact on dLGN
relay cells than the facilitation by direct cortical inputs. The finding that
thalamic relay cells in the lesioned hemisphere show a strongly reduced
likelihood of generating bursts is a strong indication for failure of
inhibitory interactions between the TRN and thalamic projection neurons. As
discussed by Steriade (2000
),
this corticogeniculate loop is essential for the synchronization of slow
thalamocortical rhythms, like
waves. Elimination of the cortical input
to TRN will disrupt this resonance loop but may also affect the
state-dependent transmission of retinal signals.
Finally, modulatory inputs from the brainstem arousal centers might also
come into play; however, this scenario is less likely, because these systems
are not directly affected by our experimental procedures.
It is by now widely accepted that the interactions between thalamus,
brainstem, and cortex are primarily responsible for the generation of the
different EEG states, in part by influencing the response modes of thalamic
cells. Intracortical mechanisms seem to be less important in this respect.
This view is also supported here. The consistency of our results with the
different mechanisms discussed above strongly suggests that effects occurring
at the geniculate cells themselves are primarily responsible for the enhanced
visual responsiveness during the syn state in cortex and dLGN. Intracortical
plasticity reported by others (Kaas et
al., 1990
; Eysel et al.,
1999
) is expected to also occur under the experimental conditions
reported here, but the increased excitability of dLGN neurons favors a
thalamic process. Intracortical plasticity, however, may underlie the changed
relationship between activity and receptive-field size of cortical neurons, as
discussed below.
The change in EEG-dependent activity in thalamus and cortex implies that
also the spectral composition and coherence of the EEG within the lesioned
cortex may have changed. This, however, was actually not the case. The
diameter of the EEG electrode above the lesioned cortex (<0.5 mm) should
have been small enough compared with the diameter of the lesioned area of
layer 6(
1.9 mm) to detect local changes in activity. One explanation
could be that the huge number of synapses that originate from lateral cortical
projections and that are not affected by the lesion compensate for the loss of
state-dependent oscillatory activity within the much smaller number of
thalamic inputs to layers 4 and 6 of the lesioned site. Thus, the local
cortical processing of visual activity in individual neurons seems to be
affected, whereas the global generation of rhythmic activity patterns is
not.
Third, why does RF size scale with tonic activity in experimental cortex,
but not in control hemispheres, which operate essentially in an RF
size-invariant condition? Here, it is more likely that cortical rather than
thalamic mechanisms are involved, because dLGN neurons show little if any
state-dependent changes in RF size
(Hartveit et al., 1993
;
Suder et al., 2002
).
Furthermore, lateral inhibition in the dLGN itself
(Tsumoto et al., 1978
) is
spatially too limited to cause the observed changes in cortical RF size. Thus,
it seems that changes in the strength and/or spatial convergence of excitatory
and inhibitory cortical inputs are likely to be the source of the reduced size
invariance.
Layer 4 neurons have been shown to receive direct excitatory input from
layer 6, which is less efficient than the input from other layer 4 neurons,
but with a tendency for facilitation with repetitive input
(Stratford et al., 1996
;
Tarczy-Hornoch et al., 1999
).
Using reversible inactivation of layer 6 with GABA injection, Bolz and Gilbert
(Bolz and Gilbert, 1986
;
Bolz et al., 1989
) demonstrated
an inhibitory action of layer 6 on layer 4 and superficial layers to be
responsible for the length tuning of the layer 4 neurons. It seems likely that
the balance between intracortical excitation and inhibition has been disturbed
by our experimental procedures, possibly with the final result of a reduced
lateral inhibition in the cortical network. This is supported by findings
showing that spatial RF properties in the intact cortex are independent of the
level of activity (Sclar and Freeman,
1982
; Skottun et al.,
1986
). Similar normalizing mechanisms may be involved in other RF
properties like orientation tuning and local contrast adaptation
(Heeger, 1992
;
Carandini and Ferster, 1997
;
Troyer et al., 1998
;
Sanchez-Vives et al., 2000
).
Lateral inhibition is one possible mechanism to achieve a narrow cortical RF
width, even under high-activity conditions of a less synchronized EEG
state.
Together, the experiments reported here demonstrate that selective chronic
elimination of corticogeniculate feedback results in a loss of EEG-correlated
differences in the remaining thalamocortical network, leading to a significant
increase in excitability during syn EEG, at the expense of reduced spatial RF
specificity in cortical neurons. Our results indicate that corticogeniculate
feedback is critical for the establishment of differences in sensory
processing, and that the observed changes are most likely related to a
weakening of cortically driven inhibitory thalamic networks.
 |
Footnotes
|
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Received Nov. 1, 2002;
revised May. 28, 2003;
accepted May. 29, 2003.
This work was supported by a collaborative grant from the Human Frontiers
Science Program (F.W. and J.D.M.) and by a National Institute of Child Health
and Human Development Mental Retardation Research Center grant (J.D.M.).
Additional support was provided by grants from the National Institutes of
Health (J.D.M.) and Deutsche Forschungsgemeinschaft (F.W. and K.F.). We thank
Cindy C. Tai and Max Christian for excellent technical assistance, Nicolas
Kerscher for experimental assistance, Ulf Eysel for helpful discussions, and
Sanjay S. P. Magavi for helpful input from parallel mouse work.
Correspondence should be addressed to Dr. Klaus Funke, Department of
Neurophysiology, Medical Faculty, Ruhr University Bochum, D-44780 Bochum,
Germany. E-mail:
funke{at}neurop.ruhr-uni-bochum.de.
D. Eyding's present address: PAION GmbH, Martinstrasse 10-12, D-52062
Aachen, Germany.
Copyright © 2003 Society for Neuroscience
0270-6474/03/237021-13$15.00/0
* J.D.M., K.F., and F.W. contributed equally to this work. 
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References
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