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J Neurophysiol 96: 1981-1990, 2006. First published June 21, 2006; doi:10.1152/jn.00404.2006
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Two-Dimensional Coincidence Detection in the Vibrissa/Barrel Field

Krista M. Rodgers, Alexander M. Benison and Daniel S. Barth

Department of Psychology, University of Colorado, Boulder, Colorado

Submitted 17 April 2006; accepted in final form 16 June 2006


 ABSTRACT
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
Coincidence detection in visual and auditory cortex may also be critical for feature analysis in somatosensory cortex. We examined its role in the rat posteromedial barrel subfield (PMBSF) using high-resolution arrays of epipial electrodes. Five vibrissae, forming an arc, row, or diagonal, were simultaneously or asynchronously stimulated to simulate contact with a straight edge of different angles at natural whisking velocities. Results indicated supralinear responses for both slow-wave and fast oscillations (FOs, about 350 Hz) at intervibrissa delays <2 ms. FO represented the earliest and most precisely tuned response to coincident vibrissa displacement. There was little difference in the spatiotemporal pattern of slow-wave or FO responses in the row, arc, or diagonal. This equivalence of function suggests that the PMBSF may be capable of working as a two-dimensional integrative array, processing spatial features based on coincidence detection despite the direction that the vibrissae pass across an object.


 INTRODUCTION
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
Spatiotemporally structured stimuli, such as a figure moving across the retina or a low-frequency sound arriving at the left and right cochlea at slightly different times, provide essential information about object presence, location, and in the case of vision, information about form, based solely on the timing with which subsections of the receptive surface are coincidentally excited (Carr 1993Go; Lee and Blake 1999Go; Usher and Donnelly 1998Go). In the visual system, temporal synchronization of neuronal responses between regions of retinotopically organized sensory cortex has been postulated as a fundamental mechanism by which salient stimulus features may be dynamically bound together (Engel et al. 1992Go; Singer 1993Go; Singer and Gray 1995Go) and has been demonstrated to occur with millisecond accuracy in the CNS (Konig et al. 1996Go; Singer et al. 1996Go). Temporal coincidence detection on a much finer time scale of microseconds occurs in the auditory cortex and is essential for coding intraaural time differences required for sound localization (Carr 1993Go).

Coincidence detection may also be critical for feature analysis in the somatosensory system (Roy and Alloway 2001Go). Perhaps the most attractive candidate for exploring this possibility is the rodent vibrissa system. The somatosensory system of rodents is dominated by afferent input from the vibrissae, which serve as a primary means of close range environmental exploration. Approximately half of the primary somatosensory cortex consists of an orderly array of cellular columns, or "barrels" (usually referred to as the posteromedial barrel subfield or PMBSF), in register with the macrovibrissae on the contralateral face. As rats examine an object in the environment, they repeatedly whisk the vibrissae forward as a unified array, establishing rapid spatiotemporal patterns of contact (Sachdev et al. 2001Go) that presumably result in similarly rapid spatiotemporal patterns of neuronal activity within and between the barrels of the PMBSF. Although the rodent vibrissa system is thought to perform a number of complementary tasks, including texture discrimination (Andermann et al. 2004Go; Arabzadeh et al. 2004Go, 2005Go; Carvell and Simons 1990Go; Guilmage-Robles et al. 1989Go; Neimark et al. 2003Go) and spatial sampling such as gap detection, distance discrimination, and head-centered orientation (Harris et al. 1999Go; Hutson and Masterson 1986Go; Krupa et al. 2001Go; Sachdev et al. 2000Go; Schiffman et al. 1970Go; Shuler et al. 2002Go; Vincent 1912Go), behavioral and physiological studies suggest that the macrovibrissae may also provide information about object features such as edge orientation and shape (Benison et al. 2006Go; Carvell and Simons 1990Go; Harvey et al. 2001Go; Simons 1995Go).

Features extracted by whisking might be uniquely identified by coincident contact of multiple whiskers with an object as it sweeps across the two-dimensional vibrissa array. Such coincidence detection in the PMBSF would require a highly accurate temporal relationship between vibrissa displacement and cortical response, which has been clearly indicated by single-unit studies of single and multiple vibrissa stimulation (Ego-Stengel et al. 2005Go; Sachdev et al. 2001Go; Shimegi et al. 1999Go, 2000Go; Simons 1985Go; Simons and Carvell 1989Go). In addition, we recently demonstrated temporal fidelity in field potentials recorded with epipial electrode arrays placed on the surface of the PMBSF (Barth 2003Go; Benison et al. 2006Go). The precise timing of field potentials across the PMBSF permits classification and reconstruction of object orientation and shape based solely on submillisecond timing patterns in the barrels (Benison et al. 2006Go). Of particular interest are very fast oscillations (FOs, about 350 Hz) that accompany the classic field potential slow wave in somatosensory cortex (Barth 2003Go; Jones and Barth 1999aGo; Jones et al. 2000Go; Kandel and Buzsaki 1997Go; Staba et al. 2003Go, 2004Go, 2005Go) because these have been shown to exhibit phase-sensitive interactions between barrels with submillisecond precision and exert a strong influence on the probability of cell firing (Barth 2003Go).

However, there were several limitations of our previous study of multivibrissa interactions (Benison et al. 2006Go) based mainly on the stimulus paradigm used. First, only five vibrissae aligned dorsoventrally ("arc") were stimulated, providing no insight into how spatiotemporal information may be integrated between arcs. Second, the stimulus consisted of a straight edge rotating on a smooth drum. The vibrissae could not be placed individually on the drum to record their separate responses and then replaced in the same location as a group to examine multivibrissa responses. Thus we could not estimate supralinear and sublinear responses in this study because we could not obtain an accurate linear model for comparison (i.e., a model constructed from the linear combination of single vibrissa responses). Finally, slight misalignment of the vibrissae on the x-axis (axis of rotation) resulted in asynchronous contact even for upright edges (which should simultaneously strike an arc of vibrissae). This misalignment may have had the effect of obscuring the potential impact of simultaneous stimuli (coincidence detection) while at the same time potentially masking distinct phase-sensitive interactions of FO.

The purpose of the present study was to examine the possible role of coincidence detection in identifying stimulus features in the PMBSF. Stimuli consisted of precisely timed displacement of groups of five vibrissae aligned in an arc, rostrocaudally ("row"), or along a diagonal. The timing of vibrissa stimulation was under independent computer control and set to simulate the vibrissae moving at a physiologically realistic speed and contacting a straight edge of various angular orientations, producing either simultaneous or varying degrees of asynchronous displacements. To identify preferred stimuli, we recorded population field potentials from the entire PMBSF with high-resolution arrays of epipially placed electrodes and examined possible supra- and sublinear responses as a function of simulated stimulus angle. FO and slow-wave responses were analyzed separately to obtain information about their potentially unique contribution to coincidence detection.


 METHODS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
Animals and surgery

All procedures were conducted within the guidelines established by the University of Colorado Institutional Animal Care and Use Committee. Adult male Sprague–Dawley rats (n = 4, 250–400 g) were anesthetized to surgical levels using an intraperitoneal injection of urethane (1.25 g/kg body weight) and a mixture of xylazine (14 mg/kg) and acepromazine (2.3 mg/kg). Animals were placed on a regulated heating pad to maintain normal body temperature (37°C). Anesthesia levels were maintained throughout the experiment so that the corneal and flexor withdrawal reflexes could barely be elicited. A unilateral craniotomy was performed over the right hemisphere extending from bregma to lambda and from the midsagittal suture to the lateral aspect of the temporal bone, exposing a wide region of the parietotemporal cortex. The dura was reflected and the exposed cortex regularly doused with Ringer solution containing (in mM): NaCl 135, KCl 3, MgCl 2, and CaCl 2, pH 7.4 at 37°C. At the conclusion of the experiment, animals were killed by anesthesia overdose without ever regaining consciousness.

Stimulation

Vibrissae on the left mystacial pad were trimmed to 2 cm and displaced about 300 µm (0.1 ms in duration, 1-s interstimulus interval) by inserting them into the ends of 6-cm stainless steel hypodermic tubes attached to laboratory-built solenoids (Barth 2003Go; Jones and Barth 1999bGo). Prior calibration of vibrissa displacement produced by these solenoids revealed no notable afteroscillations at the latency or frequency of fast or slow evoked potential components reported here (Barth 2003Go). Three groups of five vibrissae were studied (Fig. 2), forming a single arc (A3–E3), diagonal (A1–E5), or row (C1–C5). Within each group, the timing of sequential pulses delivered to the five solenoids simulated a straight edge moving at 0.2 mm/ms, to approximate natural whisking velocities observed in behaving animals (Sachdev et al. 2001Go). Simulated angles for each group were referenced to 0°, which represented a straight edge simultaneously striking the five vibrissae in a direction perpendicular to their axis of orientation (i.e., moving in the caudal, dorsocaudal, or dorsal direction for the arc, diagonal, or row, respectively). The timing of sequential vibrissa displacement was computed to simulate angles of ±45, 30, 20, 10, 5, 1, and 0° in one experimental condition and angles of ±6, 5, 4, 3, 2, 1, and 0° in a second condition, to obtain finer spatial and temporal resolution. Because the velocity of the simulated straight edge was 0.2 mm/ms, this resulted in delays between adjacent vibrissae of 25, 14.4, 9.1, 4.4, 2.18, and 0.44 ms in the first condition and 2.63. 2.18, 1.75, 1.31, 0.87, and 0.44 ms in the second condition. For example, a +45° straight edge moving caudally through the arc of vibrissae was simulated by displacing vibrissa E3 first, followed at 25-ms intervals by D3, C3, B3, and A3. An opposite A3–E3 sequence simulated –45°. Lead vibrissae for positive angles in the diagonal and row were E5 and C5, respectively.


Figure 2
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FIG. 2. Maps of power for slow waves (1–100 Hz) and fast oscillations (FOs; 250–1,000 Hz) for the different vibrissa groups. A: power was computed as the root-mean-squared (RMS) amplitude of digitally filtered SEPs, averaged across animals and mapped as a function of stimulation angle (±45° range) separately for the Arc (A3–E3, top row), Diagonal (A1–E5, middle row), and Row (C1–C5, bottom row) vibrissa groups. In all 3 groups, slow-wave power was largest throughout the array at 0°, with significant (P ≤ 0.05) supralinear responses (white dots) in electrodes adjacent to the principal barrels (black circles). Supralinear responses were also recorded from several electrodes during asynchronous stimulation at –1 and +1–10° for arc, –1 and +1 and +10° for diagonal, and –1° for row stimulation groups. However, RMS power declined rapidly with intervibrissa delays >2 ms and approached half-peak amplitude at angles of ±5° in all groups. At greater angles, sublinear responses (black dots) predominated. At greater angles, a pattern emerged where the response of the initial vibrissa contacted (i.e., A3 for –45° or E3 for +45° of the arc) to be largest, with marked suppression of subsequently displaced vibrissae. B: same as A, but showing maps for a ±6° range of angles in 1° increments. In all vibrissa groups, supralinear responses were confined to a window of several degrees flanking 0°. Sublinear responses at angles > ±1° were particularly notable during row stimulation. C: compared with the slow wave, FO power was more constrained to the principal barrels for each group. Significant supralinear responses were most pronounced throughout the array during 0° stimulation of arcs and rows, but were also present during diagonal vibrissa stimulation. Similar to the slow wave, sublinear responses predominated with angles > ±5°. D: however, in contrast to the slow wave, FO declined with angle much more sharply, reaching half-peak amplitude (compared with the maximum 0° response) at ±2°. As noted in the example of Fig. 3, FO power displayed a phase sensitivity in all vibrissa groups, approaching minima at ±3–4°, where the 1.31- to 1.75-ms intervibrissa delays are close to the 1.45 ms required to bring FO out of phase between barrels. In all groups, FO amplitude began to recover at ±6° with 2.63-ms intervibrissa delay, close to the 2.9-ms delay required to bring FO fully back into phase.

 
Evoked potential recording

Epipial maps of the vibrissa-evoked SEP (somatosensory-evoked potential) complex were recorded using a flat multichannel electrode array consisting of 64 silver wires arranged in a 8 x 8 grid (tip diameter: 100 µm; interelectrode spacing: 500 µm) covering a 3.5 x 3.5-mm area of the cortical surface in a single placement. Surface field potentials were referenced to a silver ball electrode secured over the contralateral frontal bone, amplified (x1,000), analog filtered (band-pass cutoff = –6 dB at 1 to 3,000 Hz, rolloff = 5 dB/octave), and digitized at 10 kHz.

Data collection and analysis

At the outset of each experiment, SEPs evoked by individually stimulating each of 25 macrovibrissae (arcs 1–5 and rows A–E) were averaged (n = 100; duration = 500 ms). Bicubic spline interpolated maps of the initial positive SEP deflection (Fig. 1C), representing the most focal response before intracortical spread (Fig. 1B, inset), were computed for all 25 single vibrissa responses and the array positioned such that these maps were aligned across animals; xy coordinates for all 25 single vibrissa response maxima were logged and averaged across animals. Average loci were used to construct a template of the PMBSF for subsequent illustration (Fig. 1, D and E).


Figure 1
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FIG. 1. Somatosensory-evoked potential (SEP) slow waves evoked by multivibrissa stimulation of the A3–E3 arc. A: 25 macrovibrissae form an approximately square array on the mystacial pad consisting of 5 arcs labeled 1–5 on the caudorostral axis and 5 rows labeled A–E on the dorsoventral axis. Stimulated vibrissa C3 is marked with a blue dot in this example. B: displacement of C3 results in an SEP slow wave of largest amplitude in 4 electrodes of the 8 x 8 electrode epipial recording array. Single vibrissa slow wave always consisted of a positive/negative/positive series of amplitude peaks, labeled P1/N1/P2 to indicate their polarity and sequence of occurrence (inset). C: initial positive deflection (inset) was mapped across the array using bicubic spline interpolation and the locus of maximum amplitude used to locate the underlying principal barrel (C3 in this example). This procedure was repeated for the remaining 24 vibrissa. xy coordinates of the 25 barrels derived from single vibrissa SEPs were averaged across animals to form a template of the posteromedial barrel subfield (PMBSF) for subsequent illustration (D and E; circles). D: in this example, a straight edge canted at –45° from the dorsoventral axis of the arc and moving caudally at a velocity of 0.2 mm/ms was simulated. An edge at this angle would strike the A3 vibrissa first and then B3–E3 in sequence, with an intervibrissa delay of 25 ms (based on the assumption of a 5-mm separation between vibrissae). Evoked response (blue traces) and linear model (red traces) revealed multiple slow waves, reflecting sequential deflection of the vibrissae. Earliest response was from an electrode near the principal barrel for A3 (enlarged in a) with an initial slow wave (blue trace, arrow) that closely matched the linear model (red trace, "="). Subsequent slow waves were also recorded at this site, reflecting the 25-ms interval between displacements of adjacent vibrissae in the arc. These were notably attenuated and sublinear ("–") compared with the model, as were later slow waves such as those recorded from a electrode near vibrissa/barrel D3 (b). E: stimuli simulating a 0° straight edge involved simultaneous stimulation of all 5 vibrissae, resulting in a simplification of SEP morphology to a triphasic P1/N1/P2 form. Enlargements of traces near barrels B3 (a) and E3 (b) indicate that the P1 was sublinear ("–"), whereas both the N1 and P2 were supralinear ("+"). Supralinearity was common for simultaneous or near-simultaneous vibrissa stimulation and was typically largest at electrode sites adjacent to the principal barrels for a given group (i.e., c and d).

 
For each vibrissa group (arc, diagonal, or row) and condition (±45 or ±6° angle ranges), 100 trials (500 ms) were randomly sampled at each of the 13 simulated angles and later sorted and averaged. Data were analyzed separately for the slow-wave (1- to 100-Hz digital band-pass) or fast oscillatory (FO; 250- to 1,000-Hz digital band-pass) components. Digital filtering was performed forward and backward in time to eliminate phase shifts using a second-order Butterworth response to minimize the possibility of ringing that could contaminate FO. Interpolated maps of root-mean-squared (RMS) power in the slow-wave or FO frequency bands were plotted as a function of simulated stimulus angle. A linear model of SEPs for each angle was also computed by summing the appropriately time-shifted SEPs (based on the sequential intervibrissa delays used for simulation) obtained from the separate principal vibrissae for a given group (i.e., single vibrissae SEPs for A3–E3 during the arc condition). RMS power at each electrode was compared with the linear model and tested for significant supra- or sublinear responses using paired t-tests with significance set to P ≤ 0.05. RMS power within the slow-wave and FO frequency bands was also averaged across the electrode array and plotted as a function of stimulus angle. Because power consistently declined with deviations from 0° (simultaneous) stimulation, the angles at which power dropped to half-amplitude were determined for each condition and frequency band and tested for significant differences, again using paired t-tests with significance set to P ≤ 0.05. Results are reported as means (±SE) unless otherwise noted.


 RESULTS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
The 25 macrovibrissae form a 5 x 5 array, with arcs typically labeled 1–5 on the caudorostral axis and rows labeled A–E on the dorsoventral axis (Fig. 1A). The somatotopic representation of these vibrissae in the contralateral PMBSF consists of a similar array of distinct cellular aggregates with a similar caudorostral organization of the vibrissa arcs but an inverted dorsoventral organization of the rows. The 8 x 8 epipial electrode array was consistently aligned to the PMBSF across animals using SEPs evoked by stimulating each of the 25 vibrissae separately. For example, stimulation of the C3 vibrissa (Fig. 1A, blue dot) evoked a typical positive/negative/positive slow wave of maximum amplitude at its corresponding barrel (Fig. 1B, labeled P1/N1/P2 in the inset to reflect the polarity and sequence of the temporal components). The earliest visually identifiable positive deflection at the rising phase of the P1 (Fig. 1B, inset) yielded the most focal interpolated amplitude maps (Fig. 1C) preceding intracortical spread. These maps were used to locate each barrel in the PMBSF based on locus of maximum response. Loci of barrels within the PMBSF, determined from single-vibrissa SEPs, were averaged across animals (SE = 0.19 mm; n = 4) and used as a template for further illustration (Fig. 1, D and E).

Sequential stimulation of a vibrissa arc (A3–E3), starting with vibrissa A3 and an intervibrissa delay of 25 ms (simulating a straight edge set at 45° from vertical and moving caudally at 0.2 mm/ms with a 5-mm intervibrissa separation on the rostrocaudal and dorsoventral axis), produced multiple slow waves in the SEP (Fig. 1D, blue traces). The earliest response recorded from an electrode near barrel A3 (Fig. 1Da, arrow) was followed by several additional lower-amplitude slow waves separated by the 25-ms intervibrissa stimulus interval. The SEP slow waves recorded near vibrissa D3 were largest in amplitude at the latency of D3 stimulation (Fig. 1Db, arrow) but were also present in lower amplitude during preceding and subsequent vibrissa stimulation in the sequence. A notable feature of the asynchronous SEP was marked attenuation of sharp wave amplitude following response to the first (A3) vibrissa deflection (Fig. 1D, a and b). To quantify this attenuation, a linear model (Fig. 1D, red traces) was computed for comparison. The linear model consisted of the sum of appropriately time-shifted single-vibrissa SEPs (recorded separately for isolated deflections of vibrissae A3–E3). Only the initial slow wave produced by A3 matched the linear model (Fig. 1Da, "="). Subsequent slow waves throughout the array were attenuated to roughly 50% of the linear model (Fig. 1D, a and b, "–"). Simultaneous stimulation of vibrissae A3–E3, simulating an upright straight edge at 0° to the orientation of the arc, produced a simpler SEP morphology that was similar to the P1/N1/P2 slow wave evoked by single-vibrissa stimulation but spread across the principal vibrissa barrels (Fig. 1E, blue traces). However, the evoked response still differed from the linear model (Fig. 1E, red traces). The initial P1 was typically sublinear (Fig. 1E, a and b, "–"), whereas the N1 and subsequent P2 were typically supralinear (Fig. 1E, a and b, "+"). Supralinear responses were particularly evident at electrode sites surrounding the principal vibrissae (Fig. 1E, c and d).

Maps of slow-wave power, averaged across animals at all electrode sites during arc stimulation, indicated maximum responses with simultaneous (0°) or near-simultaneous (±1°) vibrissa deflections (Fig. 2A, top row). Significant supralinear responses (Fig. 2A, top row, white dots; P ≤ 0.05) occurred at electrode sites immediately surrounding areas of maximum response during simultaneous 0° stimulation and with 0.44-ms interbarrel delays simulating ±1°. Several electrodes near barrel E3 showed supralinear responses at interbarrel delays as long as 4.4 ms (+10°), although, at this and longer interbarrel delays extending to 25 ms (±45°), the predominant response was attenuated and typically sublinear (Fig. 2A, top row: black dots; P ≤ 0.05). Stimulation of the A1–E5 diagonal (Fig. 2A, middle row) and C1–C5 row (Fig. 2A, bottom row) yielded similar results, with a window of about ±0.4-ms interbarrel delay (±1°) where simultaneous and near-simultaneous stimulation produced maximum and usually supralinear responses at electrode sites on and flanking the principal barrels. Outside this window (±5–45° or ±2.18–25 ms), responses were considerably attenuated and sublinear at most sites. Stimulation simulating a straight edge ranging from –6 to +6° in 1° increments (±2.63-ms interbarrel delays in 0.44-ms increments) provided a more precise view of changes in sharp wave power with small changes in interbarrel delays (Fig. 2B). In all three stimulation conditions (arc, diagonal, and row), the largest slow-wave responses occurred during simultaneous stimulation (0°) and were supralinear in electrodes adjacent to the maximum response. Arc and diagonal stimulation (Fig. 2B, top and middle rows, respectively) also produced large and often supralinear responses at interbarrel delays ≤1.75 ms (diagonal) and 2.63 ms (arc) that corresponded to 4 and 6°, respectively. Responses during row stimulation differed in that supralinear responses were confined almost entirely to simultaneous (0°) stimulation with attenuation and sublinear responses becoming apparent at interbarrel delays of ±0.87–1.31 ms (±2–3°).

As depicted in the example of Fig. 1E, when supralinear responses were evoked, they were confined to the N1 and P2. In all animals, the P1 was either linear or sublinear. This effect is depicted again in Fig. 3A, displaying wideband (1–1,000 Hz) SEPs from an electrode site near barrel C3 during ±6° stimulation of the arc in one animal. In this example, the P1 was sublinear and the N1 was slightly supralinear at all angles. However, close examination of the P1 during simultaneous stimulation (0°) revealed small, high-frequency FOs superimposed on this component and on the falling limb of the N1 (Fig. 3C). In this example, FOs in the wideband trace consisted of slight rises and dips just preceding and following the crest of the P1 that were aligned with successive FO waves in the 250- to 1,000-Hz filtered trace (Fig. 3C; Composite). FO bursts of similar latency relative to the P1 were recorded in all animals, with an average period of 2.9 ± 0.3 ms (or 345 ± 38 Hz). Interbarrel delays in the range of ±2.63 ms produced by ±6° stimulation in this example would be expected to bring FO out and then almost back into phase because the half-period (180° out of phase) was 1.45 ms. FOs did indeed demonstrate a marked phase sensitivity (Fig. 3B), with the largest and supralinear responses at 0 and +1° (0.44 ms), minimum responses at ±3–4° (±1.31–1.75 ms), and partial recovery of amplitude at ±6° (±2.63 ms). Full in-phase recovery would not be expected until a delay of 2.9 ms, which was not examined here.


Figure 3
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FIG. 3. Phase-sensitive interactions of FOs (about 350 Hz) superimposed on the initial P1 slow wave. A: wide-band (1–1,000 Hz) SEPs from an electrode site near barrel C3 during a ±6° range of arc stimulation in one animal. At all angles, the P1 of the evoked slow wave (blue traces) was less than the linear model (red traces), whereas the N1 was supralinear. Wide-band filtering revealed FO superimposed on the P1 and beginning of the N1, particularly evident at 0° stimulation (see C). B: in contrast to the P1, which was sublinear at all angles, superimposed FOs were maximum and supralinear at 0 and +1°. FO also displayed distinct phase-sensitive interactions corresponding to submillisecond changes in intervibrissa delays. At ±3–4°, intervibrissa delays were 1.31–1.75 ms, which was close to half the period (1.45 ms in this example) required to bring FO exactly out of phase. These angles produced minimum amplitude FO, with partial recovery of amplitude at ±6° (±6.6° stimulation would be required to produce the 2.9-ms intervibrissa delays required to bring FO fully back into phase). C: black trace depicts essentially unfiltered data (1–3,000 Hz) from the 0° stimulation condition. Blue trace beneath this shows the same data filtered for 1–250 Hz, providing an estimation of what the P1 would look like without FO. Below this, the 2 traces are superimposed as a composite to better examine deviations of FO waves about the slow wave. To highlight these deviations, they are filled in with either red or green, depending on their polarity. Below this is a difference waveform computed by subtracting the slow waveform from the wide-band one. This shows clear FO, also colored alternatively with red and green for comparison to the composite. Area under each FO wave in the difference waveform is (by the way it was computed) exactly the same as the respective colored areas on the composite drawing. Finally, the red trace at the bottom shows 250–1,000 band-pass–filtered data used for subsequent analysis of FO, which is exactly the same as the difference waveform and reveals no filter artifact.

 
Compared with the slow wave, averaged power maps of FOs indicated that they were consistently more confined to the principal barrels in all stimulation conditions (Fig. 2, C and D). During asynchronous stimulation at ±45° (Fig. 2C), FO amplitude dropped rapidly at angles of ±1° (interbarrel delays of ±0.44 ms) with supralinear responses (Fig. 2C, white dots; P ≤ 0.05) largely confined to this temporal window. As with the slow-wave, attenuated and sublinear responses predominated at angles > ±5° (2.18 ms; Fig. 2C; black dots; P ≤ 0.05). Similar to the example of Fig. 3, submillisecond phase sensitivity was apparent in the power maps when smaller 1° (0.44-ms) angular increments were simulated (Fig. 2D). The largest FO responses were evoked by 0° (simultaneous) and ±1° angles (±0.44 ms), reached a minimum at ±3–4° (±1.31–1.75 ms), and appeared to be recovering amplitude at ±6° (±2.63 ms). Supralinear responses were most prevalent during simultaneous or near-simultaneous stimulation (however, note +2 to +5° conditions during both arc and row stimulation, where supralinear responses appear to cluster around the earliest vibrissa contacted).

Power was averaged across all 64 electrodes in the array to simplify direct comparison of changes in FO and slow-wave amplitude as a function of simulated stimulus angle and interbarrel delay (Fig. 4). With a range of ±45° stimulation, FO displayed the steepest decline in power with increasing angle (Fig. 4A, red traces). The total angular window widths (symmetrical about 0°) at which FO amplitude had dropped to half-peak amplitude were 5.59 ± 0.25, 6.91 ± 0.94, and 3.5 ± 0.1° for arc, diagonal, and row stimulation, respectively (Fig. 4A, light red traces). Half-amplitude angular windows for FO were significantly narrower for the row versus arc stimulation conditions (P = 0.011), and the grand average across conditions was 5.3 ± 0.2° (Fig. 4A, dark red trace). The half-amplitude angular window computed for the sharp wave was consistently broader than FO, averaging 15.9 ± 0.46° (Fig. 4A, dark blue trace) and equaling 19.3 ± 1, 17.45 ± 2, and 11.18 ± 0.71° for arc, diagonal, and row stimulation, respectively. Again, row stimulation produced a significantly smaller angular window than the arc (P = 0.002). The more rapid decline of FO with stimulation angle compared with the slow wave was significant across conditions (P < 0.00003) as it was for the separate arc, diagonal, and row conditions (P values of 0.005, 0.019, and 0.006, respectively).


Figure 4
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FIG. 4. Comparison of FO and slow-wave power as a function of stimulus angle. A: total power was estimated by averaging RMS amplitude in the FO or slow-wave frequency bands (1–100 and 250–1,000 Hz, respectively) across all electrodes in the array. In all 3 stimulus conditions, FO power (separate vibrissa groups = thin red traces; average across groups = thick red trace) fell to half-maximum amplitude by ±2–3°, yielding an average "half-amplitude window" of 5.3° or 2.3-ms intervibrissa delay. This was one third the half-amplitude angle of the slow wave (separate vibrissa groups = thin blue traces; average across groups = thick blue trace) at 15.9° or 7-ms intervibrissa delay. B: FOs maintained this higher temporal resolution when examined in the ±6° angular range. Here, the half-amplitude window for FO was 2.69° (1.18-ms delay) compared with 6.33° (2.6-ms delay) for the slow wave. Submillisecond phase sensitivity is still notable in total FO power, with minima separated by the average FO period of 2.9 ms, when FO would be expected to be out of phase between barrels, and a partial recovery at ±6° (2.63-ms intervibrissa delay) as the FO come back into phase between barrels. Submillisecond phase sensitivity was not observed in slow wave power for any of the vibrissa groups.

 
Similar differences between FO and slow-wave amplitude were observed when finer 1° changes in stimulus angle were examined (Fig. 4B). Here, the half-amplitude angular width of FO (Fig. 4B, dark red trace) averaged 2.69 ± 0.06°, which was significantly smaller (P = 0.000015) than 6.33 ± 0.15° for the slow wave (Fig. 4B, dark blue trace). Angular widths of FO and slow wave for the arc, diagonal, and row stimulation conditions were 2.8 ± 0.12, 3.1 ± 0.22, 2.1 ± 0.19, and 6.5 ± 0.45, 7.3 ± 0.61, 5.1 ± 0.35, respectively, with FO (Fig. 4B, light red traces) significantly smaller than the slow wave (Fig. 4B, light blue traces) in each condition (P values of 0.007, 0.009, and 0.031, respectively). No significant differences in half-amplitude angle widths were observed between conditions within the FO or slow-wave frequency bands when examined separately. As in the example of Fig. 3, FO power appeared to reach a minimum in all animals at ±3–4° and begin to recover at ±6°. The spacing of interbarrel delays between the FO minima was close to the average FO period of 2.9 ms.


 DISCUSSION
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
Sublinear responses, feedforward inhibition, and temporal integration

Temporal integration in somatosensory cortex is shaped largely by inhibition. Slow- or long-latency inhibition (Connors et al. 1988Go) corresponds to a long period (50–100 ms) of maximum response suppression in somatosensory cortex noted in paired stimulus paradigms (Gardner and Costanzo 1980Go; Hellweg et al. 1977Go; Mountcastle et al. 1957Go; Shimegi et al. 1999Go; Simons 1985Go; Simons and Carvell 1989Go; Steriade 1984Go; Steriade et al. 1979Go), exceeding all but the maximum intervibrissa delays examined in the present study. Our data indicate a more rapid decline in cortical responsiveness, most pronounced at intervibrissa delays of 10–15 ms, that is most likely attributable to fast feedforward inhibition (Connors et al. 1988Go). This conclusion is supported by observation that the onset of rapid suppression is typically delayed in the PMBSF by application of the {gamma}-aminobutyric acid type A (GABAA) blocker bicuculline (Berger and Luscher 2003Go). Unit studies of paired vibrissa stimulation in rats, typically reveal a time-dependent suppression after initial stimulation that is maximum at about 10–20 ms (Shimegi et al. 1999Go; Simons 1985Go; Simons and Carvell 1989Go), similar to intervibrissa delays yielding minimum responses in the present study. Feedforward inhibition is also typically more widely distributed than excitation, consistent with the widespread suppression and significant sublinear responses observed for simulated stimulus angles > ±10° in the present results. Finally, recent evidence combining direct cortical responses to electrical stimulation with subsequent vibrissa stimulation suggests that intracortical inhibitory pathways play a minimal role in interbarrel-suppressive effects, and that either widespread thalamocortical feedforward inhibition or intrathalamic inhibition may be involved (Civillico and Contreras 2005Go, 2006Go). There is compelling evidence that rapid feedforward inhibition results from monosynaptic thalamocortical input to inhibitory interneurons, in tandem with excitatory input to the pyramidal cells, establishing a brief window of excitability before inhibitory suppression (Gabernet et al. 2005Go; Sun et al. 2006Go; Swadlow 2003Go, 2002Go). Such a narrow window of excitability would suggest that pyramidal cells are maximally responsive to closely timed excitatory inputs in that only these stimuli would be given a chance to bring cells to threshold. Supporting this conclusion are unit recordings indicating that regular spiking units (RSUs, probably pyramidal cells) show peak facilitation with simultaneous multivibrissa stimulation (Shimegi et al. 1999Go) and drop off rapidly in response amplitude with increases in intervibrissa delays greater than a couple of milliseconds, similar to the rapid decline of both FO and slow-wave power in the present study.

Supralinear responses, excitation, and temporal integration

Within the brief window of excitation imposed by feedforward inhibition, our data indicate that short intervibrissa delays (<2 ms) produce significant supralinear responses in wide areas of the PMBSF for both slow-wave and FO power measurements. These results are in agreement with a number of unit studies demonstrating response facilitation with closely timed stimuli (Ego-Stengel et al. 2005Go; Erchova et al. 2003Go; Ghazanfar and Nicolelis 1997Go; Shimegi et al. 1999Go, 2000Go). It is thus puzzling why several unit studies of the spatiotemporal dynamics of multivibrissa stimulation report a predominance of suppressive interactions even with short (0- to 5-ms) intervibrissa delays (Mirabella et al. 2001Go; Simons 1985Go; Simons and Carvell 1989Go). As noted by Simons and coworkers (Simons 1985Go), one explanation may be that the failure to find supralinear responses to simultaneous vibrissa deflections reflects a ceiling effect produced by occlusion of multiple inputs to maximally activated neural pools. In studies where multivibrissa stimulation at short intervals do not produce supralinear responses, there is usually a dramatic recovery from sublinearity with decreasing delay, approaching a linear or barely sublinear response with simultaneous stimuli (Mirabella et al. 2001Go; Simons 1985Go; Simons and Carvell 1989Go). This finding is consistent with increased excitation or less inhibition resulting from closely timed stimuli, even if the net effect is not a supralinear response.

We also reported a ceiling effect arising from maximum depolarization in field potential measurements of excitability cycles in the PMBSF (Barth and Di 1991Go). This may explain why the supralinear responses of the present data are almost exclusively recorded from electrodes surrounding the principal vibrissa barrels for a given stimulation condition (i.e., 0°; Fig. 2A). Responses from sites corresponding to the principal vibrissa barrels typically sum linearly (except, note Fig. 2C; 0°). Similar results, obtained from mapping studies of spatially distributed unit responses in the PMBSF, indicate supralinear summation only in the far surround of a neuron's receptive field and rarely in the center (Ghazanfar and Nicolelis 1997Go). The largest supralinear responses are usually observed in cells that respond weakly or not at all to individual vibrissae but are robustly driven by combined stimulation, suggesting minimum single-vibrissa response levels are most effective for revealing supralinear multivibrissa effects (Ego-Stengel et al. 2005Go; Ghazanfar and Nicolelis 1997Go; Shimegi et al. 1999Go, 2000Go). Interestingly, recent examination of intervibrissa interactions using voltage-sensitive dyes failed to find supralinear responses in the PMBSF to simultaneous vibrissa deflection, except rarely and in the extreme periphery of the principal barrels (Civillico and Contreras 2006Go). One possible explanation for this difference with the present data is that these investigators used paired vibrissa stimulation as opposed to five-vibrissa stimulation of the present study. Facilitative interactions between multiple barrels may be better suited to production of reliable supralinear responses.

Fast oscillations versus slow waves in coincidence detection

Although the brief window of responsiveness in our results is probably shaped in large part by fast inhibition, the angular tuning of FO is significantly narrower than the slow wave, suggesting involvement of an additional mechanism. Unlike the slow wave, angular sensitivity of FOs reveals a periodicity that corresponds to the average frequency of 345 Hz in these animals, suggesting submillisecond phase sensitivity in addition to the inhibitory damping evident for both FO and the slow wave. Because FOs represent the earliest and the most precisely tuned response to simultaneous or near-simultaneous vibrissa displacement, they may serve a primary role in coincidence detection in the PMBSF. The angular tuning of slow waves is roughly threefold wider than that of FO, suggesting a heightened sensitivity to coincident stimuli, yet one that is not further narrowed by the phase sensitivity apparent in FO. It is notable that only the N1 and P2 produce supralinear responses to coincident stimuli; the P1 is typically linear or sublinear, suggesting different functional roles for these temporal components. Laminar field potential studies have demonstrated that the P1 reflects depolarization of the proximal apical dendrites of supragranular (Di et al. 1990Go) and, to a lesser extent, infragranular (Staba et al. 2004Go) pyramidal cells in the PMBSF. Although not registering supralinear responses to simultaneous stimuli, the P1 may reflect establishment of an essential background of common excitation among subgroups of activated barrels, bringing select populations of cells near threshold and facilitating phase-sensitive interbarrel interactions of concurrently recorded FOs. Recent computational models suggest that, under conditions of near-threshold depolarization, even weakly correlated synaptic inputs can dramatically increase discharge probability (Salinas and Sejnowski 2000Go), possibly improving coincidence detection between pyramidal cells of mutually depolarized barrels. Laminar recording of the subsequent N1 in PMBSF indicates depolarization of distal apical dendrites of both supra- and infragranular pyramidal cells (Di et al. 1990Go). Supralinear responses recorded for the N1 and P2 during closely timed stimuli suggest a late phase of coincidence detection distinct from FOs. It cannot be determined from our data whether this is conducted independently of FO or is in fact boosted by preceding discharge of FO-generating neurons. However, the long poststimulus latency and wider spatial distribution of these late components suggest the involvement of multisynaptic pathways for their generation, perhaps serving to distribute the results of coincidence detection performed locally in the principal barrels to wider areas of the PMBSF.

Homogeneity of multivibrissa integration: two-dimensional processing in the barrel field

Anatomical studies show a bias toward interconnectivity between barrels within rows versus arcs in the PMBSF (Bernardo et al. 1990Go; Hoeflinger et al. 1995Go) that may be reflected in elongation of vibrissa-evoked activity patterns along the rows (Armstrong-James and Fox 1987Go; Kleinfeld and Delaney 1996Go; Simons 1978Go). Perhaps for this reason, a number of studies concerned with multivibrissa stimulation have examined integration within barrel rows as opposed to arcs (Goldreich et al. 1998Go; Kleinfeld and Delaney 1996Go; Simons 1985Go). Investigations that have compared multivibrissa stimulation within an arc versus row at short interstimulus intervals variously suggest a tendency toward supra- versus sublinear responses in arcs and rows, respectively (Ego-Stengel et al. 2005Go; Ghazanfar and Nicolelis 1997Go), or sublinear responses in both (Mirabella et al. 2001Go).

A surprising finding of the present experiment is that there is little difference in the spatiotemporal pattern of sub- or supralinear responsiveness in the rows versus arcs, and neither differs from the diagonal group of vibrissa. To our knowledge intradiagonal integration within the PMBSF has not been previously examined. For all three conditions (arc, diagonal, and row), course range (±45°) stimulation yields half-amplitude angular windows averaging 5.3° for FO and 15.9° for the slow wave. Closer examination, with a finer range of stimulation angles (±6°), yields half-amplitude angular windows averaging 2.7 and 6.3° for FO and slow wave, respectively. Whereas the angular windows in both frequency bands are significantly smaller in the rows (FO = 2.1°, slow wave = 5.1°) than in the arcs (FO = 2.8°, slow wave = 6.5°), suggesting a slight improvement of angular tuning in the rows (neither significantly differing from the diagonal), this difference is quite small. Indeed, the most striking result is the similarity in all response characteristics between stimulus conditions. These characteristics include the spatial distribution of responses (relative to the principal barrels), sublinear and supralinear responsiveness with large and small stimulus angles, respectively (intervibrissa delay), and correlated changes in both FO and slow-wave power, suggesting an appreciable absence of direction specificity within the PMBSF. Furthermore, in all experimental conditions, the decline of both FO and slow-wave power with stimulus angle is nearly symmetrical about 0°, indicating that intervibrissa interactions are insensitive to the order in which the vibrissae are stimulated. Field potential mapping was used in the present study to examine the central tendency of population interactions in the entire PMBSF. This central tendency suggests a predominant spatial and temporal homogeneity underlying multivibrissa integration. However, unlike unit recording, field potential recordings may be relatively insensitive to selective activation of subpopulations of cells within or between barrels. Thus our results ignore the potential contributions to spatiotemporal integration of somatotopically organized motion direction maps, recently demonstrated in single- and multiple-unit recordings (Andermann and Moore 2006Go). Proper examination of possible contributions from directionally tuned subpopulations at the subcolumnar level to the present field potential records would require multivibrissae stimulation at a variety of orientations instead of the consistently orthogonal orientation used here.

Coincidence detection and spatial feature analysis

The present experiments were performed in anesthetized rats with passive stimulation. As such, they may be assumed to provide a simplified view of mechanisms underlying spatial feature analysis in the awake behaving animal, where attentional states, whisking strategies, head position, and accompanying interactions between motor and somatosensory cortex all must come into play. However, the sharp angular tuning of population responses recorded here suggests that simultaneous or near-simultaneous displacement of multiple vibrissae may constitute a preferred stimulus in the PMBSF. Responses to asynchronous vibrissa contact, with delays more than a couple of milliseconds, are considerably suppressed. Inhibition has long been thought to enhance both spatial contrast (Laaris et al. 2000Go; London et al. 1989Go; Mountcastle and Powell 1959Go; Petersen et al. 2001Go; Simons 1995Go; Simons and Carvell 1989Go) and temporal contrast (Gabernet et al. 2005Go; Gardner and Costanzo 1980Go; Pinto et al. 2000Go, 2003Go) in somatosensory cortex. Temporal contrast enhancement could serve to improve resolution of asynchronous input by briefly suppressing responses to an initial stimulus in preparation for response to a subsequent one (Gardner and Costanzo 1980Go). In the PMBSF, this would result in an improved resolution of sequentially activated vibrissae within a row when brought in contact with an object during forward extension (Simons 1985Go).

However, our results support an alternative role for temporal contrast enhancement, one in which asynchronous vibrissa contact outside a short time window of several milliseconds is powerfully suppressed in favor of simultaneous or nearly simultaneous contact, producing sharply tuned supralinear responses particularly notable in high-frequency oscillations arising from additional phase sensitivity. In this way, intra- and interbarrel circuitry may serve the function of coincidence detection (Berger and Luscher 2003Go; Gabernet et al. 2005Go; Ghazanfar and Nicolelis 1997Go; Pinto et al. 2000Go, 2003Go; Roy and Alloway 2001Go; Schaefer et al. 2003Go; Shimegi et al. 1999Go, 2000Go; Stuart and Hausser 2001Go; Swadlow 2003Go), favoring inputs with low temporal contrast, and identifying common object features on the basis of simultaneous contact with subgroups of vibrissae (Pinto et al. 2000Go, 2003Go; Shimegi et al. 2000Go). The equivalence of function apparent during arc, diagonal, and row stimulation suggests that the PMBSF may be capable of working as a two-dimensional integrative array, processing spatial features according to common mechanisms despite the direction with which the vibrissae pass across an object. Spatial features, extracted from coincident contacts within two-dimensional vibrissa space, include orientation of straight edges or planes (Shimegi et al. 2000Go), with a potential resolution of 1° as suggested here. However, the same mechanism of coincidence detection should also provide information about object curvature or shape (Benison et al. 2006Go) indicated by behavioral studies of object discrimination in rats (Harvey et al. 2001Go; Polley et al. 2005Go).


 GRANTS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
This research was supported by National Institute of Neurological Disorders and Stroke Grant 1 R01 NS-36981, the Marion Downs Center, and the University of Colorado Undergraduate Research Opportunity Program.


 ACKNOWLEDGMENTS
 
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 GRANTS
 ACKNOWLEDGMENTS
 REFERENCES
 
We thank Dr. Eva Fifkova for the careful review of this manuscript and helpful comments.


 FOOTNOTES
 
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.

Address for reprint requests and other correspondence: D. S. Barth, Department of Psychology, University of Colorado, Campus Box 345, Boulder, CO 80309-0345 (E-mail: dbarth{at}psych.colorado.edu)


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K. M. Rodgers, A. M. Benison, A. Klein, and D. S. Barth
Auditory, Somatosensory, and Multisensory Insular Cortex in the Rat
Cereb Cortex, December 1, 2008; 18(12): 2941 - 2951.
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J. Neurophysiol.Home page
P. J. Drew and D. E. Feldman
Representation of Moving Wavefronts of Whisker Deflection in Rat Somatosensory Cortex
J Neurophysiol, September 1, 2007; 98(3): 1566 - 1580.
[Abstract] [Full Text] [PDF]


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J. Neurophysiol.Home page
A. M. Benison, D. M. Rector, and D. S. Barth
Hemispheric Mapping of Secondary Somatosensory Cortex in the Rat
J Neurophysiol, January 1, 2007; 97(1): 200 - 207.
[Abstract] [Full Text] [PDF]


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