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Volume 16, Number 9,
Issue of May 1, 1996
pp. 3056-3066
Copyright ©1996 Society for Neuroscience
High-Frequency Oscillations in the Output Networks of the
Hippocampal-Entorhinal Axis of the Freely Behaving Rat
James J. Chrobak and
Gyorgy Buzsáki
Center for Molecular and Behavioral Neuroscience, Rutgers, The
State University of New Jersey, Newark, New Jersey 07102
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
DISCUSSION
FOOTNOTES
REFERENCES
ABSTRACT
Population bursts of the CA3 network, which occur during eating,
drinking, awake immobility, and slow-wave sleep, produce a large field
excitatory postsynaptic potential throughout stratum radiatum of the
CA1 field (sharp wave). The CA3 burst sets into motion a short-lived,
dynamic interaction between CA1 pyramidal cells and interneurons, the
product of which is a 200 Hz oscillatory field potential (ripple) and
phase-related discharge of the CA1 network. Although many CA1 pyramidal
neurons discharge during the time frame (50-100 msec) of each sharp
wave, each wave of a ripple (~5 msec) reflects the synchronization of
more discrete subsets of CA1 neurons.
When we used multi-site recordings in freely behaving rats, we observed
ripples throughout the longitudinal extent (~4-5 mm) of the dorsal
CA1 region that were coherent for multiple cycles of each ripple.
High-frequency ripples were also observed throughout the
hippocampal-entorhinal output pathway that were concurrent but less
coherent on a cycle-by-cycle basis. Single and multiunit neuronal
activity was phase-related to local ripples throughout the
hippocampal-entorhinal output pathway. Entorhinal ripples occurred
5-30 msec after the CA1 ripples and were related to the occurrence of
an entorhinal sharp wave. Thus, during each hippocampal sharp wave,
there is a powerful synchronization among the neuronal networks that
connect the hippocampus to the neocortex. We suggest that this
population interaction (1) biologically constrains theoretical models
of hippocampal function and dysfunction and (2) has the capacity to
support an ``off-line'' memory consolidation process.
Key words:
hippocampus;
subiculum;
entorhinal cortex;
oscillations;
sharp waves;
memory;
epilepsy
INTRODUCTION
The hippocampus and entorhinal cortex (EC) are
substrates for the formation of enduring memories and the
etiology/pathology of Alzheimer's dementia as well as temporal
lobe epilepsy. The manner and mechanisms by which these structures
interact have implications for both physiological and
pathophysiological processes.
Synchronous population potentials and localized oscillatory patterns
occur in many neural networks (Buzsáki et al., 1983 , 1992 ;
Steriade et al., 1993 ; Freeman and Barrie, 1994 ; Gray, 1994 ; Singer,
1994 ). These events reflect synchronizing mechanisms for coordinating
ensembles of neurons within distributed neural networks and for
bringing neuronal aggregates within/across structures together in time
(Buzsáki and Chrobak, 1995 ).
The physiology of the hippocampal-entorhinal networks is characterized
by behaviorally regulated, macroscopic potentials that temporally
organize specific subsets of network neurons. occurs during
exploratory behavior and rapid eye movement sleep and represents a
period when hippocampal circuits receive rhythmic input from neurons
within the superficial layers of the EC (Mitchell and Ranck, 1980 ;
Buzsáki et al., 1983 ; Boeijinga and Lopes da Silva, 1988 ; Stewart
et al., 1992 ). In contrast, during sharp waves, which occur during
consummatory behaviors and slow-wave sleep, the output neurons of the
hippocampus and EC participate in organized population bursts
(Buzsáki, 1989 ; Chrobak and Buzsáki, 1994 ; Ylinen et al.,
1995 ). These patterns seem to serve companion processes. synchronizes the input pathway into the hippocampus, whereas sharp
waves synchronize the output pathway from the hippocampus back to
neocortical structures. Each potential is associated with more
localized oscillatory field potentials that reflect the temporal
organization of neuronal subsets within 5-25 msec (Bragin et al.,
1995 ; Buzsáki and Chrobak, 1995 ; Ylinen et al., 1995 ).
The sharp wave is a large amplitude (1-3 mV), aperiodic, field
potential observed most prominently in stratum radiatum of the CA1
region (Buzsáki et al., 1983 ; Buzsáki, 1986 ; Suzuki and
Smith, 1987 ). Released from inhibitory constraints associated with (Leung and Yim, 1986 ; Fox, 1989 ; Soltész and Deschénes,
1993 ), the highly interconnected CA3 network exhibits population
bursts. The burst of the CA3 network produces a field excitatory
postsynaptic potential (EPSP) (a sharp wave) in the target of the CA3
Schaffer collaterals, the dendrites of CA1 pyramidal cells, and
interneurons. The massive depolarization of CA1 sets into motion a
short-lived, dynamic interaction between these cell populations. The
product of this interaction is an oscillatory field potential (ripple)
within stratum pyramidale and a phase-related discharge of the CA1
network at 200 Hz (Buzsáki et al., 1992 ). The synaptic currents
mediating the ripple are rhythmic inhibitory postsynaptic potentials
(IPSPs) near the soma of CA1 neurons produced by a high-frequency
discharge of CA1 basket cells and other interneurons (Ylinen et al.,
1995 ). Although interneurons discharge at a high frequency, CA1
pyramidal cells, excited by the CA3 input yet constrained by the
interneuron barrage, typically fire once or not at all. Throughout the
entire CA1 network, however, a large number of pyramidal cells reach
discharge threshold on each ~5 msec wave of the ripple.
The present study examined the interaction between this synchronized
output of CA3-CA1 and the output neurons of a larger integrated
network that includes the subiculum and deep layers of the
presubiculum, parasubiculum, and EC. We found that similar to the CA1
region, each output population of the hippocampal-entorhinal network
produces an organized, short-lived, fast oscillation of their
discharging neurons concurrent with CA1 ripples.
MATERIALS AND METHODS
Animals and surgery. Twenty-four adult
Sprague-Dawley rats were used in the following experiments. For
surgery, rats were anesthetized with a ketamine cocktail (4 ml/kg)
consisting of 25 mg/ml ketamine, 1.3 mg/ml xylazine, and 0.25 mg/ml
acepromazine. After a midline scalp incision, two to four burr holes
were drilled in the skull over the hippocampal and retrohippocampal
cortices. Two or three sets of four 50 µm tungsten wires were
positioned into the dorsal hippocampus/subicular regions
[anterior-posterior (AP), 2.5, 5.0, 7.5 from bregma;
medial-lateral (ML), 1.5, 2.5, 4.0; dorsal-ventral (DV), 2.0-4.0 from
the skull and above retrohippocampal regions (AP, 7.5-9.0; ML,
3.0-5.0)]. One or more sets were chronically fixed, whereas the other
was attached to a drive consisting of a brass post and a single machine
screw. The latter allowed for optimal, postsurgical positioning of
electrodes. One or two single tungsten microelectrodes (0.5-3.0
M ) mounted to similar drives were positioned over either
or both retrohippocampal areas (AP, 7.5-9.0; ML, 3.0-5.0). These
mounts allowed for the slow passage of the microelectrode through the
retrohippocampal region. In two animals, a 16-channel silicon probe
(100 µm tip separations) (Bragin et al., 1995 ) was positioned via a
movable microdrive into the EC. A pair of 150 µm wires were also
positioned in the angular bundle (AP, 7.2; ML, 4.2; DV, 4.0) or CA3
region (AP, 4.0; ML, 4.0; DV, 4.0) for stimulation. Two stainless steel
watchscrews driven into the bone above the cerebellum served as
indifferent and ground electrodes. Two or more additional support
screws were positioned, and the entire ensemble was secured to the
skull with dental acrylic. All electrodes indifferent, ground, and
stimulating were attached to male pins that were secured in a
rectangular 3 × 4 pin array and secured with dental acrylic.
Recording. Bioelectrical activity was recorded in the freely
behaving rats during movement, awake immobility, or distinct sleep
stages. The headstage of the animal (male pins) was connected to
sixteen MOSFET-input operational amplifiers mounted in a female
connector. This direct amplification at the headstage serves to
eliminate cable movement artifacts (Buzsáki et al., 1989 ). An
attached cable fed into a rotating swivel (Biela, Irvine, CA) allowed
for the free rotation of the recording cable and movement of the rodent
within a standard plexiglas home cage. An amplifier system (Grass
Neurodata Acquisition System, Quincy, MA) and an analog-to-digital
hard/software system (RC Electronics, Santa Barbara, CA) run on a PC
computer allowed for direct visualization and storage of electrical
activity. Wide band signals (1 Hz-5 kHz) were sampled at 10 kHz (100 µsec) and stored on optical disks.
After optimization of hippocampal microelectrodes for detection of
ripples (200 Hz oscillations) within stratum pyramidale of CA1 and
sharp waves within stratum radiatum of CA1, the tungsten microelectrode
or multielectrode 50 µm wires were lowered through retrohippocampal
structures. Discriminable units and/or prominent oscillations were
recorded during both sharp waves (awake immobility) and states
(locomotor activity and paradoxical sleep); 100-400 (400 msec) epochs
triggered by the occurrence of a sharp wave and/or ripple were
recorded. When possible (depending on the stability of unit recording),
additional continuous epochs (30-90 sec) were recorded during both
sharp waves and states. When prominent retrohippocampal
oscillations or a prominent retrohippocampal sharp potential was
observed, additional epochs triggered by the occurrence of these events
were recorded. After completion of a single pass of the movable
microelectrode(s), rats were anesthetized with pentobarbital and
perfused with the electrode in situ.
Data processing and analysis. Unit activity and field
potentials were filtered digitally (120 dB/octave: unit, band pass
0.5-5.0 kHz; high-frequency ripples, band pass 100-400 Hz) and
analyzed off-line on a 486/33 or an IBM RS 6000 computer or both.
Putative single units were verified by the absence of spikes 1 msec
(typically >3-5× baseline amplitude) in autocorrelograms, reflecting
the refractory period. Remaining unit activity (units >2× baseline,
with interspike intervals <1 msec) were considered multiunit. Ripple
peaks were detected after off-line filtering (100-400 Hz), using a
peak-detection algorithm.
Single and multiunit activity were cross-correlated with local ripple
peaks and local ripple peaks with CA1 ripples, using the ripple peaks
as the zero reference point. Local field averages were obtained by
averaging wide-band and filtered signals, using ripple peaks or unit
pulses as the zero reference.
Histology. Tissue was processed using either thionin stain
or a modified silver method that allows for direct visualization of
damaged neurons (Gallyas et al., 1990 ). The latter technique allowed
for more direct visualization, and thus localization, of neurons at the
electrode tip. Briefly, after completion of the experiments, the rats
were anesthetized deeply and perfused through the heart with
cacodylate-buffered saline, pH 7.5, followed by a cacodylate-buffered
fixative containing 4% paraformaldehyde and 5.9% calcium chloride, pH
7.5. Brains were left in situ for 24 hr, removed, and then
postfixed in the same solution for 1 week. The brains were sectioned on
a vibratome at 80 µm, dehydrated with propanol, and placed in an
esterifying solution (98% propanol, 1.2% sulfuric acid) at 56°C for
16 hr. After rehydration and sectioning, they were processed according
to the following procedure: (1) pretreatment in 8% acetic acid for 10 min, (2) washing in water for 1 min, (3) physical development with
tungstosilicic acid for ~10 min, and (4) washing in 1% acetic acid.
Finally, the sections were dehydrated, mounted on slides, and
coverslipped.
RESULTS
Coupling of CA1 ripples along the long axis of the hippocampus
Transient high frequency oscillations (ripples) at ~200 Hz were
observed as electrodes traversed near the CA1 pyramidal cell layer
coincident with hippocampal sharp waves. CA1 ripples are defined as a
series of 5-15 oscillatory waves of varying amplitude/duration with a
peak-to-peak time of ~5 msec (Figs. 1,
2). Our measurements along the longitudinal axis of the
hippocampus indicate that several cycles (three to five) of the
dynamically developing CA1 ripples are coherent along this dimension
for distances of 4-5 mm (n = 6; Fig. 1E). It is
important to note that the waxing and waning of CA1 ripples is a
localized phenomenon, which is likely to represent the local
development of synchrony among subpopulations of CA1 interneurons.
Figure 2 illustrates that although distant sites within the dorsal CA1
region are on average coherent over several cycles of a ripple, ripples
at specific sites can occur quite independently. Although the absence
of a prominent ripple in the contralateral hippocampus was not unusual,
occurring 30-50% (Fig. 2C), the absence of a prominent
ipsilateral ripple was rare (<5%; Fig. 2B). Ripples
developed in both hemispheres of the hippocampus virtually
simultaneously, with cross-correlograms demonstrating peak occurrence
near the zero-reference ripple; however, there was no
cycle-by-cycle synchrony between ripples in the contralateral
hippocampus (Fig. 1F).
Fig. 1.
CA1 ripple and associated neuronal events in the
ipsilateral and contralateral CA1 regions. A, Recording
locations in ipsilateral and contralateral CA1 regions of hippocampus.
B, Hippocampal sharp wave is a synchronized field EPSP in
the apical dendritic targets of the CA3 Schaffer collateral input. This
depolarization sets into motion a short-lived population interaction
between CA1 pyramidal cells and interneurons whose product is an
oscillatory field potential (200 Hz) and phase-related discharge of CA1
neurons. Typically, a CA1 pyramidal cell fires a single spike in
association with a local ripple (as shown). Upper and
middle traces, recording from pyramidal layer (100-400 Hz
and 0.5-5.0 kHz, respectively). Bottom trace,
simultaneously recorded field potential (1-50 Hz) from stratum
radiatum. C, Average ripple recorded in septal extent of the
dorsal CA1 region. Relationship between negative peak of CA1 ripple (as
shown in C) and locally recorded single and multiunit
(D) activity and CA1 ripples recorded in the ipsilateral
(E) and contralateral hippocampus (F). Note that
ripples with the ipsilateral dorsal CA1 region are coherent for three
to four cycles of the oscillation, whereas those recorded in the
contralateral hippocampus are not.
[View Larger Version of this Image (22K GIF file)]
Fig. 2.
Ripples at various positions with the CA1 region
can emerge independently. A, B, C, Single 200 msec traces
recorded concurrently in the ipsilateral (~5 mm distance from
reference CA1 ripple) and contralateral CA1 pyramidal cell region.
Ripples typically occur concurrently at various sites within CA1
(A), but the occurrence, amplitude, and duration can be
independent at various sites within CA1 (B, C).
[View Larger Version of this Image (18K GIF file)]
Coupling of retrohippocampal neurons to local field, and
CA1 ripples
While examining the relationship between CA1 ripples and the
discharge of retrohippocampal neurons, we observed prominent local
field oscillations within the subicular and deep layer presubicular,
parasubicular, and entorhinal cortices. We examined the relationship
between these retrohippocampal ripples and unit discharge as well as
the relationship of the retrohippocampal ripples to CA1 ripples. Given
that principle neurons discharge only on some limited number of local
ripple events, ripple-ripple cross-correlograms yield a more accurate
reflection of population synchrony between CA1 neurons and
retrohippocampal neurons.
At all sites within the hippocampal-entorhinal output network where
high-frequency ripples could be observed, single and multiunit activity
was correlated to the negative phase of the local field oscillation
(Figs. 3, 4, 5), although
the degree of modulation for multiple cycles of the oscillation varied
from site to site. This variation is likely to depend on the position
of the recording electrode within the synaptic field generating the
ripple, which may not be optimal for recording well isolated units, as
well the number of times a neuron discharges during any given ripple.
Thus, for example, the subicular neuron illustrated in Figure 3 seems
better modulated because this neuron tended to fire more than once,
often exhibiting multiple spikes, on any given ripple with which it
discharged.
Fig. 3.
CA1 ripple and associated neuronal events in the
ipsilateral and contralateral subiculum. A, Single 400 msec
sweep with ripple doublets recorded at three sites and subicular unit.
B, Cross-correlograms of ipsilateral (black) and
contralateral (gray) subicular ripples to the peak of the
CA1 reference ripple (n = 224 CA1 ripples). Note the
prominent wave-by-wave coherence on the ipsilateral side and its
absence in the contralateral subiculum. Insets in
B illustrate position of electrodes in the dorsal subiculum
(figures as from Swanson, 1992 ). C, Averaged subicular
ripple (n = 193) and its relation to single
(black) and multiunit (gray) activity recorded at
the same site. D, Zero reference was negative peak of the
local subicular ripple. Inset in D,
autocorrelogram of single unit.
[View Larger Version of this Image (32K GIF file)]
Fig. 4.
CA1 ripple and associated neuronal events in the
deep layers of the ipsilateral presubiculum. A, Single 400 msec sweeps recorded from CA1 and the ipsilateral presubiculum.
Top trace illustrates the discharge of a single (*) and
multiunit presubicular neurons. B, Cross-correlogram of
ipsilateral presubicular ripple to the peak of the CA1 reference ripple
(n = 257 CA1 ripples). Inset in B
illustrates position of electrode in the dorsal presubiculum.
C, Averaged presubicular ripple (n = 213).
D, Cross-correlograms of single (black) and
multiunit (gray) activity and presubicular ripples; zero
reference was negative peak of local presubicular ripple.
Inset in D, Autocorrelogram of single unit.
[View Larger Version of this Image (26K GIF file)]
Fig. 5.
CA1 ripple and associated neuronal events in the
deep layers of the ipsilateral entorhinal cortex. A, Single
400 msec sweeps with concurrent ripples in CA1 and the ipsilateral EC.
Top trace, discharge of entorhinal neurons at the site where
the entorhinal ripple was recorded. B, Cross-correlograms of
the ipsilateral entorhinal ripple with the peak of CA1 ripple as zero
reference (n = 211). Note the absence of ripple-related
modulation in the cross-correlogram. Inset in B
illustrates position of electrodes in the rostral EC. C,
Averaged entorhinal ripple (n = 213). D,
Cross-correlograms of single (black) and multiunit
(gray) activity and entorhinal ripples; zero reference was
negative peak of entorhinal ripple. Inset in D,
Autocorrelogram of single unit.
[View Larger Version of this Image (23K GIF file)]
Figure 3 illustrates that ripples in the ipsilateral dorsal subiculum
were coherent with CA1 ripples for multiple cycles (n = 4;
Fig. 3B), as was observed at sites across the dorsal CA1
region. Ripples at contralateral subicular sites occurred concurrently
but were not coherent on a cycle-by-cycle basis (Fig. 3B).
Both single (n = 13) and multiunit subicular unit activity
were phase-related to the negative peaks of these local high-frequency
oscillations (Fig. 3).
High-frequency ripples were also observed near the deep layers of the
presubiculum. Figure 4 illustrates the relation of presubicular ripples
to an ipsilateral CA1 ripple. Note the qualitative decrement in
cycle-by-cycle coherence in the ripple-ripple cross-correlogram (Fig.
4B), although the peak of the cross-correlogram indicates
that these dynamically developing events occur virtually simultaneously
in both structures. The peaks of ripple-ripple cross-correlograms did
not indicate any significant (>5 msec or a single cycle) lag in the
occurrence of presubicular ripples as compared with CA1 ripples (Fig.
4B). Single presubicular (n = 8) and multiunit
neurons recorded at all sites within the deepest layers near the
overlying white matter were modulated powerfully by local
high-frequency oscillations (Fig. 4A,D), discharging on the
negative peak of the local oscillation.
Entorhinal ripples were more variable and exhibited fewer oscillatory
waves per ripple (Figs. 5A, 6). Although an occasional
entorhinal ripple preceded the occurrence of CA1 ripples, the majority
(~95%) occurred either virtually simultaneously (±5 msec) or were
delayed (>5-30 msec peak-amplitude wave to peak-amplitude wave) as
compared with a dorsal CA1 site (Figs. 5A,D;
6A,D).
Fig. 6.
Depth profile of an entorhinal sharp wave and its
relation to a CA1 ripple. A 16-channel silicon probe (arrow)
was used to record concurrently at multiple laminar sites within the
entorhinal cortex. The figure illustrates the relation of this large
depolarizing input to the dendritic fields of layers V-VI and III
neurons throughout the broad expanse of layers IV and III of the
entorhinal cortex. Image (right) illustrates the position of
the silicon probe with its tip near the superficial border of the
EC. ab, Angular bundle.
[View Larger Version of this Image (55K GIF file)]
Entorhinal and parasubicular single and multiunit activity were
phase-related to local ripples, although the degree of oscillatory
modulation was clearly less than at CA1, subicular, or presubicular
sites (Fig. 5A,D). Entorhinal neurons were phase-related to
the negative peak of the local oscillation (n = 17), with
several neurons (n = 6) exhibiting two or three oscillatory
peaks in their cross-correlogram (Fig. 5D). It also was
observed that the peak amplitude entorhinal oscillations were not the
most prominent within layers V-VI, but were better expressed in the
most superficial aspect of layers V, IV, and III.
Entorhinal ripples, observed as electrodes penetrated layers V-VI and
entered the broad expanse of layer III, were associated with a
prominent negative-going wave that we refer to as entorhinal sharp
waves (Figs. 6, 7). This slow potential
reversed in polarity near layer II, suggesting that it represents a
synchronized field EPSP in the apical dendritic zone of layer V-VI
neurons. This entorhinal sharp wave is similar to that described
previously by Paré and colleagues (1995) in the cat. These
authors also observed that deep layer EC neurons discharge regularly in
association with these events, whereas superficial neurons discharged
much less frequently.
Fig. 7.
CA1 ripple and associated high-frequency
oscillations in the EC. A, Single 400 msec sweeps with
concurrent ripples in the CA1 region and both hemispheres of the EC.
Note the time lag and lower frequency of the entorhinal oscillations.
B, Averaged extracellular fields (wide band) in
the hippocampus and ipsilateral EC triggered by the negative peak of
CA1 ripples (n = 243). Top trace is average
extracellular fields in stratum oriens. Bottom traces are
averaged entorhinal sharp waves illustrating reversal near the border
of layers II-III. C, Average extracellular fields in the
same EC locations triggered by the negative peak of the entorhinal
high-frequency oscillation. Top and bottom traces
(1-5 kHz) are layers III and II sites as shown in B,
respectively. Middle traces are the same sites filtered
(100-400 Hz) for ripples. Note reversal of high-frequency oscillation.
D, Relation of contralateral entorhinal ripples
(black) and ipsilateral CA1 ripples (gray) to the
negative peak of the ipsilateral entorhinal ripple (same zero reference
as C).
[View Larger Version of this Image (25K GIF file)]
Figure 7 illustrates the relationship between entorhinal ripples and
their associated entorhinal sharp waves to the hippocampal CA1 ripple.
Correlations were observed between the occurrence of these entorhinal
sharp waves and CA1 ripples in all animals (Figs. 6, 7); however, there
was an obvious variability in degree of concurrence of these field
events. This variation may represent differences in the topographical
innervation of the EC from CA1. The topography of CA1 to the EC is such
that the septal CA1 and subiculum project more to the lateral aspect of
the EC, whereas the temporal CA1 projects to the more medial aspect of
the EC (Amaral and Witter, 1995 ). We have a limited sample over the
rostral-caudal, medial-lateral dimension, and although Figure
illustrates a prominent relationship between dorsal CA1 and
the caudal-medial extent of the EC, additional studies will be
needed to define the topography of the observed physiological
connectivity.
DISCUSSION
The present study demonstrates novel findings that integrate the
ripple-related discharge of CA1 neurons during hippocampal sharp waves
with electrophysiological events occurring throughout the output
networks of the hippocampal-entorhinal axis. First, during hippocampal
sharp waves, local field oscillations are synchronous throughout the
dorsal CA1 region, as well as in the subicular and deep layers of the
presubicular, parasubicular, and entorhinal cortices. Second,
throughout the hippocampal-entorhinal output network, discharge of
neurons synchronized to the negative peak of locally developing ripples
in each region. Third, entorhinal ripples are associated with a
negative-going entorhinal sharp wave that reverses in polarity near the
border of layers II-III. This latter phenomenon may reflect the
synchronized depolarization of the apical dendritic field of layer
V-VI neurons by the hippocampal sharp wave-related discharge of CA1,
subiculum, and presubiculum neurons that synapse in this region.
Thus, in association with hippocampal sharp waves, highly organized
discharges occur throughout the entire output network of the
hippocampal-entorhinal axis. These organized discharges bring tens of
thousands of neurons within these interconnected networks together so
that they discharge in discrete subsets on each of several
high-frequency oscillatory waves. This coordinated population output is
likely to have a potent impact on many forebrain targets.
Temporal structure in hippocampal-entorhinal neuronal networks: a
role for interneurons
Our observations demonstrate that in association with hippocampal
sharp waves, there are locally developing field oscillations throughout
the output network of the hippocampal-entorhinal axis. The
extracellulary recorded oscillatory fields may reflect synchronous
membrane oscillations in pyramidal neurons caused by rhythmic IPSPs.
Previous findings demonstrate that the 200 Hz field oscillation
observed within CA1 reflects synchronized IPSPs in the perisomatic
region of CA1 neurons (Ylinen et al., 1995 ). Networks of interneurons
can achieve rhythmic, synchronous population discharges, which then
exert a hyperpolarizing oscillation on the membrane potential of
pyramidal neurons (Michelson and Wong, 1994 ; Whittington et al., 1995 ;
Traub et al., in press). Such oscillations, occurring in the context of
a depolarizing input, can impose a periodic fluctuation in the
pyramidal cell membrane close to, but below, discharge threshold.
Although CA1 interneurons discharge near 200 Hz, CA1 pyramidal cells
typically discharge once or not at all during a ripple. The discharge
of CA1 pyramidal cells is thus highly constrained, despite a massive
depolarization from the CA3 input.
We suggest that the locally developing field oscillations throughout
the hippocampal-entorhinal output network develop in a manner
analogous to that observed in CA1. Thus, feed-forward excitation
simultaneously drives low-threshold networks of interneurons that
discharge at a high frequency, whereas pyramidal cells discharge in
population bursts: the population burst driven by feed-forward
excitation, but concurrently constrained by the influence of the local
interneuron barrage. The high degree of transient synchrony observed
throughout the network is likely to reflect the anatomical arrangement
of (1) feed-forward excitatory projections and/or (2) long-range
inhibitory projections. Coupling across regions may be achieved by
GABAergic interneurons with wide-ranging axon collaterals (Sik et al.,
1995 ) and/or gap junctions, and such interneuronal ``supernetworks''
may co-operatively entrain large populations of pyramidal cells in the
hippocampal-entorhinal axis (Buzsáki and Chrobak, 1995 ).
Fast oscillations within the hippocampal/retrohippocampal output
pathways during sharp waves: coordinated activity in a distributed
neural network
The temporally coordinated activity of neurons within spatially
distributed networks is an important functional unit within the nervous
system (Hebb, 1949 ; Konorski, 1949 ). Rhythmic field potentials reflect
temporal frameworks for synchronizing neural activity, i.e., for
bringing neuroanatomically distributed and sparsely connected neurons
together in time (Buzsáki et al., 1983 ; Steriade et al., 1990 ,
1993 ; Gray, 1994 ). Although sharp waves are aperiodic, they are
associated with a high-frequency oscillation within the entire
hippocampal-entorhinal output network. Synchronized neural discharges
occur within this large network during these events. It is important to
note that synchronized oscillations and unit discharges do not occur
throughout the entire network with each and every sharp wave; rather
they emerge within varying topographical locations and involve varying
subpopulations of neurons. The degree of synchronization between any
two sites within the network varies from event to event and is likely
to reflect anatomical/synaptic connectivity. Clearly, the degree of
synchronization across the dorsal CA1 and adjacent subicular region,
over many ripple events, is much greater within any given hemisphere as
compared with the contralateral hemisphere (Figs. 1, 2, 3) or ipsilateral
retrohippocampal sites (Figs. 4, 5, 6). As suggested above, the degree of
synchronization within/across regions may reflect the anatomical
interconnectivity of interneuronal networks. In this regard, it is
important to appreciate the extensive interconnectivity of GABAergic
interneurons within the CA1 region (Sik et al., 1995 ), the lack of
substantial interconnections among CA1 pyramidal neurons (Christian and
Dudek, 1988 ; Thomson and Radpour, 1991 ), and the lack of any
significant contralateral projections from either CA1 interneurons or
pyramidal neurons (Amaral and Witter, 1995 ).
Bringing neurons within the hippocampal-retrohippocampal network
together in time on such a short time-scale provides a potent means of
enhancing their impact on common postsynaptic targets. If convergent
activation of neurons is related to potentiating synaptic efficacy
(Bliss and Lømo, 1973 ; Bliss and Collinridge, 1993 ), then the
convergent activity of the hippocampal-entorhinal output network is a
potent, endogenous, means for modifying the synaptic
connectivity within this network and in its anatomical targets
throughout the forebrain.
Relevance of hippocampal-entorhinal population oscillations to
cognitive/computational processes
We have suggested that formation and consolidation of memories
within this network involves two distinct companion processes
(Buzsáki, 1989 ; Chrobak and Buzsáki, in press). The initial
transfer of information into the circuitry of the hippocampus is
thought to be supported by -modulated oscillations within the
entorhinal-dentate axis and at their targets within CA3-CA1 (Bragin
et al., 1995 ; Chrobak and Buzsáki, 1995 ; in press). This on-line
modification of preexistent network connectivity serves as a means of
imprinting information on the output circuitry of the hippocampus. Free
from the ongoing transfer of input into its circuitry, the
CA3-CA1-retrohippocampal network then engages in synaptic modification
of its own and target neocortical networks. The synchronization of the
output circuitry associated with each sharp-wave burst is thought to
play a fundamental role in a protracted consolidation process,
``whereby medial temporal lobe structures direct the gradual
establishment of memory representations in neocortex'' (Squire and
Alvarez, 1995 ; also see Marr, 1971 ). This general framework is
compatible with a considerable volume of evidence documenting the
temporal gradient of retrograde amnesia associated with temporal lobe
insult (Ogden and Corkin, 1991 ; Squire, 1992 ; Cho et al., 1993 ; Kim et
al., 1995 ). This literature demonstrates that the
hippocampal-entorhinal substrates participate in a consolidation
process that takes place after the acquisition of information and over
a variable period of minutes, hours, days, weeks, and even many months
transfers representations, or access to representations, to a
neocortical substrate. This framework is also compatible with recent
multiunit recordings in freely behaving rats demonstrating correlated
neural activity among pairs of neurons as a consequence of recent
experience that is maintained during subsequent sleep periods (Wilson
and McNaughton, 1994 ; Kudrimoti et al., 1995 ), as well as theoretical
modeling studies that have examined the relative efficiency of this
dual-process approach for modifying neural networks (McClelland et al.,
1995 ).
We suggest that the major physiological role of this organized network
burst is long-term alterations in synaptic efficacy. The synchronized
200 Hz discharge of the hippocampal-entorhinal output network (1)
occurs within the appropriate anatomical pathway, so as to convey the
outcome of hippocampal processing to neocortical networks, (2) occurs
within a logical time domain, so as to be relevant to an ``after the
fact'' consolidation process, and (3) may provide the prerequisite
depolarizing force needed to produce synaptic modifications of
neocortical networks.
Entorhinal sharp waves: the impact of the output network on the
input (layers II-III) network
Cells within the deep layers of the presubiculum and parasubiculum
appear continuous with the principal cell layer of the subiculum and
the deep layers of the EC (Amaral and Witter, 1995 ). Our present
findings support the continuity of this functionally integrated output
network.
Previous findings demonstrated that the superficial layer (II-III)
neurons within these regions do not seem to be influenced by
hippocampal sharp waves (Chrobak and Buzsáki, 1994 ). Anatomical
circuits exist for the activation of layer II-III neurons by the
hippocampal-entorhinal output network, which would then allow for
reentrant activation of the hippocampus via the perforant path;
however, the physiological activity of this circuitry seems to be
constrained powerfully by dominant inhibitory influences within the
superficial layers (Finch et al., 1986 , 1988 ; Jones and Heinemann,
1988 ; Bartesaghi et al., 1989 ; Jones and Lambert, 1990 ; Jones and Buhl,
1993 ; Chrobak and Buzsáki, 1995 ; Paré et al., 1995 ). This
dominant inhibition, however, may provide mechanisms for a
circumscribed activation of superficial layer neurons, and this
possibility is under investigation. On the other hand, a general
compromise of this inhibition would expose this circuitry to an
unaccustomed excitatory barrage. Failure of inhibition at this critical
juncture is likely to play a prominent role in the transition of
physiological network bursting to pathophysiological reverberating
epileptiform activity (Paré et al., 1992 ; Jones, 1993 ). We
believe that understanding the basic physiology of this intricate
neural machinery at the level of an operational system is essential for
describing the neural substrate of memory formation as well as the
pathological dysfunction of this substrate as manifest in temporal lobe
epilepsy and Alzheimer's dementia.
FOOTNOTES
Received Nov. 30, 1995; revised Jan. 18, 1996; accepted Jan. 22, 1996.
This work was supported by the National Institutes of Health (NS34994,
1P41RR09754), National Science Foundation, Human Frontiers Science
Project, the Whitehall Foundation (G.B.), and the Alzheimer's
Association (J.J.C.). We thank Drs. H. Read and A. Bragin for all their
help, comments, and discussion, and K. Wise and J. Hetke for supplying
silicon probes.
Correspondence should be addressed to Gyorgy Buzsáki, CMBN,
Rutgers University, 197 University Avenue, Newark, NJ
07102.
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