Abstract
Layer V pyramidal cells in rat barrel cortex are considered to play an important role in intracolumnar and transcolumnar signal processing. However, the precise circuitry mediating this processing is still incompletely understood. Here we obtained detailed maps of excitatory and inhibitory synaptic inputs onto the two major layer V pyramidal cell subtypes, intrinsically burst spiking (IB) and regular spiking (RS) cells, using a combination of caged glutamate photolysis, whole-cell patch-clamp recording, and three-dimensional reconstruction of biocytin-labeled cells. To excite presynaptic neurons with laminar specificity, the release of caged glutamate was calibrated and restricted to small areas of 50 × 50 μm in all cortical layers and in at least two neighboring barrel-related columns. IB cells received intracolumnar excitatory input from all layers, with the largest EPSP amplitudes originating from neurons in layers IV and VI. Prominent transcolumnar excitatory inputs were provided by presynaptic neurons also located in layers IV, V, and VI of neighboring columns. Inhibitory inputs were rare. In contrast, RS cells received distinct intracolumnar inhibitory inputs, especially from layers II/III and V. Intracolumnar excitatory inputs to RS cells were prominent from layers II–V, but relatively weak from layer VI. Conspicuous transcolumnar excitatory inputs could be evoked solely in layers IV and V. Our results show that layer V pyramidal cells are synaptically driven by presynaptic neurons located in every layer of the barrel cortex. RS cells seem to be preferentially involved in intracolumnar signal processing, whereas IB cells effectively integrate excitatory inputs across several columns.
Keywords: barrel cortex, layer V, pyramidal cell, burst spiking, regular spiking, functional connectivity, excitatory inputs, inhibitory inputs, morphology, electrophysiology, biocytin, caged glutamate, somatosensory, slices
Cortical information processing is mediated by complex interactions between local neuronal circuits within functional columns involving several classes of excitatory and inhibitory neurons. The barrel field in the primary somatosensory cortex of rodents is a particularly useful model for the investigation of cortical columnar organization and signal processing, because the functional columns can be recognized even in unstained living slices (Agmon and Connors, 1991; Kötter et al., 1998). Here neuronal clusters in layer IV (barrels) are related to principal whiskers on the contralateral side of the face in a one-to-one relationship (Woolsey and Van der Loos, 1970; Welker and Woolsey, 1974). Together with supragranular and infragranular neurons, in register with a barrel, they form a functional (barrel-related) column and respond preferentially to stimulation of the whisker, which is topographically related to the barrel within this column (Armstrong-James, 1975; Simons, 1978). However, substantial signal integration occurs not only within but also between barrel-related columns. Because of the size of their receptive fields, which can comprise a multitude of whiskers (Simons, 1985; Zhu and Connors, 1999), pyramidal cells in supragranular and infragranular layers are considered to play a crucial role in this signal integration (Staiger et al., 2000).
In layer V of the cerebral cortex, two major classes of pyramidal cells have been described: intrinsically burst spiking (IB) and regular spiking (RS) cells (Connors et al., 1982; Chagnac-Amitai et al., 1990; Larkman and Mason, 1990). The thick, tufted IB cells are capable of discharging high-frequency bursts of action potentials and show extensive horizontal axonal projections within infragranular layers and diverse corticofugal projections (Kasper et al., 1994). The dendritically rather sparsely arborizing RS cells discharge more regularly and project extensively to supragranular layers (Chagnac-Amitai et al., 1990) and to ipsilateral and contralateral cortical areas (Wise and Jones, 1976). Extensive synaptic coupling between pyramidal cells within layer V (Markram et al., 1997) and between pyramidal cells in layer II/III and layer V (Reyes and Sakmann, 1999) was demonstrated using paired recordings (Thomson et al., 1993;Thomson and Deuchars, 1994). Moreover, layer V pyramidal cells receive inhibitory inputs from different laminar origins, and the spatial organization of these inputs varies with the class of the pyramidal cell (Nicoll et al., 1996). These findings indicate the existence of complex excitatory and inhibitory inputs modulating the functional status of layer V pyramidal cells. To receive detailed information about the spatial distribution of synaptic inputs, it is necessary to stimulate numerous presynaptic sites covering a sufficiently large cortical area and to construct a synaptic input map for each single cell. Thus we investigated the spatial distribution and strength of excitatory and inhibitory synaptic inputs onto layer V pyramidal cells using a combination of caged glutamate photolysis and whole-cell patch-clamp recordings. Thereby we obtained detailed maps of layer-specific intracolumnar and transcolumnar functional connectivity of electrophysiologically characterized and morphologically reconstructed RS and IB cells that demonstrate a differential involvement of the two cell types in local cortical circuits.
Part of this study was published previously in abstract form (Schubert et al., 2000).
MATERIALS AND METHODS
Slice preparation and chemicals. We prepared coronal slices from rat somatosensory cortex containing the barrel cortex (Par1) (Paxinos and Watson, 1986). Male Wistar rats (postnatal days 18–22) were deeply anesthetized with enflurane and decapitated. Blocks of tissue containing the barrel cortex were excised, quickly removed from the skull, and stored in ice-cold artificial CSF (ACSF) oxygenated with carbogen (95% O2/5% CO2). Normal ACSF consisted of (in mm): 124 NaCl, 1.25 NaH2PO4, 26 NaHCO3, 1.6 CaCl2, 1.8 MgCl2, 3 KCl, 10 glucose, at pH 7.4. To block synaptic transmission, modified ACSF containing 0.2 CaCl2, 4 MgSO4 (low Ca2+/high Mg2+ ACSF) was used. The tissue block was glued to the chilled platform of a Vibratome (Series 1000, TPI, St. Louis, MO) and submerged in ice-cold carbogenated ACSF. Slices of 300 μm nominal thickness were cut and incised along the midline to separate the hemispheres. The slices were stored in an incubation chamber containing carbogenated ACSF at 34°C for at least 1 hr. The slices were then transferred to the recording chamber and submerged in ACSF at a flow rate of ∼1 ml/min at 32°C. During the application of caged glutamate, a total amount of ∼5 ml ACSF containing the caged compound was continuously oxygenated and recirculated. The caged glutamate (l-glutamic acid, γ-[α-carboxy-2-nitrobenzyl]ester; Molecular Probes, Eugene, OR) was dissolved in ACSF and added to the circulating ACSF, resulting in a 1 mm concentration.
Identification of layer V pyramidal neurons. The slices were placed in a fixed stage, submerged chamber under an upright microscope (Axioskop FS, Carl Zeiss, Göttingen, Germany) fitted with a 2.5× and a 40× water-immersed objective (40×/0.75 W; Olympus, Hamburg, Germany). The barrel field was visualized at low magnification (Fig.1), and a target region in layer V, which was in vertical register with a barrel, was selected. Individual pyramidal cells were visually identified at 40× magnification using infrared enhanced quarter-field illumination. A bipolar tungsten stimulating electrode was placed in deep layer VI of the same column.
Electrophysiology. Whole-cell patch-clamp recordings from the selected pyramidal cells were performed in current-clamp mode using patch pipettes (4–6 MΩ) pulled from borosilicate glass capillaries (1.5 mm outer diameter, 1.16 mm inner diameter; Science Products, Hofheim, Germany) on a Narishige PP-830 puller (Narishige, Tokyo, Japan). The patch pipettes were filled with (in mm): 13 KCl, 117 K-gluconate, 10 K-HEPES, 2 Na2ATP, 0.5 NaGTP, 1 CaCl2, 2 MgCl2, 11 EGTA, and 1% biocytin. After obtaining a stable seal of >1 GΩ, the whole-cell configuration was achieved by gentle suction. The cells were electrophysiologically characterized by recording their resting membrane potential and their intrinsic membrane properties under current-clamp conditions by injecting depolarizing and hyperpolarizing current pulses. Orthodromic synaptic responses were elicited with the bipolar stimulating electrode (200 μsec duration at 0.1 Hz). To exclude possible influences of caged glutamate on the properties of the recorded cells, electrophysiological characterization and long time recordings were performed in ACSF alone as well as in ACSF containing caged glutamate. Their results were virtually identical.
Scanning of glutamate evoked activity. The setup that we used for the photolysis of caged glutamate has been described previously (Kötter et al., 1998). However, to implement single-cell recordings, some modifications were necessary. We added a circular linear-wedge neutral-density filter into the light path (Dr = 0.0–2.0) (Melles Griot, Irvine, CA) for the exact calibration of the illumination intensity. The light pulses (∼500 μsec) were focused on areas that were 50 × 50 μm large, with the focus plane ∼50–80 μm deep in the slice, which was equal to the depth of the recorded cell soma. The membrane potential was recorded during every photostimulus. In the beginning of the study, fields at varying distances from a recorded soma were stimulated, always with use of the same stimulation strength. This was done to ensure that the photostimulation provided layer-specific excitation. In ACSF, aside from layer V pyramidal cells (n = 42), other neurons in layers II/III, IV, V and VI also were recorded at the resting membrane potential (Vrmp) of the cells (n= 19). In none of these control experiments could action potentials be elicited by photostimulation at distances >100 μm from the soma. In two of five pyramidal cells in layer II/III, no suprathreshold activation was evoked from any of the tested fields. Every 10 sec the stimulation area was moved in a meandering fashion across a rectangular field for further scanning in steps of 50 μm (Fig. 1). While the synaptic connectivity was mapped, the cell was held at a potential (Vhold) of −60 mV in current-clamp mode to reveal hyperpolarizing inhibitory inputs. As shown in Figure 1, the scanned cortical areas included at least two barrel-related columns from layers I–VI, and thus up to 450 different fields were stimulated without any intermittent gaps. To determine the spatial distribution of glutamate-evoked direct activity in the recorded cell, we blocked synaptic transmission using ACSF containing low Ca2+/high Mg2+. The intrinsic properties of the recorded cell were controlled before and after termination of each map.
Data acquisition and analysis. The signals were amplified (SEC-05L; npi-electronics, Tamm, Germany), filtered at 3 kHz, and digitized using an ITC-16 interface (Instrutech, Great Neck, NY). Data were recorded, stored, and analyzed with PC-based software (TIDA 4.1 for Windows; Heka Electronik, Lambrecht, Germany). After recording, the slices were photographed in the bath chamber to document the topography of barrel-related columns and laminae as well as the respective position of the patch and stimulating electrode. Slices were then fixed in 4% buffered paraformaldehyde and stored at 4°C. For visualization of the biocytin-filled neurons, the slices were processed using a previously described protocol (Angulo et al., 1999). Reconstruction and morphological analyses of the biocytin-labeled neurons were made using a Nikon Eclipse 800 (Nikon, Ratingen, Germany) attached to a computer system (Neurolucida; Microbrightfield Europe, Magdeburg, Germany). IB and RS cells were compared in terms of the following morphological properties: soma area, total length of apical and basal dendrites, total number of branches of the apical dendrite, and the maximal diameter of the apical trunk. The data were not corrected for tissue shrinkage. The reconstructed cells were superimposed onto the photomicrograph of the native slice using standard graphics software.
Different maps of glutamate-induced activity obtained in low Ca2+/high Mg2+ containing ACSF were constructed using (1) flash evoked peak amplitudes and (2) delays between stimulus and onset of activity. For maps in normal ACSF, the following properties of stimulus-induced activity were analyzed within a time window of 150 msec after stimulus for each single trace: (1) delay-to-onset of stimulus-evoked activity, (2) occurrence of IPSPs, (3) maximal peak amplitude, and (4) integral of all EPSPs. Only subthreshold responses with amplitudes of >0.2 mV were included for further analysis. In control experiments using repetitive photostimulation, we additionally analyzed (1) the delay between stimulus and action potential threshold (action potential latency), (2) the peak amplitude of the first EPSP, and (3) 20–80% rise-time of the first EPSP. Spontaneous activity with amplitudes of >0.2 mV was very rare and, when present, was excluded from further analysis. Response properties that were analyzed were transformed into pseudocolored values using the software Origin 6.0 (Microcal Software, Northampton, MA), and the resulting maps were superimposed on the respective sites on the micrographs. Statistical analysis was performed using repeated measures ANOVA with post hocpair-wise comparisons (Bonferroni corrected) and unpaired two-tailed Student's t test (SPSS 9; SPSS Inc., Chicago, IL). Data are presented as mean ± SD.
RESULTS
In the present study, we investigated 55 layer V pyramidal cells in rat barrel cortex. For 27 layer V IB/doublet spiking cells and 28 layer V RS cells, whole-cell patch-clamp recordings were combined with topographic mapping of glutamate-induced activity. Complete maps in ACSF including all cortical layers and at least two barrel-related columns were obtained for seven IB cells and eight RS cells. Partially mapped cells (11 IB cells, 12 RS cells) were used for complementary verification of the results obtained from the completely mapped cells. The remaining cells were used for control experiments (see Materials and Methods). Only cells with a stable resting membrane potential negative to −60 mV during the whole experiment were included in the analysis.
Electrophysiological and morphological identification of RS and IB cells
As indicated by previous studies, layer V pyramidal neurons can be divided into RS and IB cells according to their firing properties, their synaptic input pattern in response to orthodromic stimulation, and their specific morphology (Connors et al., 1982;Chagnac-Amitai et al., 1990; Larkman and Mason, 1990; Amitai, 1994;Williams and Stuart, 1999; Hefti and Smith, 2000). In accordance with these studies, we found that IB cells responded to injection of a just suprathreshold depolarizing current pulse with an initial high-frequency burst consisting of two to three action potentials with decreasing amplitudes mounted on a depolarizing after potential (DAP) (Fig. 2A). This initial burst with a first interspike interval (ISI) of 175 ± 22 Hz (n = 17) was followed either by rhythmic action potential (AP)-firing or by single APs showing longer ISIs. Injection of current pulses with increasing amplitudes did not alter the first ISI but increased the number of action potentials in the initial burst to three to six spikes. In 10 cells, just suprathreshold as well as increased current injections reproducibly induced doublets of APs at a mean first ISI of 152 ± 27 Hz (Fig. 2B). Except for the different response pattern to depolarizing current injection, these doublet spiking cells were indistinguishable from IB cells and showed the same response to orthodromic stimulation and the same morphology. Thus, doublet spiking cells were added to the group of IB cells in accordance with the description by Schwindt et al. (1997). RS cells, however, responded to suprathreshold current injection with a series of single APs (Fig. 2C). In 11 of 28 RS cells, the firing rate became more or less constant after an initial frequency adaptation [comparable to RS1-type in Hefti and Smith (2000)]. In the remaining cells, the firing rate adaptation continued for the duration of the depolarizing current pulse. In 14 of 28 RS cells, APs were followed by a small DAP (comparable to RS2-type). However, rhythmic AP firing or high-frequency bursts/doublets of APs were never observed in RS cells. The average resting membrane potential (Vrmp) and the membrane resistance (Rm) were not significantly different between IB cells (Vrmp = −62.6 ± 3.2 mV; Rm = 133 ± 64 MΩ;n = 27) and RS cells (Vrmp = −63.7 ± 3.7 mV;Rm = 202 ± 124 MΩ;n = 28).
We also used orthodromic synaptic stimulation for a functional characterization of the two cell types. As demonstrated in Figure2D, orthodromic stimulation evoked an EPSP, eliciting a burst of action potentials in IB cells with no visible IPSP. In contrast, in 19 of 28 RS cells, the initial EPSP was followed by a prominent fast and slow IPSP (Fig. 2E). The remaining nine RS cells showed no detectable IPSPs.
All cells were labeled with biocytin for subsequent morphological identification. All completely filled IB and RS cells showed an apical dendrite reaching layer I (n = 25). A quantitative evaluation of cell type-specific morphological properties of reconstructed IB and RS cells is given in Table1. In agreement with the studies mentioned before, large triangular somata and thick apical dendrites were typical features of IB cells (Fig.3A). The apical dendrite usually possessed numerous oblique collateral branches. The main trunk started to bifurcate in layers IV or II/III, giving rise to a rich terminal tuft. The basal dendrites were also extensively ramified. In contrast, RS cells possessed a smaller ovoid soma with a thinner apical trunk and a less ramified apical dendrite (Fig.3B).
Table 1.
IB cells (n = 7) | RS cells (n = 5) | |
---|---|---|
Soma area (μm2) | 377.9 ± 122.7 | 248.7 ± 76.4* |
Total length of basal dendrites (μm) | 3199 ± 1210.5 | 2531.8 ± 811.1 |
Total length of apical dendrite (μm) | 6231.7 ± 3320.6 | 2153.3 ± 684.8** |
Number of branches of apical dendrite | 49.1 ± 27.6 | 23.4 ± 9.6* |
Maximal apical trunk diameter (μm) | 6.3 ± 1.7 | 4.1 ± 1.4* |
Data are mean ± SD; *p < 0.05, **p < 0.01.
Direct effects of uncaged glutamate
To investigate the direct effects of uncaged glutamate on functional properties of the recorded cell, we performed experiments in ACSF containing low Ca2+/high Mg2+ to block synaptic transmission. After 30 min of perfusion with low Ca2+/high Mg2+ ACSF, even strong electrical stimuli were not capable of evoking postsynaptic responses in the recorded neuron (n = 4 IB and 5 RS cells). The photolysis of caged glutamate within a field of tissue containing dendritic extensions of the recorded cell led to a transient depolarization (Fig.4A,B). For both cell types, 20 repetitive flashes at 10 sec intervals on a selected proximal dendritic field revealed a stable pattern of evoked depolarizations. Perisomatic stimulation induced strong depolarizations of 15–20 mV that reliably elicited a single action potential, doublet, or burst in accordance with electrical characterization (Fig.4C,D). However, depending on the size of the depolarization amplitude, short trains of action potentials after the initial response also could be elicited (Dantzker and Callaway, 2000). The delay-to-onset times within distances of ≤100 μm from the soma were <1 msec, and the estimated rise-times were >5 msec. At distances of >500 μm from the soma, the 20–80% rise-times could increase up to 30 msec. Neither the delay-to-onset of activation (Fig.5A) nor the 20–80% rise-times (Fig. 5B) changed significantly during repetitive flash activation. In contrast, the depolarization amplitudes (Fig.5C) and action potential latencies (Fig. 5D) were more variable.
To determine the spatial distribution of the direct glutamate-induced activity under low Ca2+/high Mg2+ conditions, we stimulated 250 fields and converted the depolarization amplitudes or the delay-to-onset of activation into color-coded maps (Fig. 6) (n = 4 IB and 4 RS cells). In the matched figure of the native slice and the reconstructed cell, each colored square indicates the location of a stimulated field of tissue where a depolarizing response was evoked. Figure 6 illustrates the spatial distribution of the glutamate-induced activity for an IB cell. Membrane depolarizations were observed only in fields containing dendritic extensions of the recorded cell. Highest response amplitudes were induced at perisomatic locations and along the proximal dendrites; lowest response amplitudes were induced at peripheral locations of the basal dendrites and at distal parts of the apical dendrite. Action potentials were evoked only by flashing fields very close to the soma. The delay-to-onset of activation (Fig. 6B) and the rise-time (20–80%; data not shown) directly correlated with the distance of the flashed field to the recording site. The stimulation of fields at or near the soma caused an almost immediate depolarization (Fig.6D3). Longer delay-to-onset times were observed by flashing the apical tuft near the pial surface (Fig.6D1). A linear regression of the data resulted in the calculation of an average electrotonic propagation velocity of 0.26 m/sec along the dendrites (Fig. 6E).
Characterization of synaptically evoked inputs onto layer V pyramidal cells
In experiments performed in normal ACSF, the uncaged glutamate was able to induce (1) activity resulting from direct stimulation of dendritic extensions of the recorded cell and (2) EPSPs and IPSPs after activation of presynaptic excitatory and inhibitory neurons, respectively. Repetitive stimulation of selected sites was used to characterize the properties of synaptically evoked activity (n = 4 RS and 4 IB cells). As demonstrated in Figure7, the recorded IB cell received distinct excitatory and inhibitory synaptic inputs from presynaptically activated neurons. Repetitive stimulation of some fields reliably elicited IPSPs with stable rise-time and delay-to-onset time (Fig. 7A). However, the amplitude of the IPSPs varied from trial to trial. In other fields, unlike the IPSPs, EPSPs were initiated during repetitive stimulation, with a failure rate of 5–40% (as at site 2), but with relatively stable amplitudes and rise-times (Fig. 7B). The delay-to-onset times of the EPSPs varied between 5 and 50 msec. Furthermore, the flash often evoked two or multiple EPSPs. As under low Ca2+/high Mg2+ conditions, perisomatic stimulation reliably elicited an action potential (Fig. 7C).
Figure 8A shows recordings of two populations of EPSPs after repetitive stimulation at the same site. The two populations varied not only in their delay to onset but also in their order of appearance (Fig.8A,B). However, the two populations differed significantly in their mean amplitudes (EPSP1: 2.9 ± 0.2 mV; EPSP2: 1.3 ± 0.2 mV; n = 15;p < 0.001, t test), integrals (EPSP1: 0.03 ± 0.005 mVs; EPSP2: 0.012 ± 0.004 mVs;p < 0.001), and rise-times (EPSP1: 1.1 ± 0.1 msec; EPSP2: 1.6 ± 0.2 msec; p < 0.001). Therefore, these parameters could be used to distinguish between the EPSPs (Fig. 8C,D). Consequently, the delay-to-onset times could not be used as an indicator for the site of the synaptic input onto the recorded cell.
Intracortical inputs onto layer V pyramidal cells
For the topographic mapping of the functional connectivity we stimulated 450 different fields of 50 × 50 μm in size comprising an area of all six cortical layers and two or more neighboring barrel-related columns. Stimulation of fields containing dendritic extensions of the recorded cells often resulted in a mixture of direct nonsynaptic activation and synaptic events. Therefore it was necessary to separate the direct nonsynaptic responses from the synaptically evoked activity to obtain “pure” synaptic input maps. Figure 9 shows the spatial distribution of evoked responses recorded in low Ca2+/high Mg2+ ACSF (Fig. 9A) as well as in normal ACSF (Fig. 9B) for an IB cell. Direct nonsynaptic responses recorded in low Ca2+/high Mg2+ ACSF reached the soma within 8 msec (Fig. 9C, top panel). In normal ACSF, we always observed a comparable amount of evoked events within the first 8 msec (Fig. 9C, bottom panel). The remaining events were recorded with delay-to-onset times of >11 msec. In accordance with the morphology of the cell, all responses with delay-to-onsets ≤8 msec could be related to direct nonsynaptic activation of the dendritic extensions (Fig.9B,D). Therefore, we could construct maps specifically showing synaptic inputs to the recorded cells (Fig. 9B). Aside from various subthreshold events, several sites were found to induce action potentials >100 μm away from the soma. This is explained by the fact that during mapping the recorded cells were depolarized by up to 10 mV to reachVhold = −60 mV. Control stimulations of the respective fields after mapping atVrmp never evoked APs (data not shown).
Typical spatial distribution and strength of synaptic inputs onto an IB and an RS cell are illustrated in Figure10. The maps clearly indicate that the IB as well as the RS cell received excitatory inputs from neurons located in layers II–VI within the same column and, to a lesser degree, also from the adjacent barrel-related column. The spatial distribution of fields providing excitatory inputs was generally continuous in infragranular layers and more patchy in the granular and supragranular layers. Especially in layers II/III, EPSPs could be elicited predominantly in fields near the apical dendrite of the recorded cells. In contrast to the EPSPs, inhibitory inputs were spatially more limited to fields in layers II/III and V of the same column.
Stimulation of presynaptic fields often elicited multiple EPSPs. To estimate the strength of excitatory input we determined the integral of all synaptically evoked excitatory events within a time window of 150 msec after stimulus. In several cases, photostimulation elicited synaptically evoked events as well as a direct response. Whenever possible, we separately calculated the integral of the synaptically evoked events only. In the remaining cases the traces were excluded from the integral analysis. The integrals of EPSPs ranged in 69% from 0.01 to 0.05 mVs. For both cell types, integrals obtained from fields in layers II/III normally did not exceed these values. However, “hot spots” of excitatory input could be found in layers IV, V, and VI, mainly located intracolumnarly. In these fields the integrals comprised a multitude of EPSPs and could reach 0.1–1 mVs. Especially in layer IV, hot spots could be found in discrete patches adjoining fields delivering no or very weak input. To analyze layer- and column-specific distribution of excitatory input, the mean integrals values within each layer and column were calculated. In general, excitatory input arising from intracolumnarly located fields was significantly stronger than from transcolumnarly located fields (p = 0.001, ANOVA). Integrals of EPSPs arising from layer II/III were significantly weaker than from layers IV (p = 0.03) and V (p = 0.02). However, within the layers the statistical analysis of excitatory integrals showed a high variability because of the large range of integral values. Thus, a significant cell type-dependent difference was not detectable.
Significant cell type-specific differences were found in the distribution of excitatory and inhibitory synaptic inputs originating from the same and neighboring columns (p = 0.03). The quantitative analysis of the spatial distribution of synaptic input demonstrates that both cell types received widespread excitatory inputs from all cortical layers (Fig.11A). The input was most prominent from within their respective column (p < 0.001). The prevalent source of excitatory inputs onto IB cells was layer VI. On average, 88 ± 7% of the intracolumnar and 54 ± 15% of the transcolumnar layer VI fields elicited an EPSP in IB cells. For the remaining layers, average intracolumnar inputs varied between 33 and 64%, and transcolumnar inputs varied between 19 and 43%. RS cells received most of their excitatory inputs from fields in layer V; 60 ± 17% of the intracolumnarly and 28 ± 17% of the transcolumnarly located fields delivered excitatory input during stimulation. For the remaining layers the average intracolumnar inputs varied between 25 and 53%; transcolumnar inputs varied between 8 and 21%. Intracolumnarly, a significant difference between the amount of excitatory inputs onto IB and RS cells was observed in layer VI only (p < 0.001, t test). IB neurons received significantly stronger transcolumnar excitatory inputs from layer VI (p= 0.001, t test), layer IV(p = 0.05), and layer II/III (p = 0.02) than RS cells.
Inhibitory inputs as well originated from layer II–VI (Fig.11B). Intracolumnar inhibitory inputs onto IB cells could be demonstrated from layers II/III and IV as well as V and amounted to <2%. Weak transcolumnar inhibitory inputs originated only from layer V. On the other hand, RS cells received significantly more intracolumnar inhibitory inputs from fields in layers II/III (7.5%;p < 0.001, t test) and V (8.3%;p = 0.003). In layer II/III, inhibitory inputs were often aligned to the apical dendrite of the RS cells. Occasionally RS cells also received distinct inhibitory inputs from fields in layers IV and VI, but because of their high variability these values were not significantly different compared with the IB cells. The differences in the strength of the inhibitory and excitatory synaptic inputs between RS and IB cells became even more apparent after the ratio was calculated between fields providing excitatory and fields providing inhibitory inputs for both cell types (Fig. 11C). IB cells revealed on average a 10-fold higher ratio of excitatory to inhibitory inputs than RS cells (IB: 84 ± 55, n = 7; RS: 8 ± 2, n = 8; p < 0.001, ANOVA).
DISCUSSION
In the present study we combined whole-cell recordings with biocytin-containing electrodes and local photolysis of caged glutamate to study the intracortical synaptic inputs onto layer V pyramidal cells in rat barrel cortex in vitro. We were able to show that the excitatory projection neurons of layer V, i.e., intrinsically burst spiking and regular spiking pyramidal cells, each possess a number of unique connectional properties. Remarkable are the previously undescribed prominent excitatory inputs from layers IV and VI that were stronger for IB than for RS cells, intracolumnarly and transcolumnarly. Furthermore, we could directly show the laminar origins and distribution of inhibitory inputs, which were much more prominent in RS than in IB cells.
Technical considerations
We have shown previously with extracellular recording techniques that long-term stable responses can be obtained by local release of (gamma-CNB)-caged l-glutamic acid in rat cortical slices (Kötter et al., 1998). Here, we focused on layer V pyramidal neurons and performed a number of important control experiments to evaluate our setup for analyses at the single-cell level. We reduced the intensity of the UV flash and the size of the activated area to reliably elicit an action potential only during stimulation of perisomatic fields restricted to 50–100 μm from the soma of the cell, thus providing a layer-specific resolution. For that purpose, we performed control recordings from neurons in all cell-containing cortical layers. Furthermore, we defined a criterion to differentiate between synaptic responses resulting from suprathreshold activation of presynaptic neurons and direct nonsynaptic stimulation caused by activation of glutamate receptors on the recorded cell. Recordings from the same cell were performed in normal ACSF as well as in low Ca2+/high Mg2+-containing solution to block synaptic transmission to allow comparison of the spatial distribution of the different types of evoked activity. The delay-to-onset times were longer for the synaptic responses because of long and variably sized action potential latencies in the presynaptic neurons (Katz and Dalva, 1994; Molnar and Nadler, 1999). Consequently, we can interpret the layer-specific spatial distribution of connected neurons but not the temporal properties of their input. Therefore, the stimulation procedure as well as the data analysis allow us to construct detailed maps of neuronal locations giving rise to intracortical synaptic inputs onto identified layer V pyramidal cells. In these maps, analysis of percentages of sites with detectable PSPs turned out to be more sensitive to cell type-specific differences than analysis of EPSP integrals. The latter showed a higher variability resulting from a large range of values for each single cell. This variability of synaptic transmission may result partially from paired-pulse facilitation and depression (Thomson, 1997).
Structural properties and firing patterns of layer V pyramidal cells
In agreement with previous reports, we found a significant correlation between the morphology of the cell and its intrinsic firing pattern. Layer V cells with a large soma, a thick apical trunk, and a rich apical dendritic tree responded to injection of a suprathreshold current pulse with a burst of action potentials (Chagnac-Amitai et al., 1990; Larkman and Mason, 1990) or at least a doublet (Schwindt et al., 1997). In contrast, all regular-spiking cells were characterized by a smaller soma, a thinner apical trunk, and a more restricted dendritic branching pattern. In addition to confirming these properties of different layer V pyramidal cells, our results demonstrate that these two cell types also differ in their intracortical synaptic inputs.
Intracolumnar and transcolumnar inputs onto layer V pyramidal cells
The topographic maps show extensive excitatory and inhibitory synaptic inputs from neurons located in layers II–VI onto layer V pyramidal cells. The weak synaptic inhibition of IB neurons, mainly derived from interneurons located relatively close to the recorded cell, as demonstrated here, is in agreement with previous electrophysiological investigations (Chagnac-Amitai and Connors, 1989a;Chagnac-Amitai et al., 1990; Nicoll et al., 1996). The more pronounced inhibitory inputs onto RS cells originated mainly from layers II/III and V of the same column (Nicoll et al., 1996), as well as from layer V of the adjacent column (Salin and Prince, 1996). Inhibitory interneurons in layer IV provided only a weak synaptic input in accordance with their highly restricted axonal arbors (Harris and Woolsey, 1983). These data clearly demonstrate that IB cells are under less inhibitory control than RS neurons. Therefore IB cells should be capable of distributing their activity reliably within a larger neuronal network.
In our experiments, excitatory inputs from layer II/III, which are supposed to be the main extralaminar source of excitatory input onto layer V pyramidal cells (Thomson and Deuchars, 1997; Reyes and Sakmann, 1999), were comparatively weak and spatially restricted. However, referring to our control experiments (see Materials and Methods), for some cells in layer II/III our stimulation may have been too weak to elicit action potentials. One possible reason for this could be that layer II/III pyramidal cells have lower resting membrane potentials than, for example, layer V pyramidal cells and require higher depolarization amplitudes to reach threshold (Mason and Larkman, 1990).
We expected excitatory inputs originating from the granular layer to be weak, because (1) anatomical studies have shown relatively sparse layer IV to V projections (Gilbert and Wiesel, 1983; Callaway and Wiser, 1996; Lübke et al., 2000), and (2) because physiological studies have supported a sequential intracortical pathway leading from layer IV to layer II/III and finally to layer V (Armstrong-James et al., 1992;Laaris et al., 2000). In contrast, our results clearly show strong, patchy inputs from layer IV within the same and adjacent column for both cell types. Such strong excitatory influences of layer IV onto layer V were recently described at the population level in a study of functional connectivity in the rat barrel cortex (Staiger et al., 2000). Here we show that in addition to the oligosynaptic pathway mentioned above, a strong monosynaptic input also exists. According to its spatial pattern, this input was probably provided by clusters of strongly coupled spiny neurons in layer IV (Feldmeyer et al., 1999), with most of the synaptic contacts onto layer V pyramidal cells located in or near the granular layer (Lübke et al., 2000). The possible occurrence of synaptic contacts between axons of spiny stellate neurons and apical dendrites of layer V pyramidal cells extending through granular and supragranular layers might resolve the discrepancy of an anatomically sparse but functionally potent layer IV to V input.
The bulk of excitatory synaptic inputs onto IB cells was provided from neurons located in infragranular layers of the same and adjacent column. These dominant excitatory inputs are probably mediated by the extensive intralaminar coupling between layer V IB cells (Chagnac-Amitai et al., 1990) and ascending collaterals arising from layer VI spiny neurons (Zhang and Deschenes, 1997). Photostimulation of fields in layer VI caused strong and widespread excitatory responses in IB cells, whereas RS neurons received only moderate inputs from this layer. This finding indicates a strong but cell type-dependent interaction between the two major cortical output layers V and VI (Deschenes et al., 1998). For RS cells, inputs from layer V were more pronounced than from layer VI, indicating a strong coupling between RS cells and other pyramidal cells within layer V.
Functional implications
The present study demonstrates cell type-specific differences in functional connectivity for the two major types of excitatory cells in layer V of the rat barrel cortex. Extensive intracolumnar and transcolumnar excitatory inputs onto IB cells are provided by neurons from all layers and accompanied by only weak inhibitory control. Under physiological conditions, IB cells may effectively integrate inputs from several cortical columns. Ensembles of these cells could possibly function as intracortical pacemakers and mediate widespread synchronous activity with characteristic rhythmic properties (Chagnac-Amitai and Connors, 1989b; Silva et al., 1991; Flint and Connors, 1996). Such rhythms are considered to be instrumental in the integration of different features of a distinct sensory percept (Singer, 1993) and have been shown to exist in the barrel cortex as well (Barth and Di, 1991; Jones and Barth, 1997). According to our data, IB cells may not only synchronize cortical circuits, but may also boost cortical outputs to subcortical and feedback circuits (Ahissar et al., 2000). Finally, the strong and widespread intracortical interactions, the weak inhibitory control, and the burst discharge may promote the initiation and propagation of epileptiform discharge. Therefore, layer V IB cells could play a critical role in synchronizing cortical modules under physiological as well as pathophysiological conditions (Connors and Amitai, 1993).
The complex excitatory and inhibitory intracolumnar control of RS cells obviously provides them with different information-processing capabilities. By feeding back inputs to the supragranular layers, these cells could participate in filtering sensory information by decoding the physical properties of tactile stimuli derived from the respective “principal” whisker (Simons, 1978, 1995). How these “intracolumnar RS” and “transcolumnar IB” circuits interact remains an important issue for further investigations.
In conclusion, our analyses revealed the following aspects of layer V circuitry organization. (1) The specific pattern of functional connectivity of layer V pyramidal cells correlates with the morphological and electrophysiological properties of these neurons. (2) Both IB and RS cells receive excitatory synaptic inputs from all cortical layers, in a more or less homogenous fashion from layers V and VI, whereas inputs from layers IV and II/III show a patchy pattern. Inputs from layer VI are significantly stronger for IB than for RS pyramidal cells. (3) IB cells receive only a weak inhibitory input, mainly originating locally from within layer V. In contrast, the more extensive inhibitory inputs onto RS cells originate primarily from layers II/III and V of the same column and from layer V of the adjacent column.
Footnotes
This study was supported by the Gesellschaft der Freunde und Foerderer der Heinrich-Heine-Universitaet, Duesseldorf, the C. & O. Vogt-Institut fuer Hirnforschung GmbH, the Gertrud Reemtsma Stiftung, and Deutsche Forschungsgemeinschaft Grant Lu 375/3-2 to H.J.L. We thank U. Opfermann-Emmerich for skilled technical assistance.
Correspondence should be addressed to Dirk Schubert, Institute of Neurophysiology, Heinrich-Heine-University Duesseldorf, POB 101007, D-40001 Duesseldorf, Germany. E-mail:schubd@uni-duesseldorf.de.
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