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1 School of Biomedical Sciences, Worsley Building, University of Leeds, Leeds LS2 9JT, UK
2
Johannes-Müller-Institute of Physiology at the charité, Humboldt University Berlin, Tucholskystr. 2, 10117 Berlin, Germany
3
University Hospital Neurology, Department of Clinical Neurobiology Im Neuenheimerfeld 364, Heidelberg D-69120, Germany
4
Department of Physiology and Pharmacology, SUNY Health Science Center, Brooklyn, NY 11203, USA
Abstract
Using whole-cell patch-clamp recordings in conjunction with post hoc anatomy we investigated the physiological properties of hippocampal stratum oriens and stratum pyramidale inhibitory interneurones, before and following the induction of pharmacologically evoked gamma frequency network oscillations. Prior to kainate-induced transient epochs of gamma activity, two distinct classes of oriens interneurones, oriens lacunosum-moleculare (O-LM) and trilaminar cells, showed prominent differences in their membrane and firing properties, as well as in the amplitude and kinetics of their excitatory postsynaptic events. In the active network both types of neurone received a phasic barrage of gamma frequency excitatory inputs but, due to their differential functional integration, showed clear differences in their output patterns. While O-LM cells fired intermittently at theta frequency, trilaminar interneurones discharged on every gamma cycle and showed a propensity to fire spike doublets. Two other classes of fast spiking interneurones, perisomatic targeting basket and bistratified cells, in the active network discharged predominantly single action potentials on every gamma cycle. Thus, within a locally excited network, O-LM cells are likely to provide a theta-frequency patterned output to distal dendritic segments, whereas basket and bistratified cells are involved in the generation of locally synchronous gamma band oscillations. The anatomy and output profile of trilaminar cells suggest they are involved in the projection of locally generated gamma rhythms to distal sites. Therefore a division of labour appears to exist whereby different frequencies and spatiotemporal properties of hippocampal rhythms are mediated by different interneurone subtypes.
(Received 31 July 2004;
accepted after revision 11 October 2004;
first published online 14 October 2004)
Corresponding author T. Gloveli: Johannes-Müller-Institut für Physiologie, Charité Universitätsmedizin Berlin, Tucholskystr. 2, 10117 Berlin, Germany. Email: tengis.gloveli{at}charite.de
Synchronous gamma-frequency oscillations (3080 Hz) represent a temporally coherent activity and are thought to be important in cortical information processing (Gray & Singer, 1989; Jones & Barth, 1997; Ritz & Sejnowski, 1997; Fries et al. 2001). One of their putative roles may be the synchronization of groups of spatially segregated cortical neurones at sites that can be many millimetres apart (Gray et al. 1989). Synchronous activity is ideally suited to provide a mechanism for the functional binding of sensory features. Gamma frequency oscillations have been observed in a variety of brain structures (Singer & Gray, 1995), amongst them the hippocampus, which has a key role in memory formation (Morris et al. 1982; Zola-Morgan & Squire, 1993), and shows oscillatory activity in the theta/gamma frequency band during specific behavioural states (Buzsaki et al. 1983; Soltesz & Deschenes, 1993; Sik et al. 1995; Singer & Gray, 1995; Penttonen et al. 1998). There is compelling evidence that hippocampal interneurones have a pivotal role in driving inhibition-based rhythms, such as gamma and theta frequency network oscillations (Whittington et al. 1995; Fisahn et al. 1998; Hormuzdi et al. 2001; Gillies et al. 2002; Klausberger et al. 2003, 2004).
Interneurones can be broadly classified into several classes on the basis of different criteria, such as action potential firing properties, somato-dendritic architecture and axonal ramification pattern, neurochemical content, voltage and ligand-gated conductances as well as plastic changes in excitatory synaptic transmission (for reviews see Freund & Buzsaki, 1996; McBain & Fisahn, 2001; Maccaferri & Lacaille, 2003). One of the classification schemes is based on the axonal ramification patterns of interneurones and, in particular, the innervation of spatially segregated domains on the somato-dendritic surface of principal cells. Thus hippocampal interneurones can be divided into perisomatic targeting interneurones, such as basket and axo-axonic cells, and dendrite targeting cells, such as oriens lacunosum-moleculare (O-LM), bistratified and trilaminar interneurones (Buhl et al. 1994; Freund & Buzsaki, 1996). Within this broad classification scheme further subdivision is possible based on the proximo-distal segregation of efferent target domains (Maccaferri et al. 2000). Although it is reasonable to assume that the anatomical heterogeneity of hippocampal interneurones is reflected in their functional diversity, in particular during different forms of network activity, there are few studies which have attempted a correlation of structure and function. In particular, the way in which oscillatory input affects the activity of individual interneurones in the active network remains to be clarified.
Whole-cell patch-clamp recordings using infrared differential contrast videomicroscopy (Dodt & Zieglgansberger, 1990, 1994) have greatly expanded our understanding of interneurone function. However, this approach has been hampered due to the difficulty of generating physiologically relevant population activity, such as network oscillations in submerged conditions. In the present study we employ brief pressure ejections of kainate to generate oscillatory network activity in submerged slices. Using a technical modification of a pharmacological protocol which, in mechanistic terms, is reasonably well understood (Traub et al. 2000; Hormuzdi et al. 2001), we were able, for the first time, to record from visually identified interneurones during gamma frequency network oscillation. By correlating the physiological properties of distinct types of anatomically identified hippocampal interneurones we were able to demonstrate that these anatomically heterogeneous cell classes show differences in some of their biophysical properties, synaptic mechanisms and firing patterns. These different properties of interneurones, in turn, determine their differential involvement in the generation of hippocampal oscillatory network activity. In addition, we also address the unresolved issue as to how the hippocampal network can generate nested rhythms concurrently occurring in the theta and gamma frequency bands.
Methods
Slice preparation
Brains were taken from C57BL6 mice (P1825), anaesthetized with a lethal dose of inhaled isoflurane, immediately followed by an I.M. injection of ketamine (100 mg kg1) and xylazine (10 mg kg1) in accordance with the UK Animals (Scientific Procedures) Act 1986. Horizontal combined entorhinal cortexhippocampal slices (450 µm thick) were prepared using a tissue slicer (Leica VT 1000S, Nussloch, Germany).
Perisomatic interneurones were studied using transgenic mice that expressed enhanced fluorescent protein under the control of the parvalbumin promoter. Transgenic mice were generated using bacterial artificial chromosome techniques, as described in detail elsewhere (Meyer et al. 2002). Slices were incubated at room temperature for at least 1 h in a holding chamber and then transferred to the recording chamber. The solution used during incubation and recording contained (mM): NaCl, 126; KCl, 3; NaH2PO4, 1.25; CaCl2, 2; MgSO4, 2; NaHCO3, 24; glucose, 10, saturated with 95% O2 and 5% CO2.
Extracellular field recordings
Experiments were performed at 29°C in a submerged-type chamber. ACSF in the submerged chamber was maintained at a low level and the rate of superfussion with the ACSF was 34 ml min1. The ejecting and recording electrodes were maintained in close proximity (typically < 0.2 mm) so as to get prominent field oscillations. Field potential recordings and pressure application of kainate (1 mM, 60 p.s.i., duration 1060 ms) were done in the stratum radiatum of area CA3 using patch pipettes. Ejected volume was generally correlated with oscillatory peak power and duration, whereas the peak frequency remained constant for any given slice. Field potentials were recorded with an Axoclamp 2B amplifier (Axon Instruments, Union City, CA, USA). Data were digitized with an ITC-16 A/D board (Instrutech Corp., Port Washington, NY, USA) and further analysed using Axograph (Axon Instruments) and KaleidaGraph (Synergy Software, Reading, PA, USA) software. Oscillatory peak frequency was determined by averaging several consecutive Fourier transforms, contained within a 230 s epoch. Power in the gamma frequency band was calculated by integration of power spectra between 20 and 80 Hz. Auto- and cross-correlations were calculated over a 2 s epoch. Student's t test was used for statistical comparisons; differences were considered significant if P < 0.05. Average values are expressed as the mean ± S.E.M.
Whole-cell recordings
Concomitant with the extracellular field potential whole-cell patch-clamp recordings in current and voltage clamp mode were obtained from stratum oriens and pyramidale interneurones or pyramidal cells of area CA3 visualized by infrared differential interference contrast (DIC) videomicroscopy (Zeiss Axioscope microscope, Hamamatsu CCD camera, Luigs & Neumann Infrapatch set-up). Whole-cell recording pipettes (35 M
) were filled with a solution containing (mM): potassium gluconate, 135; KCl, 5; ATP-Mg, 2; GTP-Na, 0.3; Hepes, 10; plus biocytin, 0.5% (pH 7.3 and 280 mosmol l1). An Axopatch 1D amplifier (Axon Instruments) was used for current- and voltage-clamp recordings. The holding potentials were 60 mV and 70 mV for current- and voltage-clamp recordings, respectively, unless indicated otherwise. The seal resistance before establishing whole-cell mode was
2 G
. The series resistance was monitored repeatedly during the experiment by measuring the amplitude of the capacitive current in response to a 10 mV pulse. Series resistance (range 1218 M
) was not significantly different between different interneurone types (14.2 ± 0.9 M
(n = 15), 15.1 ± 0.8 M
(n = 8), 13.4 ± 1.2 M
(n = 6) and 15.3 ± 1.4 M
(n = 3) in O-LM, trilaminar, basket and bistratified cells, respectively). Voltage measurements were not corrected for the potassium gluconate junction potential.
The intrinsic properties of cells were measured in whole-cell current-clamp mode. The resting membrane potential was estimated during the absence of a holding current. The input resistance and membrane time constant were estimated from voltage responses to current injection (500 ms; ± 100 pA, at 10 pA increments). The input resistance was determined from the slope of the steady state responses in a linear region around, and including, the origin. The membrane time constant was obtained from the slowest time constant of exponential fits to voltage transients in the same linear region of the IV plot (see Spruston et al. 1997). Sag was quantified by the ratio of the steady state voltage to the peak voltage in response to current injections (200 pA, 500 ms). As recorded cells did not fire action potentials at rest, the analysis of the amplitude and duration of action potentials as well as decay time constant and half-duration of afterhyperpolarization (AHP) were performed on first action potential discharges elicited by stepwise increased constant depolarizing current injection, causing small (
5 mV) graded voltage changes. The recorded interneurones typically showed rapid-onset, deep spike AHP which decayed rapidly and monophasically. The duration of action potentials was measured at half-amplitude. The accommodation parameters were measured on discharges elicited by application of 500 ms depolarizing current pulses. Repetitive firing in response to depolarizing current injection (500 ms) was evaluated by measuring the number of spikes versus the amplitude of injected current (up to 600 pA). The action potential discharge frequency was measured between the first two spikes (initial) and at the end of firing (steady-state) during a depolarizing current injection (500 ms) at all stimulation intensities tested.
The spontaneous excitatory postsynaptic currents (EPSCs) and potentials (EPSPs) as well as kainate-evoked EPSCs were measured at the reversal potential for GABAA receptor-mediated events (around 70 mV). The threshold of spontaneous and evoked EPSCs was determined from their absolute amplitude. Because of the very high frequency of kainate-evoked individual events of compound EPCSs, these events were carefully selected after visual inspection of recorded traces in order to discard supposed bi- or multiquantal events. Particularly, single events typically detectable at the rising part of kainate-evoked compound EPSCs, which due to their distinct time course allowed us to measure their 1090% rise time and decay time constant, were individually selected. The individual events (40 events from each cell) were aligned for averaging and calculating kinetic parameters of EPSCs. Postsynaptic events as well as the inter-event interval of compound EPSCs (from ca 600 events) were further analysed with Mini Analysis Program (Synaptosoft, Decatur, GA, USA).
Signals were filtered at 5 kHz (whole-cell recording) or 0.0021 kHz (extracellular field potential recording) with an external 8-pole Bessel filter (Applegarth Electronics, Oxford, UK) and digitized at 10 kHz using an ITC-16 A/D board (Instrutech). EPSC and AHP kinetics (decay time constant, half-duration) were studied using Mini Analysis Program. The Kolmogorov-Smirnov statistical test was used to compare two different cumulative distributions with P < 104 reaching statistical significance.
Anatomical identification of interneurones
Slices with a biocytin-filled interneurone were sandwiched between two Millipore filters to avoid deformation and fixed in 0.1 mM phosphate buffer (pH 7.4) containing 4% paraformaldehyde, 0.05% glutaraldehyde and 15% saturated picric acid at 4°C for 2448 h. Following gelatine embedding, 75 µm sections of the slices were prepared. The filled neurones were visualized by incubating sections in avidinbiotin conjugated horseradish peroxidase (ABC, Vector Laboratories, Ltd, UK) and reacting them with diaminobenzidine and hydrogen peroxide. Sections were then intensified in 0.5% OsO4, dehydrated and embedded into epoxy resin (Durcupan, Sigma) on glass slides. Subsequently, the cells were reconstructed with the aid of a camera lucida or a Neurolucida 3D reconstruction system (MicroBrightField, Inc., Williston, VT, USA).
Results
Network gamma oscillations in submerged slices
We employed a pharmacological gamma-induction protocol to study network oscillations in submerged slices. Pressure ejection of kainate (1 mM) onto stratum radiatum of the hippocampal CA3 area reliably and repeatedly induced a transient (840 s) period of network gamma frequency (
) oscillations that could be detected with an extracellular field electrode located in close proximity to the ejection site (n = 47, Fig. 1A and B). The onset of the oscillation was preceded by a small (200800 µV) and short (< 1 s) negative-going DC shift in the field recording (Fig. 1B). The power spectrum of the oscillatory activity shows a prominent peak in the gamma frequency range (Fig. 1C). The mean frequency of the
oscillations was 32.8 ± 0.6 Hz (n = 47).
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Concomitant with extracellular field potential recordings whole-cell patch-clamp recordings were obtained from interneurones in stratum oriens/alveus of area CA3 of the hippocampus. Stratum oriens interneurones were morphologically diverse. Based on their somato-dendritic architecture and their axonal ramification pattern they could be classified into several groups (see also Maccaferri et al. 2000; for review see Freund & Buzsaki, 1996). For further detailed analysis, we selected two classes of post hoc anatomically identified horizontal cells, dendrite-targeting oriens lacunosum-moleculare (O-LM, n = 15) and trilaminar (n = 8) interneurones. These are clearly distinguishable as they establish spatially segregated postsynaptic target domains on distal versus proximal pyramidal dendrites and have characteristic electrophysiological properties. In addition bistratified (n = 3), and parvalbumin (PV)-positive perisomatic targeting interneurones (n = 6) in stratum oriens/pyramidale as well as CA3 pyramidal cells (n = 9) were studied for comparison. Having largely similar physiological and morphological (basket-like) features, PV-positive cells were grouped together and classified as perisomatic interneurones. About one-third of recorded interneurones could not be completely reconstructed, either because of their proximity to the slice surface or because of the incomplete labelling. We excluded these cells from our study.
All recorded and biocytin-labelled O-LM interneurones displayed a previously described horizontal organization of dendritic tree and axonal termination in the stratum oriens and lacunosum-moleculare (Fig. 2A, see also Ali & Thomson, 1998; Maccaferri et al. 2000), coaligned with the distal apical dendrites of the pyramidal cells. The trilaminar cells have the similar horizontally distributed dendrites in stratum oriens, but are clearly different from O-LM cells in respect of axonal arborization (Fig. 2BD) and exibit clearly different physiological features. In contrast to the O-LM cells, the trilaminar interneurone had axon collaterals in strata oriens, pyramidale and radiatum (see also, Sik et al. 1995) which extended a long distance transversally in the area CA1/subicular direction (Fig. 2B and D).
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There were no significant differences in the resting membrane potentials of O-LM and trilaminar interneurones. O-LM interneurones had a significantly higher input resistance and slower membrane time constant than trilaminar cells (Table 1). A consistent electrophysiological feature of O-LM cells contrasting the trilaminar and all other studied interneurones was the sag in response to hyperpolarizing current injection (Fig. 3A and B, see also Lacaille & Williams, 1990; Sik et al. 1995; Maccaferri & McBain, 1996; Ali & Thomson, 1998; Lien et al. 2002). Mean sag ratio in O-LM cells (200 pA, 500 ms hyperpolarizing current injection) was 0.79 ± 0.02 (n = 10). During intrasomatic current injection trilaminar cells discharged in clusters of short-duration action potentials (Table 1, Fig. 3C). Afterhyperpolarization (AHP) decayed significantly faster in trilaminar cells than in O-LM cells (Table 1, Fig. 3C). In response to depolarizing current injection (up to 600 pA), the O-LM cells showed significantly lower frequency discharges than trilaminar cells (Table 1). Mean initial and steady state firing frequencies were 130.0 ± 19.1 Hz and 70.0 ± 17.2 ms in O-LM (n = 15) and 179.3 ± 26.6 Hz and 110.0 ± 13.1 Hz in trilaminar cells (n = 8, P < 0.05 for both initial and steady state firing frequency). However, these cells demonstrated a similar degree of action potential accommodation to corresponding current pulse (the ratio of the steady state firing frequency to the initial frequency was 0.54% in O-LM and 0.61% in trilaminar cells, P > 0.05, Fig. 3D and E).
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oscillations. During kainate-evoked gamma frequency activity both classes of interneurones with horizontal dendrites in stratum oriens (Fig. 2) received a sustained barrage of gamma frequency compound EPSCs (Vhold 70 mV) that were temporally correlated with the antiphasic extracellular field oscillation (Fig. 4A and B).
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cycle (Fig. 4Cii). O-LM cells instead discharged at theta frequency during the gamma oscillations. The average firing probability of O-LM interneurones during a cycle was 25.8 ± 4.3% and the mean firing frequency was in the theta frequency range (Table 1). While the power spectrum of the field oscillatory activity showed a peak in the gamma frequency range, the power spectrum of current clamp recording in O-LM interneurones demonstrated a clear peak at the theta frequencies following kainate ejection (Fig. 4Ciii and iv). Remarkably O-LM cells discharged with theta frequency not only at resting membrane potential but also at more depolarized level (mean membrane potential 49.7 ± 1.0 mV, n = 4) close to threshold of AP firing (Fig. 4Dii), with the average firing probability during a cycle of 28.4 ± 5.6% (n = 4) and a mean frequency of 9.1 ± 2.3 Hz (n = 4) suggesting that the observed firing properties during the gamma oscillations in fact reflect an actual cellular specificity of these cells. In contrast, trilaminar cells discharged on every cycle of the gamma frequency oscillation (Fig. 4Eii). Moreover, the latter showed a propensity to fire spike doublets (mean AP interval 5.73 ± 0.09 ms, n = 8). The power spectrum of current clamp recordings in trilaminar cells demonstrated a peak at the gamma frequency range (Fig. 4Eiiiiv). A high frequency synaptic oscillatory component in horizontal interneurones
During gamma activity both O-LM and trilaminar interneurones show a dramatic increase in synaptic activity which is temporally coherent with concomitant extracellular recordings (Fig. 5A and B). Pooled power spectra exhibited a prominent peak in the gamma frequency range (32.9 ± 2.1 Hz in O-LM, n = 6 and 31.4 ± 2.2 Hz in trilaminar cells, n = 6, P > 0.05, Fig. 5C and D). The peak power of EPSC recordings in trilaminar cells was significantly larger than in O-LM cells (Table 2, Fig. 5D). The majority of EPSCs in both cell classes were clearly multiquantal, comprising clusters of high-frequency rhythmic events, which were separated by regular intervals of aperiodically occurring EPSCs. Simultaneous extracellular and patch-clamp recordings during gamma oscillations showed that such clusters of EPSCs in the O-LM interneurones were temporally correlated with the extracellularly recorded population activity (Fig. 5Aiii). Likewise, rhythmic, but significantly larger amplitude EPSCs were observed in trilaminar cells (Fig. 5Bii; note change in scale). When band-pass filtering epochs of compound EPSCs between 200 and 500 Hz the high-frequency oscillatory component of synaptic activity was dramatically accentuated (Fig. 5Aiii and E; and Fig. 5Biii and F). Such incremental bursts of EPSCs occurred in all studied O-LM (n = 15) and trilaminar (n = 8) interneurones and further analysis of inter-event intervals revealed a similar periodicity in O-LM and trilaminar cells (Table 2, Fig. 5G and H), suggesting a common source of excitatory input.
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O-LM and trilaminar cells showed clear differences in the amplitude and kinetics of spontaneous EPSPs (sEPSP) (Table 2, Fig. 6A). Differences in EPSPs are also reflected in postsynaptic current recordings from these two classes of interneurones. As revealed by the voltage clamp recordings, the mean amplitude of spontaneous EPSCs (sEPSCs) in O-LM cells was significantly smaller than in trilaminar interneurones (Table 2, Fig. 6B and C). Likewise, the kinetics of synaptic events in both interneurone types were markedly different. The average 1090% rise time and decay time constant of sEPSC in O-LM cells were significantly slower than in trilaminar interneurones (Table 2, Fig. 6B and C). The properties of spontaneous PSCs (amplitude, frequency) in both cell classes did not change significantly in the presence of bicuculline, a GABAA receptor antagonist (20 µM, n = 4), but these currents were completely blocked by additional application of an AMPA/kainate receptor antagonist, 1,2,3,4-tetrahydro-6-nitro-2,3-dioxo-benzo[f]quinoxaline-7-sulfonamide (NBQX; 10 µM, n = 4, data not shown) suggesting their excitatory nature. Interestingly, the differences in the kinetic properties of sEPSCs between the two interneurone types were also maintained during gamma frequency oscillations (Fig. 6D and E). The individual components of kainate-evoked compound EPSCs (eEPSCs) in O-LM cells were again significantly smaller than in trilaminar cells (Table 2, Fig. 6D and E). The mean 1090% rise time and decay time constant of averaged eEPSCs in O-LM interneurones were slower than in trilaminar cells (Table 2, Fig. 6D and E, P < 108, Kolmogorov-Smirnov statistics).
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Fast spiking perisomatic interneurones with a typical basket cell axonal arborization in the stratum pyramidale (Fig. 7A), have a mean resting membrane potential, input resistance, membrane time constant and action potential half-duration not significantly different from those in trilaminar cells (Table 1). Single action potentials were followed by AHP which were longer though not significantly different from those in trilaminar cells (Table 1). These cells showed a low degree of spike frequency adaptation (Fig. 7A). During kainate-evoked oscillation these cells showed gamma frequency EPSCs (Vhold 70 mV) that were temporally correlated with the antiphasic extracellular field oscillation (Fig. 7B). In the current clamp mode, 4 of 6 studied perisomatic interneurones discharged with doublets of action potentials, which occurred irregularly (on every 15 field gamma cycles) and were interrupted by single action potentials during the gamma activity. Mean inter-doublet interval was 8.2 ± 0.2 ms (n = 4), significantly longer then those in trilaminar cells (P < 0.05). This doublet interval corresponded approximately to twice the interval between components of the compound EPSC invading these cells (4.22 ± 0.21 ms, Table 2). The remaining two cells generated exclusively single action potentials on every gamma cycle. Both, single spikes and doublets of action potentials were phase locked to the field (Fig. 7D).
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Prominent differences were apparent when comparing the kinetic properties of EPSCs/Ps in CA3 pyramidal neurones with those in interneurones (Fig. 9C and D). In general, averaged pyramidal cell EPSCs had markedly slower time courses than those of interneurones (Table 2).
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activity. Discussion
Using a pharmacological gamma-induction protocol to study oscillations in submerged slices, we have provided clear evidence that hippocampal interneurones exhibit different functional roles in the generation of hippocampal network oscillations. In terms of output the two extremes of behaviour were shown by O-LM cells, firing at theta frequencies (every 45 field gamma periods) and trilaminar cells (firing double spikes on every field gamma period). Between these two output patterns perisomatic targeting basket cells fired single action potentials, with occasional doublets, on each gamma period and bistratified cells invariably fired only once per period. Each of these cell types received similar, compound EPSC inputs at gamma frequencies during the field rhythm. A number of factors as we will argue below may account for the large range of output profiles seen in these different types of interneurones.
EPSC/P properties of the interneurones in the oscillatory network
Our data confirm findings showing that the properties of excitatory events discriminate hippocampal principal cells from inhibitory neurones (Miles, 1990; Jonas et al. 1993; Geiger et al. 1997; Toth et al. 2000). It appears that excitatory synapses onto interneurones not only tend to have a larger number of AMPA receptors (Nusser et al. 1998), thereby increasing the quantal amplitude, but the postsynaptic receptors also appear to have a different molecular composition (Geiger et al. 1995), which, in turn, endows them with faster kinetics (Geiger et al. 1997). Hence temporal summation of EPSPs in interneurones is restricted to a relatively narrow time window and, accordingly, both computational simulations and experimental data suggest that interneurones act as coincidence detectors (Konig et al. 1996; Galarreta & Hestrin, 2001), whereas pyramidal cells are more suitable to integrate the overall level of postsynaptic activity.
The kinetic properties of excitatory events in stratum pyramidale interneurones have profound effects on network activity associated with changes in interneurone firing patterns (Fuchs et al. 2001). Here we provide evidence that different classes of str. oriens interneurones with distinct axonal ramification patterns and efferent target profiles show clear differences in both amplitude and kinetics of EPSCs/Ps. As suggested above, it is possible to explain these data solely with differences in the number and properties of AMPA/kainate receptors. However, in view of the presumably inadequate voltage clamp of remote dendritic sites, other factors may also affect the magnitude and kinetics of excitatory events, amongst them passive membrane properties, voltage-gated dendritic conductances and the electrotonic remoteness of synaptic junctions.
During kainate-evoked oscillatory activity the interneurones studied here receive gamma-frequency compound EPSPs which are temporally correlated with extracellular population activity. In view of the slice being de-afferented, it is likely that the action potential-dependent excitatory events are mediated by local excitatory feedback loops which originate in neighbouring pyramidal neurones. Although the latter fire only sporadically during gamma activity, interneurones, for three reasons, may receive a rhythmic barrage of gamma frequency EPSPs. First, in the active network, in view of their large numbers, at least several pyramidal cells are likely to fire on any given oscillatory cycle. Second, due to the convergence of numerous pyramidal cell recurrent axons onto a single postsynaptic interneurone it follows that each interneurone is also likely to receive a small number of unitary excitatory inputs on each successive gamma wave. Third, activity in pyramidal cell axons could orthodromically excite interneurones, without pyramidal cell somata necessarily firing (Traub et al. 2003).
Despite the range of interneuronal outputs seen during gamma activity (O-LM theta frequency output up to trilaminar neuronal doublets), little difference was seen in the frequency of EPSCs within the phasic compound excitatory events. The amplitudes of excitatory drive were considerably larger in doublet-firing trilaminar cells than O-LM cells, suggesting the intensity of synaptic drive may play a role in generating such different outputs. However, similar phasic drives were seen in basket and bistratified cells compared with trilaminar cells but these cells rarely, or never, fired action potential doublets. Marked differences in EPSC kinetics were also seen in cells at the ends of the output range (theta versus gamma doublet). Slower kinetics in O-LM cells may be expected to increase temporal summation of individual components of the compound EPSC during gamma oscillations but this did not result in larger phasic drive. In summary, though differences in amplitude and kinetics of EPSCs existed between the different interneurone subtypes no clear pattern sufficient to explain the range of output profiles could be found in EPSCs alone.
Intrinsic properties of interneurones with respect to firing patterns
The most striking finding in terms of interneurone output was that O-LM cells generated a robust theta frequency output whereas the other interneurones fired action potentials (singly or as doublets) at gamma frequencies. Near firing threshold O-LM cells show prominent membrane potential oscillations in the theta frequency range (T. Gloveli, M. A. Whittington, E. H. Buhl, unpublished observations; Maccaferri & McBain, 1996), whereas hippocampal fast-spiking cells preferentially resonate in the gamma range (Pike et al. 2000), thus endowing both types of cell with a greater propensity to discharge in a different frequency band. In addition, O-LM cells had a longer membrane time constant than the gamma-preferring interneurones and a considerably longer AHP. Changes in AHP profiles in interneurones have been shown to have dramatic effects on firing patterns (e.g. see Lau et al. 2000; Savic et al. 2001). The decay time constant of AHP in O-LM cells was some 5- to 10-fold slower than in interneurones generating gamma frequency outputs. In contrast trilaminar cells had the most rapid AHP (decay time constant less than 0.5 ms). This, coupled with the larger phasic synaptic excitation may, in part, explain the marked output profile differences of these two cells for a given temporal pattern of phasic input.
Different roles for interneurones during network oscillations
In vivo (Csicsvari et al. 2003), in vitro (Fisahn et al. 1998) and computational models of pharmacologically evoked persistent gamma activity (Traub et al. 2000) have revealed a critical involvement of phasic excitatory input onto interneurones. In our model of locally generated gamma oscillations the pattern of excitatory input was broadly similar in each interneurone class. The differences in output characteristics appeared to correspond mainly to the intrinsic temporal properties of these interneuronal membranes. The range of output profiles seen was accompanied by specific axonal arborization and terminal field profiles in the different cell types. Both bistratified and basket cells generated a predominantly gamma frequency output and targeted proximal dendritic and perisomatic pyramidal neuronal compartments. These anatomical and electrophysiological properties make these neurones ideally suited for generating local gamma rhythms. Given the same network stimulus O-LM cells generated a theta frequency output and targeted basal and distal apical dendritic fields. During field gamma oscillations a more prominent theta frequency inhibitory input to distal apical dendrites has been reported (Gillies et al. 2002). At the local network level it therefore appears that specific interneurones generating gamma frequency outputs present this output preferentially to perisomatic and proximal dendritic compartments. Interneurones generating theta frequency outputs target more distal dendritic compartments (certainly in the apical arbour). In vivo oscillatory activity in the hippocampus frequently takes the form of a gamma rhythm nested in a theta rhythm (Penttonen et al. 1998). This phenomenon may reflect a division of labour amongst interneurones whereby the two frequencies are generated by two distinct subclasses of interneurone and projected to different compartments of principal cells.
The most powerful interneuronal output seen during local gamma oscillations was associated with trilaminar interneurones. These cells generated highly regular fixed, short latency spike doublets. Due to the axonal arborization profile of these interneurones, this output would be targeted not only onto somatic and dendritic though not apical distal dendritic compartments of local pyramidal cells, but also onto more distal sites. Axon collaterals were seen projecting all the way along area CA1 and into the subiculum. Thus, via these cells, gamma rhythms generated locally in area CA3 could be efficiently broadcast to distal sites downstream in the classical hippocampal processing pathway.
We conclude that anatomical, intrinsic electrophysiological, and to some extent synaptic, properties combine to govern the role of different interneurone subclasses during a local hippocampal field oscillation. Different interneurones are associated with different network frequencies, different compartmental presentation of inhibitory inputs to principal cells and different local and distal communication of the interneuronally mediated rhythm. Given the very broad array of interneurone subtypes in the hippocampus alone, the small sample presented here suggests that each interneurone subtype may play a specific, and perhaps unique, role in network activity.
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Acknowledgements
This study was supported by the SFB TR3/B5 to T.G., T.D. and U.H.; and the MRC, the Wellcome Trust, NIH/NIDS and EU grant to the late E.H.B. We thank Dr F. E. N. LeBeau for comments on the manuscript and D. Harrison for expert technical assistance.
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