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The Journal of Neurophysiology Vol. 87 No. 3 March 2002, pp. 1213-1221
Copyright ©2002 by the American Physiological Society
Center for Molecular and Behavioral Neuroscience, Rutgers University, Newark, New Jersey 07102
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ABSTRACT |
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Pelletier, J. Guillaume and Denis Paré. Uniform Range of Conduction Times From the Lateral Amygdala to Distributed Perirhinal Sites. J. Neurophysiol. 87: 1213-1221, 2002. Much data indicate that the perirhinal (PRH) cortex plays a critical role in declarative memory and that the amygdala facilitates this process under emotionally arousing conditions. However, assuming that the amygdala does so by promoting Hebbian interactions in the PRH cortex is hard to reconcile with the fact that variable distances separate amygdala neurons from their PRH projection sites. Indeed, to achieve a synchronized activation of distributed PRH sites, amygdala axons should display a uniform range of conduction times, irrespective of distance to target. To determine if amygdala axons meet this condition, we measured the antidromic response latencies of lateral amygdala (LA) neurons to electrical stimuli delivered at various rostrocaudal levels of the PRH cortex in cats anesthetized with isoflurane. Although large variations in antidromic response latencies were observed, they were unrelated to the distance between the PRH stimulation sites and LA neurons. To determine whether this result was an artifact due to current spread, two control experiments were performed. First, we examined the antidromic response latency of intrinsic PRH neurons. Although we used the same methods as in the first experiment, the antidromic response latency of PRH neurons to electrical stimuli applied in the PRH cortex increased linearly with the distance between the stimulating and recording sites. Second, we measured the antidromic response latency of PRH neurons projecting to the LA. In this pathway, we also found a statistically significant correlation between conduction times and distance to target. Thus these results support the intriguing possibility that the conduction velocity and/or trajectory of LA axons are adjusted to compensate for variations in distance between the LA and distinct rostrocaudal PRH sites. We hypothesize that because of their uniform range of conduction times to the PRH cortex, LA neurons can generate short time windows of depolarization facilitating Hebbian associations between coincident, but spatially distributed, activity patterns in the PRH cortex. In this context, the temporal scatter of conduction times in the LA to PRH pathway is conceived as a mechanism used to lengthen the period of depolarization to compensate for conduction delays within intrinsic PRH pathways. In part, this mechanism might explain how the amygdala promotes memory storage in emotionally arousing conditions.
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INTRODUCTION |
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In various
neuronal networks, axonal conduction times obey clear functional
constraints. In the avian auditory system, for instance, where accurate
timing of afferent signals is essential, the conduction time between
the cochlear nucleus and its ipsi- and contralateral brain stem targets
is kept constant by lengthening the path of axons ending ipsilaterally
(Carr and Konishi 1990
). Similarly, in fish electric
organs, a synchronized activation of electrocytes is achieved by
increasing the conduction velocity of the longer axons and lengthening
the path of fibers ending in the closer part of the electric organ
(Bennett 1970
). In the preceding examples, the function
of the system was known. Could an analysis of conduction times yield
insights into the role of systems whose function is poorly understood?
The present study aimed to test this in the amygdalo-perirhinal network.
Despite the fact that the amygdala and perirhinal (PRH) cortex are
reciprocally connected (Krettek and Price 1977b
;
Russchen 1982
), lesion studies have generally emphasized
their distinct role. Indeed, PRH lesions were found to interfere with
recognition and associative memory (Suzuki 1996
;
Suzuki and Eichenbaum 2000
), whereas amygdala lesions
had little impact on performance in such tasks (Parker and
Gaffan 1998
; Zola-Morgan et al. 1989
). Instead, amygdala lesions were found to prevent the acquisition of classically conditioned fear responses (Davis et al. 1994
;
Kapp et al. 1992
; LeDoux 2000
), an issue
that remains controversial (Cahill et al. 1999
).
Yet, other data suggest that the amygdala and PRH cortex are
functionally coupled. Indeed, PRH lesions performed after classical fear conditioning interfere with conditioned fear responses
(Campeau and Davis 1995
; Corodimas and LeDoux
1995
; Rosen et al. 1992
). In humans, emotionally
arousing stories are better recalled than neutral ones, and amygdala
lesions abolish this effect (Adolphs et al. 1997
;
Cahill et al. 1995
). Moreover, imaging studies have found a high correlation between recall of emotionally arousing or
neutral material and the amount of amygdala activation observed when
these stimuli were first presented (Cahill et al. 1996
;
Canli et al. 2000
; Hamann et al. 1999
).
These and other findings suggest that the amygdala promotes
memory-storage processes in brain areas that are involved in
declarative memory (Cahill 2000
; Cahill and McGaugh 1998
; McGaugh 2000
), such as the PRH cortex.
How could the amygdala facilitate memory formation in the PRH cortex?
Most biological theories of memory posit a Hebbian mechanism (Hebb 1949
) that would strengthen synapses linking
co-active neurons (Martin et al. 2000
). However,
experimental studies have revealed that the timing of activity in
pre- and postsynaptic neurons is critical: potentiation of
cortical synapses occurs when excitatory postsynaptic potentials
(EPSPs) narrowly precede postsynaptic firing and depression develops
when postsynaptic discharges precede presynaptic inputs (reviewed in
Abbott and Nelson 2000
). As a result, assuming that the
amygdala modulates memory storage by facilitating Hebbian interactions
in the PRH cortex confronts us with an interesting problem; the PRH
area is a long strip of cortex (12 mm in the cat) and the LA is located
at rostral PRH levels. Thus LA axons must travel variable distances to
reach different rostrocaudal PRH sites. If the amygdala favors Hebbian associations between coincident but spatially distributed activity patterns in the PRH cortex, amygdala axons should display a uniform range of conduction times despite the varying distances they must travel to reach their targets. The present study was undertaken to test
this prediction.
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METHODS |
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Most amygdalo-PRH efferents stem from the basolateral amygdaloid
complex (Krettek and Price 1977a
,b
), a group of nuclei
including the lateral (LA), basolateral, and basomedial nuclei. The LA
is notable in this respect because its main extra-amygdaloid target is
the PRH cortex (Krettek and Price 1977b
). Thus the
present study focused on the conduction times of LA neurons.
Surgery
Experiments were conducted in agreement with ethical guidelines of the Canadian Council on Animal Care. Cats (2.5-3.5 kg) were preanesthetized with a mixture of ketamine and xylazine (11 and 2 mg/kg, im) and artificially ventilated with a mixture of ambient air and 2% isoflurane. The end-tidal concentration in CO2 was kept at 3.7 ± 0.2% and the body temperature was maintained at 37-38°C with a heating pad. The level of anesthesia was assessed by continuously monitoring the electroencephalogram. The bone overlying the amygdala and PRH cortex was removed on both sides and the dura mater opened.
Two types of experiments were performed. The first series of
experiments aimed to determine how the antidromic response latency of
LA neurons fluctuated as a function of distance to their PRH projection
sites. To this end, three concentric stimulating electrodes separated
by 4.5 mm in the rostrocaudal axis were inserted in the PRH cortex
(Fig. 1A1). Then, an array of
four tungsten microelectrodes (2-6 M
at 1 kHz; outer diameter of 80 µm) was lowered stereotaxically into the LA nucleus, as shown in Fig.
1A1. To construct the array, small holes were drilled in a
circular Teflon block and the electrodes were inserted into them prior
to the experiments. This experiment was repeated in both hemispheres of
three cats.
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The second series of experiments aimed to determine how the antidromic response latency of PRH neurons fluctuated as a function of distance to their LA and/or perirhinal projection sites. To this end, stimulating electrodes were inserted in the LA and PRH cortex as shown in Fig. 1A2. Then, an array of six tungsten microelectrodes, arranged in the configuration shown in Fig. 1A2, was lowered stereotaxically into the PRH cortex. This experiment was repeated five times.
During both types of experiments, the microelectrode arrays were
lowered in steps of 4 µm by a piezoelectric micromanipulator. While
moving the microelectrodes, electrical stimuli (0.3 ms, 1 mA, 2 Hz)
were delivered in the PRH cortex to increase the likelihood of finding
responsive cells. When responsive neurons with a high signal-to-noise
ratio (
3) were encountered, the stimulus intensity and duration was
decreased just above threshold (typically 0.05-0.2 ms pulses of
0.1-0.5 mA) and the nature of the response (ortho- vs. antidromic) was
determined. See RESULTS for the criteria used to
distinguish antidromic and orthodromic responses. The evoked activity
of selected neurons was observed on a digital oscilloscope, digitized,
and stored on tape.
Histological identification of recording and stimulating sites
At the end of the experiments, recording sites were marked with electrolytic lesions (0.5 mA for 5 s). Following this, the animals were given an overdose of barbiturate (sodium pentobarbital, 40 mg/kg, iv) and perfused with 500 ml of a cold saline solution (0.9%) followed by 1 l of fixative, containing 2% paraformaldehyde and 1% glutaraldehyde in 0.1 M phosphate-buffered saline (pH 7.4). The brains were later sectioned on a vibrating microtome (at 100 µm) and stained with thionin to verify the position of the recording electrodes. The sections were collected serially to facilitate estimation of the distance separating recording and stimulating sites.
The microelectrode tracks were reconstructed by combining micrometer
readings with the histological controls. We also estimated the distance
between recorded neurons (Fig. 1, B1, B3, and
B4) and stimulation sites (Fig. 1, B2 and
B3). In doing so, shrinkage due to fixation was taken into
account. The amount of shrinkage was determined by measuring the
postfixation separation of tracts left by tungsten rods inserted 10 mm
apart prior to fixation, as previously described (Paré et
al. 1997
).
Estimation of the distance between the stimulating and recording sites
It is difficult to measure the length of the path taken by axons
to reach their target because axonal trajectories are variable. For
instance, some LA axons take a relatively direct route to the PRH
cortex, whereas others take a circuitous path (Smith and Paré 1994
). Among the latter, some LA axons first course
ventrally (i.e., away from the PRH cortex), then follow the
external capsule, and later turn lateroventrally to end in the PRH
cortex (Smith and Paré 1994
). Thus, recognizing
these difficulties, we only estimated the distance between the
stimulating electrodes and backfired neurons in the rostrocaudal and
lateromedial planes using the Pythagorean theorem.
Analysis
Analyses were performed off-line with the software IGOR (Wavemetrics, OR) and homemade software running on Macintosh microcomputers. Spikes were detected using a window discriminator after filtering (0.3-10 kHz) of the raw waves. Peristimulus histograms of unit discharges were computed.
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RESULTS |
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Database
A total of 1862 neurons were recorded in this study. Histological controls (Fig. 1B) revealed that 484 of these cells were located in the LA nucleus and 508 in the PRH cortex. Examples of histologically confirmed recording sites are shown in Fig. 1 (arrows; LA, Fig. 1B1; PRH, Fig. 1, B3 and B4). Neurons recorded in other amygdala nuclei or cortical fields will not be considered here.
Neurons had to meet at least two of the following criteria to be
classified as antidromically responsive: fixed response latency (
0.2
ms jitter) (Fig.
2A),
collision with spontaneous (Fig. 2B) or orthodromically
evoked (Fig. 2C) action potentials, and ability to follow
high-frequency stimulation (
300 Hz; Fig. 2D).
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Applying these criteria to our sample of neurons revealed that 44% of LA cells (or 215 neurons) were backfired from the PRH cortex in the first series of experiments (Fig. 1A1). However, only 2% (or 5 neurons) of these antidromically responsive cells were backfired from two or more PRH sites. In the second series of experiments (Fig. 1A2), 35% (or 179 neurons) of PRH cells were backfired from the LA and 54% (or 274 neurons) were backfired from the PRH cortex. However, we did not encounter PRH cells that were antidromically responsive to both LA and PRH stimulation sites.
Conduction times from the LA nucleus to the PRH cortex
Figure 3A1 illustrates a representative experiment where six of eight microelectrodes aimed to the LA were histologically confirmed to have reached their target (2 in one hemisphere and 4 in the other). The graph of Fig. 3A1 shows how the antidromic response latency of LA cells (y-axis) fluctuated as a function of the distance between the recording and PRH stimulation sites (x-axis). In this experiment, note that irrespective of distance, antidromic response latencies varied widely within most microelectrode tracks (maximal range in one track: 25 ms). However, no clear change in the range of antidromic response latencies was observed as the distance increased.
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One possible explanation for the latency variations observed within
each track would be that as the electrodes moved dorsoventrally in the
LA, they sampled neurons located at varying distances from the PRH
cortex. If this was true, one would expect antidromic response
latencies to decrease gradually as the electrode approached the dorsal
level of the PRH cortex and then increase progressively as it moved
further ventrally. However, no such relationship was seen. In fact,
neurons whose antidromic response latency varied by
10 ms were
routinely recorded within 100 µm of each other.
Nevertheless, to address this issue quantitatively, we computed the
average latency difference between successively recorded neurons in
eight electrode tracks during which 10 or more PRH-projecting cells
were recorded. Then, we compared this average to that seen in 500 random distributions of the original latencies. The rationale for this
analysis is that if latency variations are caused by changes in the
depth of recorded neurons with respect to that of the PRH cortex, then
the average latency difference between successively recorded neurons
should be smaller than that observed randomly. At odds with this idea,
however, the average latency difference was situated within
1.18 SD
of that found in randomly generated distributions (1.64 SD is required
to reach statistical significance in a one-tailed t-test at
P < 0.05). This result suggests that variations in the
depth of recorded neurons do not account for latency variations
observed within the microelectrode tracks.
As shown in Fig. 3A2, similar results were obtained in all
experiments. In this graph, the antidromic response latency of 215 LA
neurons recorded in 19 microelectrode tracks is plotted as a function
of their distance to PRH stimulating electrodes. A negligible
correlation (r =
0.025, n = 220) was
found between conduction times and distance. Note that the discrepancy
between the number of latencies (n = 220) and LA
neurons (n = 215) results from the fact that five LA
cells were antidromically invaded from two PRH sites.
Such a LA neuron is shown in Fig. 3B. Its antidromic response latencies to two distant (9 mm) PRH stimulation sites (Fig. 3B inset, S1 and S2) differed by <1 ms. This is particularly striking because this cell (*, inset, Fig. 3B) was much closer to S1 than S2. In fact, had the conduction time to S2 been proportional to the response latency observed with S1, the latency difference between responses to S1 and S2 should have been 33 ms. In the five neurons responsive to two PRH sites, the expected latency difference ranged widely (between 13 and 35 ms) because of large cell-to-cell variations in conduction times. Yet, the observed latency difference averaged 1.2 ± 2.05 ms. Thus, even if each of these five cells showed minimal changes in conduction times with distance to target, there were large between-cell variations in conduction times for similar distances to target. In both respects, therefore, the conduction times of these neurons are consistent with that seen in the rest of our sample.
Antidromic response latency of intrinsic PRH axons
In the preceding experiments, it is conceivable that the lack of relationship between distance and conduction time was due to the artifactual backfiring of LA cells by current spread from PRH stimulation sites. However, this possibility would seem unlikely if, using the same methods, we could provide evidence that a different axonal system shows linear increases in latency with distance.
To test this issue, we examined conduction times within the PRH cortex
itself. Indeed, the PRH cortex is endowed with an intrinsic system of
longitudinal connections that spans the entire rostrocaudal extent of
the PRH cortex (Witter et al. 1986
). Moreover, two
recent studies have revealed that the latency of responses mediated by these intrinsic PRH connections increases with distance (Biella et al. 2001
; Martina et al. 2001
).
In support of our findings, the antidromic response latency of PRH
neurons to electrical stimuli applied in the PRH cortex increased
linearly with the distance between the stimulating and recording sites.
The results of a representative experiment are shown in Fig.
4A. In this cat, six
microelectrode tracks were confirmed histologically to have coursed in
the PRH cortex. Despite significant variations in response latency
within each electrode track, a strong correlation (r = 0.81; P < 0.05) was found between conduction times and
distance. In further contrast with LA to PRH projections, the latency
variations observed within each electrode track seemed to increase with
distance. Identical results were obtained when the results of all
experiments were combined (Fig. 4A2). In this context, it is
interesting to note that the associational longitudinal pathway of the
dentate gyrus also shows linear increases in conduction times with
distance (Hetherington et al. 1994
).
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Conduction times from the PRH cortex to the LA
During the aforementioned series of experiments, we also examined the conduction times of PRH neurons projecting to the LA. To this end, one or more stimulating electrodes were inserted in the LA using an oblique approach coursing through the contralateral hemisphere (Fig. 1B3).
As was found in LA neurons projecting to the PRH cortex, antidromic response latencies varied widely within most microelectrode tracks (maximal range in one track: 23 ms), irrespective of the distance separating the stimulating and recording sites (Fig. 4B). Also analogous to amygdalo-PRH projections, these variations were unrelated to the depth of PRH cells. This was determined by computing the average latency difference between successively recorded neurons in six electrode tracks that coursed along the lateral bank of the rhinal sulcus and during which we recorded 10 neurons or more. Then, we compared the average latency difference between successively recorded neurons to that seen in 500 random distributions of the original latencies. On average, the actual average latency difference was situated within 0.2 SD of that found in randomly generated distributions, thus suggesting that the depth of recorded neurons does not account for latency variations observed within the microelectrode tracks.
However, in contrast to amygdalo-PRH projections (Fig. 3A)
but consistent with previous findings (Lang and Paré
1997
), a low but statistically significant correlation
(r = 0.27; P < 0.05) was found between
conduction times and the distance separating the LA stimulating and PRH
recording sites (Fig. 4B).
The possibility that the varying conduction latencies seen between the LA and PRH cortex resulted from stimulation or recording of different PRH layers seems remote. Although we used the lowest possible stimulation intensities, it is unlikely that we activated axons located in specific PRH layers. Even if we did, the difference in axon length between different layers represents a negligible proportion of the total axonal length, whereas latencies varied several fold. Moreover, a similar range of conduction times was seen in electrode tracks that were parallel or perpendicular to the lamination of the PRH cortex.
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DISCUSSION |
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The present study was undertaken to determine whether the conduction times of LA axons are fixed or whether they increase with the distance they must cover to reach their PRH targets. The importance of this issue derives from the hypothesized involvement of the amygdala in promoting memory storage in the PRH cortex and the possibility that Hebbian mechanisms are at play.
Although large variations in conduction times were seen, they were not related to the distance between LA neurons and their PRH projection site. In contrast, a robust correlation was found between conduction times and distance in the intrinsic longitudinal connections of the PRH cortex and a weak one in PRH projections to the LA. In the following account, we will discuss these findings in light of available anatomical and physiological data and consider their significance for amygdalo-PRH interactions.
Conduction times from the LA nucleus to the PRH cortex are not related to distance
Overall, the conduction times of LA axons were independent of distance to target. This finding is intriguing because it implies that axonal conduction velocities and/or trajectories are adjusted to compensate for the varying distances separating LA neurons from their PRH targets.
Several factors suggest that this result was not due to the spurious activation of LA axons by current spread. First, if this was the case, antidromic responses from distant PRH sites should have required higher current intensities. However, a similar range of stimulation intensities was used at all stimulation sites. Second, if current spread was involved, a high proportion of LA neurons antidromically responsive to multiple PRH stimulation sites should have been observed. Yet, only 2% of LA neurons responded to more than one PRH stimulation site. Third, direct neuronal activation by current spread is essentially instantaneous, in sharp contrast with the range of antidromic response latencies observed here. Fourth, using identical methods, we observed that the conduction time of PRH neurons projecting to other rostrocaudal levels of the PRH cortex increased linearly with distance. Thus we feel confident that current spread was not involved and that the conduction times of LA neurons to the PRH cortex are truly independent of distance.
In support of this view, there are numerous examples of central and
peripheral axonal systems showing constant conduction times despite
varying distances to target (Bennett 1970
; Carr and Konishi 1990
; Sugihara and Lang 1993
). In
the olivocerebellar pathway for instance, longer climbing fibers
conduct faster than shorter ones (Sugihara and Lang
1993
), in keeping with the idea that this pathway serves as a
timing circuit for motor control (Lang 2001
;
Llinás et al. 1974
). Similarly, entorhinal sharp potentials, a population phenomenon generated by neurons of the basolateral amygdaloid nucleus, occur synchronously throughout the
rostrocaudal extent of the entorhinal cortex (Paré et al. 1995
) despite the fact that rostral entorhinal sites are
adjacent to the amygdala, whereas caudal ones are
1 cm away in the cat.
Uniform range of conduction times of LA axons allows for a synchronous activation of distributed PRH sites
This study originated from pilot experiments where we observed
that electrical stimulation of the LA nucleus elicited a PRH field
potential whose latency did not vary with rostrocaudal distance (unpublished observations). However, because multiple circuitous pathways might have given rise to this phenomenon, we opted to study
the latency of antidromic responses, an easier phenomenon to interpret.
Other studies support the idea that LA inputs favor synchronized
neuronal activity among distributed PRH sites. Indeed, multiple
simultaneous recordings of LA and PRH neurons at various rostrocaudal
levels have revealed that they show phase-locked oscillatory activity
under anesthesia (Collins et al. 2001
).
It might seem paradoxical to state, on the one hand, that LA inputs can promote synchrony in the PRH cortex, and, on the other, that the conduction times of LA neurons to the PRH cortex vary widely. However, the contradiction is only apparent because, instead of increasing with distance, the range of conduction times is the same irrespective of distance to target. Stated otherwise, it is not the variations in conduction times that promote synchrony, but the fact that the range of conduction times is unrelated to distance.
Consequences for amygdaloperihinal interactions
What could be the significance of this physiological arrangement
in LA projections to the PRH cortex? To address this issue, we now turn
to the anatomical organization of the PRH cortex and amygdalocortical
pathways. In the following paragraphs, the term PRH cortex designates
the peri- and postrhinal regions (reviewed in Burwell
2000
; Witter et al. 2000
), for simplicity.
The PRH cortex relays most neocortical sensory inputs to the
entorhino-hippocampal system and constitutes the main return path for
hippocampo-entorhinal efferents to the neocortex (Burwell and
Amaral 1998a
,b
; Deacon et al. 1983
;
Insausti et al. 1987
; Room and Groenewegen
1986
; Shi and Cassell 1999
; Van Hoesen
and Pandya 1975
; Witter and Groenewegen 1986
;
Witter et al. 1986
). Neocortical inputs are organized
topographically with rostral cortical areas focusing on rostral PRH
levels and posterior ones mainly targeting caudal parts of the PRH
cortex (Deacon et al. 1983
; Room and Groenewegen
1986
).
Superimposed on these transverse neocortical projections is an
intrinsic system of longitudinal connections that span the entire
rostrocaudal extent of the PRH cortex (Witter et al.
1986
). Recently, it was shown that these intrinsic pathways can
distribute neocortical inputs reaching different transverse levels of
the PRH cortex in the rostrocaudal axis (Biella et al.
2001
; Martina et al. 2001
). Surprisingly, these
long-range horizontal connections do not engage inhibitory interneurons
(Martina et al. 2001
). These observations and reports of
N-methyl-D-aspartate (NMDA)-dependent long-term
potentiation (LTP) in the PRH cortex (Bilkey 1996
;
Ziakopoulos et al. 1999
) have led to the suggestion that
the PRH network is biased to favor Hebbian associative interactions
between coincident and spatially distributed inputs (Martina et
al. 2001
).
In light of the present findings, an intriguing possibility would be
that the LA facilitates this process. This idea is supported by the
excitatory nature of amygdalocortical projections. Indeed, amygdalocortical pathways originate from spiny projection neurons (McDonald 1992a
,b
) whose axon terminals are enriched in
glutamate and form asymmetric (presumably excitatory) synaptic
contacts, generally with spiny cortical cells (Paré et al.
1995
; Smith and Paré 1994
). Considering
that cortical inhibitory interneurons generally do not bear spines
whereas principal cells do (Freund et al. 1983
;
Ribak 1978
), these data suggest that LA axons mostly form excitatory (glutamatergic) synapses onto excitatory cortical neurons.
How would the depolarizing inputs originating in the LA facilitate
plastic events in the PRH cortex? Considering the physiological status
of PRH neurons in conscious animals provides insight into this issue.
In the waking state, PRH cells have much lower firing rates
(Collins and Paré 1999
) than neocortical neurons
(Steriade 1978
; Steriade et al. 1974
),
suggesting that their membrane potentials are relatively
hyperpolarized. Because depolarization beyond a certain threshold is
required for NMDA-dependent LTP, we hypothesize that LA inputs push PRH
neurons in a range of membrane potential where Hebbian interactions are facilitated.
Another difficulty is to reconcile the uniform conduction times of LA axons with the progressive increase in antidromic response latency of intrinsic PRH axons with distance to target. Indeed, with respect to Hebbian plasticity, what would be the significance of a synchronized LA input to the PRH cortex if synaptic activity continued to propagate within the PRH cortex after the arrival of LA inputs? In this context, it is interesting to note that even though the conduction times of LA axons are uniform irrespective of distance to target, they do show considerable temporal dispersion. Thus we speculate that this scatter is essential to compensate for the conduction delays within the PRH cortex.
These considerations lead us to propose the following scenario for
LA-PRH interactions. Emotionally arousing conditions, through still
unidentified mechanisms, would increase the excitability of LA
projection cells (Paré and Collins 2000
). In
parallel, the LA nucleus and PRH cortex would receive excitatory inputs from an overlapping set of high-order cortical areas (Deacon et al. 1983
; McDonald 1998
; Room and
Groenewegen 1986
). Excitation would propagate within the LA
nucleus and PRH cortex via their divergent intrinsic pathways
(Krettek and Price 1978
; Witter et al.
1986
). However, the depolarization produced by LA inputs would push the membrane potential of PRH neurons into a range of values favoring NMDA-dependent LTP. Finally, the temporal scatter of conduction times in the LA to PRH pathway would lengthen the period of
depolarization to compensate for conduction delays within intrinsic PRH pathways.
Conclusions
In summary, we hypothesize that the uniform but temporally
dispersed conduction times of LA neurons generates short time windows facilitating Hebbian associations between spatially distributed activity patterns in the PRH cortex. However, a long tradition of
research indicates that interfering with amygdala activity after
encoding decreases recall at a later time (Cahill and McGaugh 1998
; McGaugh 2000
). Thus we speculate that this
mechanism is used by the amygdala to modulate long-term memory storage
in emotionally arousing conditions, not only during the initial
encoding, but possibly later when memory traces are consolidated.
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ACKNOWLEDGMENTS |
|---|
We thank E. J. Lang for comments on an earlier version of the manuscript as well as P. Giguère and D. Drolet for technical support.
This work was supported by the Medical Research Council of Canada and the National Sciences and Engineering Research Council. J. G. Pelletier was supported by a fellowship from Fonds Pour la Formation de Chercheurs et l'Aide à la Recherche.
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FOOTNOTES |
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Address for reprint requests: D. Paré, Center for Molecular and Behavioral Neuroscience, Rutgers University, 197 University Ave., Newark, NJ 07102 (E-mail: pare{at}axon.rutgers.edu).
Received 26 July 2001; accepted in final form 30 October 2001.
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