Volume 16, Number 10,
Issue of May 15, 1996
pp. 3511-3520
Copyright ©1996 Society for Neuroscience
Mesencephalic Substrate of Reward: Axonal Connections
Sandra M. Boye1 and
Pierre-Paul Rompré2
1 Center for Studies in Behavioral Neurobiology,
Concordia University, Montréal, Québec, Canada, and
2 Centre de Recherche, Hôpital du Sacré-Coeur
et Département de Psychiatrie, Université de
Montréal, Montréal, Québec, Canada
ABSTRACT
INTRODUCTION
MATERIALS AND METHODS
RESULTS
DISCUSSION
FOOTNOTES
REFERENCES
ABSTRACT
The behavioral version of the collision technique was used to study
the existence of axonal linkage between reward-relevant sites in the
ventral tegmental area (VTA) and posterior mesencephalon (PM) in six
rats trained to self-administer trains of electrical brain stimulation.
The combined use of fixed and moveable stimulation electrodes allowed
us to carry out collision tests at a total of 46 different combinations
of VTA-PM sites, and collision-like effects were observed at 24 of
these. Stimulation of the VTA and the most caudal PM sites generally
resulted in collision curves that were characterized by a single
increase in paired-pulse effectiveness (E-values), whereas recovery in
those collision curves obtained from stimulation of the VTA and more
rostral PM sites was generally slower, and often characterized by a
double rise. Despite little variability in interelectrode distances
(1.0-3.8 mm), collision intervals varied widely, ranging from 1.5 to
7.3 msec. Recovery from refractoriness (initial 25%) was also
estimated and ranged from 0.7 to 1.0 msec, resulting in conduction-time
estimates of 0.7-6.3 msec. The lack of correspondence between
interelectrode distances and conduction times suggests the presence of
axonal branching. Results of this study constitute the first behavioral
evidence of a reward-relevant axonal link between the VTA and the PM.
In addition, the finding that in one animal the anterior electrode was
located within the posterior portion of the lateral hypothalamus (LH)
suggests that the reward-relevant axonal bundle linking the LH and VTA
may extend as far back as the caudal regions of the PM.
Key words:
collision;
refractory periods;
reward;
self-stimulation;
ventral tegmental area;
posterior mesencephalon
INTRODUCTION
A major challenge in the study of the neural
substrates of behaviors induced by electrical brain stimulation is to
determine which neurons located within the stimulation field control
the behavior. One approach that has been used to characterize
reward-relevant neurons, for instance, uses responding for electrical
brain stimulation [self-stimulation (SS)] and consists of determining
trade-off functions that describe different combinations of two
stimulation parameters that support a constant level of responding.
This psychophysical approach rests on the assumption that these
trade-off functions reflect anatomical and physiological
characteristics of neurons that contribute directly to the evoked
behavior (Gallistel et al., 1981
).
Previous mapping studies that used the psychophysical approach have
revealed the presence of a continuous band of reward-relevant sites
extending between the ventral tegmental area (VTA) and central gray
(Rompré and Miliaressis, 1985
; Rompré and Boye, 1989
). Such
continuity suggests the presence of a reward-relevant pathway traveling
between these sites. This hypothesis is supported by
psychophysical data, which show that directly stimulated
reward-relevant neurons in the medial mesencephalon have refractory
periods that are comparable to those of reward-relevant neurons in the
VTA (Rompré and Miliaressis, 1987
).
One way to test the hypothesis of a common pathway is to apply the
behavioral version of the collision technique, which has been used
previously to reveal reward-relevant axonal linkage between the lateral
hypothalamus (LH) and the VTA (Shizgal et al., 1980
; Bielajew and
Shizgal, 1982
, 1986
; Durivage and Miliaressis, 1987
; Gratton and Wise,
1988
; Murray and Shizgal, 1994
). This technique takes advantage of the
conduction failure that occurs because of the collision of ortho- and
antidromic action potentials propagating along a common axon. The
behavioral version of the collision technique consists of stimulating
with pulse pairs: each site receives one pulse from each pair, and the
number of pulse pairs required to maintain a constant level of
responding is determined at different interpulse intervals. An increase
in the required number of pulse pairs at short interpulse intervals
suggests that (1) behaviorally relevant action potentials are lost
because of collision and (2) the two sites are linked directly by
reward-relevant neurons.
The collision technique has been used previously in an attempt to
reveal a reward-relevant axonal link between the LH and the posterior
mesencephalon (PM) (Bielajew et al., 1981
; Kofman and Yeomans, 1988
).
Although these earlier studies did not provide evidence of
collision-like effects, the observed summation between reward-relevant
signals triggered at each site suggested that PM and LH rewarding
effects are mediated by neural elements that converge on a common
substrate. In the present study, we attempted to reveal axonal linkage
between sites in the VTA and the PM. Contrary to previous studies,
however, we used moveable stimulation electrodes to circumvent the
problem created by the large dispersion of reward-relevant sites in the
PM (see Miliaressis and Philippe, 1983
).
MATERIALS AND METHODS
Subjects and surgery. Subjects were male Long-Evans
rats (Charles River breeding farms)that weighed between 350 and 450 gm
at the time of surgery. They were housed individually in plastic cages
with free access to food and water and were maintained on a reversed 12 hr light/dark cycle (lights on at 8 P.M.).
Surgery was conducted under general anesthesia induced by sodium
pentobarbital (65 mg/kg, i.p.). Atropine sulfate was administered 20 min before anesthesia to reduce mucous secretion. Each animal was
implanted with a moveable electrode (Kinetrods, SME-01) and either one
or two fixed monopolar stimulation electrodes. Fixed electrodes were
constructed from stainless steel wires (0.25 mm), insulated with
Formvar, and crimped to a male amphenol pin; the tip of each electrode
was honed to a hemispherical shape. Fixed electrodes were aimed at the
VTA using the following flat skull stereotaxic coordinates: 4.8-5.3 mm
posterior to bregma, 0.8-1.8 mm lateral to the midline, and 7.3-8.2
mm below dura. The moveable electrode was aimed at the midline PM,
7.3-8.0 mm posterior to bregma and 5.5-7.0 mm below the skull
surface. An uninsulated stainless steel wire, crimped at one end to a
male amphenol pin, was wrapped around four to five skull screws and
served as the inactive electrode. Acrylic dental cement was used to
chronically secure the electrode assembly to the skull.
Apparatus. Operant chambers (25 × 25 × 70 cm) were
equipped with a rodent lever located 6 cm above the wire mesh floor.
Depression of the lever allowed the animal to trigger the delivery of
trains of electrical pulses. Stimulation pulses were produced by a dual
constant-current unit driven by a two-channel pulse generator (Mundl,
1980
). Current intensity was monitored by reading the voltage drop
across a 1K
resistor in series with the rat. A light located above
the lever served as a discriminative cue and signaled the availability
of the stimulation.
Training and stabilization. One week after surgery, animals
were screened for VTA SS. Stimulation parameters consisted of 500 msec
trains of cathodal rectangular pulses of constant duration (0.1 msec).
Once responding was established, animals were allowed to self-stimulate
for 1 hr daily for 3 consecutive days with current intensity and pulse
number adjusted to support continuous responding. Only animals that
learned to self-administer stimulation via the VTA electrode were
included in the study. For animals with bilateral VTA electrodes, both
sites were screened and the one that sustained SS at the lowest current
intensity or did not induce stimulation-bound reactions was used in the
collision tests.
Subjects were subsequently trained to lever-press for stimulation of
the PM. If the subject did not learn the task within a single session,
the electrode was lowered (0.32 mm), and the new site was tested
the following day. Once a PM site that supported SS was found, subjects
were allowed to self-stimulate for 1 hr daily for 3 consecutive
days.
During the stabilization period, functions relating response rates to
the number of pulses within a train of stimulation (rate-number curve)
were obtained repeatedly. Each curve consisted of first determining the
number of pulses required to produce maximal responding during a 30 sec
trial and then decreasing this number by ~10% (0.05 log10 unit steps) to the closest pulse number
until responding extinguished. Number thresholds, defined as the number
of pulses required to support a half-maximal rate of responding, were
extrapolated from individual rate-number curves. Self-stimulation was
considered stable when number thresholds did not vary by more than
~40% (0.15 log10 units) within and across
three to four test sessions.
Collision test. Collision tests consisted of determining the
number thresholds for single- and paired-pulse stimulation conditions.
Each test session began with a warm-up single-pulse number threshold
determination for each site; these data were not included in the
analyses. Throughout the session, three additional single-pulse number
thresholds were obtained from each site; these were interspersed among
paired-pulse number threshold determinations. In the paired-pulse
condition, stimulation consisted of delivering the first pulse of each
pair (conditioning- or C-pulse) to one site and the second pulse (test-
or T-pulse) to the other, at different C-T intervals. The stimulation
site that received the first pulse from each pair alternated from day
to day [anterior-posterior (AP): C-VTA, T-PM; posterior-anterior (PA):
C-PM, T-VTA]. The order in which different C-T intervals (0.2-32
msec) were tested was first determined randomly and then
counterbalanced daily. At some sites, train duration was increased (up
to 750 msec) to test very long C-T intervals. The data from a session
were discarded if for either site the range of single-pulse number
thresholds exceeded 0.15 log10 units.
The effectiveness of paired-pulse stimulation (E-value) at each C-T
interval was estimated using the following equation:
where E = effectiveness of paired-pulse stimulation,
NTspl = lower of the two single-pulse
number thresholds, NTc-t = paired-pulse
number threshold, and NTsph = higher of the
two single-pulse number thresholds. In the equation above, an E-value
of 1 results when the paired-pulse number threshold is half the
single-pulse number threshold, and suggests that C and T pulses
contribute equally to the behavior. Conversely, an E-value of zero
results when the paired-pulse number threshold is the same as the
single-pulse number threshold, and suggests that T pulses do not
contribute to the behavior.
At each site, the AP condition was always tested first. If after two to
four replications the curve relating E-values to C-T interval
(collision curve) did not show a clear differentiation in E-values
between short and long C-T intervals, the electrode was lowered (0.16 or 0.32 mm), and the new site was tested the following day. In cases
where a differentiation in E-values was evident, additional AP-PA
collision curves were obtained until four to six replications of each
were completed. Two collision curves were obtained daily,
counterbalancing whenever possible between AP and PA conditions. When
sufficient replications had been obtained, the electrode was lowered to
the next site. At each new PM site, the current intensity was adjusted
to obtain a number threshold of ~13 pulses; once this was achieved,
the current intensity was kept constant for all subsequent collision
tests carried out at that site. Occasionally, current intensities used
for stimulation of the VTA were also readjusted before the start of the
collision tests at a new site.
Data analysis. Data were analyzed with a two-way ANOVA for
repeated measures. Missing data were estimated using Yates' formula
(Kirk, 1968
), and degrees of freedom were adjusted accordingly.
Refractory period test. In some cases, at the end of the
collision tests refractory periods were estimated from at least one of
the two stimulation sites. As with the collision tests, estimation of
refractory periods consisted of number threshold determinations for
single- and paired-pulse conditions, but with both pulses delivered via
the same electrode. To reduce the contribution of local potential
summation and to obtain a better estimate of the earliest recovery from
refractoriness (initial 25%), we used C-pulses that were 1.2-1.4
times greater in amplitude than T-pulses (Yeomans, 1979
; Bielajew et
al., 1982
; Rompré and Miliaressis, 1987
). Relative T-pulse
effectiveness was calculated with the formula used for the collision
test.
Each test session began with one warm-up single-pulse number threshold
determination for each of the two pulse intensities. During the
remainder of the test, three additional single-pulse number threshold
determinations were obtained at each current intensity; these were
interspersed among paired-pulse threshold determinations. Interpulse
intervals ranged from 0.2 to 17.0 msec, and the order in which they
were tested was first determined randomly and then counterbalanced from
day to day. The refractory period test was replicated four times. The
data from a session were discarded if the range of single-pulse number
thresholds for either current intensity exceeded 0.15 log10 units.
Histology. At the end of the study, animals were
anesthetized with sodium pentobarbital, and the tissue surrounding each
electrode tip was marked by passing a direct anodal current of 100 µA
for 15 sec. Animals were then perfused intracardially with saline
(0.9%), followed by a formalin solution containing potassium
ferrocyanide (3%), potassium ferricyanide (3%), and trichloroacetic
acid (0.5%). The bone surrounding the bottom half of the brain was
then removed, and the brain was lowered from the skull; this procedure
minimized the degree of damage to tissue surrounding the electrode and
allowed direct measurement of the distance between electrode tips.
Brains were then kept in 10% formalin. Before sectioning, brains were
immersed for consecutive 24 hr periods in each of three
sucrose-formalin solutions (10%, 20%, and 30%). Brains were then
sliced in 40 µm sections and subsequently stained with a
formalin-thionin solution. Reconstruction of the dorsoventral locations
of sites tested with the moveable electrode was made by first locating
the lesion and then inferring the position of each site using a record
of the distances by which the electrode had been lowered.
RESULTS
Location of SS sites
The location of each tested site is shown in Figures
1-6, along with the results of the respective collision
tests. In five subjects, the tip of the anterior electrode was located
within the VTA (4.8-5.3 mm posterior to bregma), and in subject F18,
the tip of the anterior electrode was located in the posterior part of
the LH (4.52 mm posterior to bregma). In four subjects, the PM
electrode was located on the midline, and in two others it penetrated
the brain at a mediolateral angle. A total of 61 PM sites were tested,
and of these, 49 supported SS. Collision tests were carried out at 46 VTA-PM site combinations.
Fig. 1.
Collision data from subject F17. Each graph shows
changes in E-values as a function of C-T interval and represents data
obtained from a single site. Graphs show AP curves (open squares,
dashed lines), PA curves (filled squares, solid lines),
or their average (filled triangles, solid lines). The
asterisk or cross next to the site number
indicates symmetry or asymmetry between AP and PA curves, respectively.
Data points represent the mean ± SEM. The two numbers in the
upper left corner of each graph indicate the current intensities
(in µA) used for the anterior and posterior electrodes, respectively.
The VTA (left) and PM (right) electrode tip
locations were reconstructed onto tracings of the Paxinos and Watson
(1986)
atlas of the rat brain. Numbers above each tracing
indicate distance (mm) from bregma. Filled squares indicate
sites that did not support SS, and filled circles show the
locations of sites that did support SS. scp, Superior
cerebellar peduncle; ml, medial lemniscus; MP,
medial posterior mammillary nucleus; CG, central gray;
DR, dorsal raphe; VTg, ventral tegmental
nucleus.
[View Larger Version of this Image (34K GIF file)]
Collision tests
In cases where AP-PA collision curves were not significantly
different (symmetrical curves, p > 0.01), only the averaged
curves (filled triangles) are shown. At sites where AP-PA
curves were statistically different (asymmetrical curves, p < 0.01), both AP (open squares) and PA (filled
squares) curves are shown. The presence of a collision-like effect
was inferred from a significant effect of C-T interval
(p < 0.01). Sites at which symmetrical or
asymmetrical collision-like effects were observed are indicated by an
asterisk or a cross, respectively, next to the
site number. All other graphs show only AP curves, or AP-PA curves
that were replicated an unequal number of times.
Figure 1 shows data obtained from subject F17. Symmetrical
collision-like effects were observed at sites 1-5 and 7. At these
sites, most of the recovery from collision block occurred between 2 and
8 msec, and the magnitude of the collision-like effects, estimated from
the percentage difference between low and high E-values, ranged from
22% (site 2) to 38% (site 5). Collision curves obtained from site 6 were asymmetrical and thus were not averaged. Most of the recovery
at site 6 occurred from 4 to 16 msec.
Figure 2 shows collision curves obtained from subject
F8. A symmetrical collision-like effect was observed only at site 13. At this site, E-values increased gradually. In addition, curves
obtained from sites 8 and 12 were also characterized by an increase in
E-values, but there was no effect of C-T interval at site 8 (p = 0.62), and an unequal number of replications at
site 12 precluded statistical analysis.
Fig. 2.
Collision data from subject F8. See Figure 1 for
details. CG, Central gray; scp, superior
cerebellar peduncle; MP, medial posterior mammillary
nucleus; VTg, ventral tegmental nucleus.
[View Larger Version of this Image (25K GIF file)]
Figure 3 shows collision curves obtained from subject
F11. Symmetrical collision-like effects were observed at sites 1, 3, and 4. Recovery from collision block at site 1 is slow (4-15 msec) and
is characterized by a double increase in E-values. Collision curves
obtained from sites 3 and 4 are characterized by a single rise over
C-T intervals of 3-6 and 2-8 msec, respectively. In this subject,
the magnitude of the collision-like effects ranged from 17% (site 3)
to 35% (site 4).
Fig. 3.
Collision data from subject F11. See Figure 1 for
details. VTA, Ventral tegmental area; DR, dorsal
raphe; xscp, decussation of the superior cerebellar
peduncle.
[View Larger Version of this Image (32K GIF file)]
Figure 4 shows collision curves obtained from
subject F9. Symmetrical collision-like effects were obtained at sites 7 and 8, and at these sites, collision curves were characterized by two
rises, with an initial increase in E-values at 6 msec at both sites and
a second increase at 17 and 24 msec, respectively. The magnitude of the
collision-like effect was 41% at site 7 and 37% at site 8. Lowering
the electrode from site 8 to site 9 resulted in asymmetrical AP-PA
collision curves. At site 9, recovery is gradual and is delayed by 3 msec in the PA curve; this asymmetry is also present at site 10.
Fig. 4.
Collision data from subject F9. Locations of the
anterior and posterior stimulation sites are illustrated in the
top and bottom panels, respectively. See Figure 1
for details. ml, Medial lemniscus; MP, medial
posterior mammillary nucleus; CG, central gray;
DR, dorsal raphe; xscp, decussation of the
superior cerebellar peduncle.
[View Larger Version of this Image (22K GIF file)]
Figure 5 shows the results of collision tests carried
out in subject F18. Symmetrical collision-like effects were observed at
sites 0-2, 4, and 7-8. Collision curves obtained from sites 0, 1, 4, and 7 revealed two rising segments. Recovery occurred predominantly
between 2 and 16 msec at sites 0-2, between 4 and 16 msec at site 4, and between 1 and 8 msec at sites 7 and 8. Although only AP curves were
obtained from sites 3, 5, and 6, it is noteworthy that E-values
increase over a similar range of C-T intervals. In this subject, the
magnitude of the collision-like effects ranged from 24% (site 4) to
42% (site 0).
Fig. 5.
Collision data from subject F18. See Figure 1 for
details. LH, Lateral hypothalamus; xscp,
decussation of the superior cerebellar peduncle.
[View Larger Version of this Image (23K GIF file)]
Figure 6 shows collision curves obtained from subject
F12. Symmetrical collision-like effects were observed at sites 3, 4, 7, and 10. Unlike the curves obtained in the five other subjects, the
shape of the collision curves in F12 differed substantially across
sites. Recovery from collision block at site 3 occurred between 5 and
21 msec and was characterized by two rises, whereas at site 4, recovery
was faster and occurred between 4 and 8.5 msec. Collision curves
obtained from sites 7 and 10 were not characterized by a sharp rise but
rather displayed a gradual increase. The largest collision-like effect
was observed at site 3 (39%), and the smallest was observed at site 4 (21%).
Fig. 6.
Collision data from subject F12. Locations of the
anterior and posterior stimulation sites are illustrated in the
top and bottom panels, respectively. See Figure 1
for details. scp, Superior cerebellar peduncle;
VTA, ventral tegmental area; MP, medial posterior
mammillary nucleus; CG, central gray.
[View Larger Version of this Image (30K GIF file)]
Refractory periods and conduction-time estimates
Twelve refractory-period estimates were obtained from a total of
10 sites at which collision-like effects were observed; estimates were
obtained from either the anterior, the posterior, or both sites. To
obtain estimates of the conduction time between the two stimulation
sites, the C-T interval at which 25% recovery from refractoriness
occurred was determined and subtracted from the C-T interval at which
25% recovery from collision block occurred. Results for each pair of
sites are presented in Table 1. As can be seen,
estimates of recovery from refractoriness varied by only 0.3 msec, from
0.7 to 1.0 msec. In contrast, estimates of recovery from collision
block varied widely and ranged from 1.5 to 7.3 msec; such variability
contributed to the wide range of conduction times (0.7-6.3 msec).
Table 1.
Estimates of conduction
times
| Subject |
Site |
Collision interval
(msec) |
Refractory period (msec) |
Conduction time (msec)
|
|
| F17 |
1 |
2.5 |
0.9 (A),
0.8 (P) |
1.6-1.7 |
|
3 |
4.4 |
0.9 (A) |
3.5 |
|
4 |
2.0 |
0.9 (P) |
1.1 |
|
5 |
2.6 |
0.9 (A) |
1.7 |
|
6 (PA) |
5.0 |
0.9 (A) |
4.1 |
|
7 |
2.7 |
0.9 (A) |
1.8 |
| F11 |
4 |
2.9 |
0.7 (A),
0.7 (P) |
2.2 |
| F9 |
7 |
7.2 |
1.0 (A) |
6.2 |
|
8 |
7.3 |
1.0 (A) |
6.3 |
|
9 (AP) |
4.9 |
0.7 (P) |
4.2 |
|
9 (PA) |
5.2 |
1.0 (A) |
4.2 |
| F18 |
0 |
4.0 |
0.7 (A) |
3.3 |
|
1 |
3.6 |
0.7 (A) |
2.9 |
|
2 |
4.0 |
0.7 (A) |
3.3 |
|
4 |
6.2 |
0.8 (A) |
5.4 |
|
7 |
1.5 |
0.8 (A) |
0.7 |
|
8 |
1.8 |
0.8 (A),
0.9 (P) |
0.9-1.0 |
| F12 |
10 |
6.9 |
0.9 (A) |
6.0 |
|
|
Conduction time estimates for sites at which collision-like
effects were observed and at which refractory periods were measured.
Conduction time estimates were obtained by subtracting the C-T
interval corresponding to 25% recovery from refractoriness from the
C-T interval corresponding to 25% recovery from collision block. For
asymmetrical collision curves, the curve used (AP or PA) in the
calculations is indicated in parentheses. For refractory periods,
letters in parentheses (A or P) refer to the stimulation site (anterior
or posterior) at which the refractory period was measured.
|
|
DISCUSSION
Symmetrical collision curves
Evidence of direct axonal linkage between two sites is inferred
from collision curves that display (1) relatively lower E-values at
short C-T intervals and (2) symmetry between AP and PA curves. The
first characteristic reflects the loss of behaviorally relevant action
potentials attributable to collision. The second characteristic is a
consequence of the bidirectional nature of axonal conduction. In the
present study, we observed symmetrical AP-PA curves at 22 different
combinations of VTA-PM sites, and of these, 50% were characterized by
a single increase in E-values (F17, sites 1-5 and 7; F11, sites 3 and
4; F18, sites 2 and 8; F12, site 4). At these sites, most of the
recovery from collision block occurred between 2 and 8 msec. The
presence of a single increase in E-values and the wide range of
recovery times suggests the contribution of a physiologically
heterogeneous population of neurons. Interestingly, the majority of
curves characterized by a single rise in E-values was obtained
generally from concurrent stimulation of the VTA and the most caudal PM
sites tested.
In another 36% of symmetrical collision curves, recovery from
collision block was characterized by two increases in E-values (F11,
site 1; F9, sites 7 and 8; F18, sites 0, 1, 4, and 7; F12, site 3). In
these, the initial recovery from collision occurred at C-T intervals
that fall within the range of recovery times of those curves
characterized by a single rise. In three animals (F9, F11, and F12),
however, the second phase of recovery clearly occurred at much longer
C-T intervals (i.e., 11-28 msec). The presence of a double rise
suggests the contribution of at least two neuronal populations with
either different conduction velocities, different refractory periods,
or multiple axonal branches. In addition, in those cases in which
recovery resumed at very long C-T intervals, the contribution of a
supernormal period may have been relevant (Yeomans, 1979
; Rompré
and Miliaressis, 1987
). In subjects F9 and F11, refractory period
curves were obtained from the VTA site only (data not shown), but
neither shows the contribution of a supernormal period. For subject
F12, however, a supernormal period was evident at a C-T interval of 8 msec in the refractory period curve obtained from the VTA, and in this
case, it might have contributed to the second phase of recovery in the
collision curve. The majority of the curves characterized by a double
rise were obtained from stimulation of the posterior LH or the VTA, and
the most anterior PM sites.
The remaining 14% of symmetrical collision curves were not
characterized by a sharp rise in E-values (F8, site 13; F12, sites 7 and 10). At these sites, E-values rise progressively and may reflect
the contribution of a heterogeneous population of axons.
Asymmetrical collision curves
Symmetry between AP-PA curves depends on the relatively constant
conduction time between the two stimulation sites and the similarity in
refractory periods of the two axonal segments. Differences in
refractory periods are expected to result in different ortho- and
antidromic conduction times and will be reflected in AP-PA curves that
recover over different C-T intervals. Likewise, the presence of one or
more synapses between the two stimulation electrodes is expected to
result in an asymmetrical delay in recovery, attributable to the
unidirectional nature of synaptic transmission. In the present study,
asymmetrical AP-PA curves were observed in only two subjects (F17,
site 6; F9, site 9). The absence of refractory period estimates from
these sites precludes assessment of the contribution of differences in
this variable to the asymmetry.
The presence of a synapse between the two stimulation electrodes will
limit the occurrence of collision to some site along the postsynaptic
neuron. Assuming recruitment of a mixed population of uninterrupted and
synaptically linked neurons, recovery from collision block will be
delayed when the C-pulse is delivered via the electrode located
upstream from the synapse. This delay results from the added time
required for transmission across the synapse (see Yeomans and
Buckenham, 1992
). Inspection of curves obtained at site 9 of subject F9
reveals that recovery in the PA condition is delayed by ~3 msec and
suggests transmission of the reward signal in a caudorostral direction.
The presence of a synapse also may be inferred from a reduction in
E-values some time after an initial recovery has occurred in those
axons directly linking the two sites. Again, the reduction in E-values
will be expected to occur only when the C-pulse is delivered via the
upstream electrode. Curves obtained from site 12 of subject F8 are
consistent with such a model and are similar to transynaptic collision
curves obtained in a previous study (Yeomans and Buckenham, 1992
). The
initial recovery in both curves at short C-T intervals and the
subsequent reduction in E-values in the AP condition (12-32 msec)
suggest that in addition to axons directly linking the two sites, the
stimulation also may have recruited descending neurons that terminated
in between.
Topography of the substrate
The present results reveal several important characteristics about
the anatomical distribution of those reward-relevant axons responsible
for the collision-like effects. First, these findings show that at
least part of the substrate travels between the VTA and midline regions
of the PM. The data obtained from subject F18 further suggest that the
extent of this pathway may be greater and may extend to the LH. Indeed,
the overlap in the range of collision intervals observed here and in a
previous study (Murray and Shizgal, 1994
) suggests the existence of a
common axonal bundle traveling between anterior forebrain sites and the
PM.
Second, the magnitude of the collision-like effects was generally
small, ranging from 20 to 40%. This suggests that a significant
proportion of axons stimulated by the anterior electrode did not pass
through the stimulation field of the posterior electrode or vice versa.
Accordingly, E-values at short C-T intervals were always >0. If the
axons responsible for the collision-like effects are localized near the
midline in the PM but distributed between both hemispheres in rostral
mesencephalic regions, a subgroup of reward-relevant neurons stimulated
by the medially implanted PM electrode will not be stimulated by the
unilateral VTA electrode. The simplest model would predict a maximal
collision-like effect of 50%, an estimate close to that obtained in
the present study. In accordance with this model, collision-like
effects were obtained between the PM and both left (F17, F9) and right
(F8, F11, F12) VTA sites.
Third, the total percentage collision across all tested sites in
three subjects (F17, F18, and F12) exceeds 100%, suggesting that some
reward-relevant axons contributed to collision-like effects at more
than one site. Indeed, the small distances by which the posterior
electrode was lowered would in fact predict overlapping of the
stimulation fields. In addition, the distance over which collision-like
effects were observed suggests that reward-relevant axons are widely
dispersed in PM regions and provides a possible explanation for the
failure of previous studies to reveal an axonal link using fixed
stimulation electrodes (Bielajew et al., 1981
; Kofman and Yeomans,
1988
). For example, comparison of the results obtained from F17 and F8
reveals that although these subjects had anterior and posterior
electrodes located within the same coronal planes, their respective
profiles differ. In effect, a greater number of collision-like effects
were obtained when the posterior electrode was located just off the
midline (compare F17 and F8). In addition, the high stimulation
intensities used in subject F17 suggest that the reward-relevant axons
responsible for the collision-like effects in F17 are located away from
the midline or that these are small-caliber axons.
Last, it is interesting to note that with the exception of subject F9,
stimulation intensities for the anterior electrode gradually increased
as the posterior electrode was lowered through successive sites. Such
an increase in the required intensity is consistent with a reduction in
rewarding efficacy subsequent to destruction of some reward-relevant
neurons, an observation that indirectly supports the collision-like
effects observed here.
Refractory periods and conduction time estimates
Recovery from refractoriness began after 0.4-0.7 msec and was
complete by 2-4 msec, times that are comparable to previous estimates
(Bielajew et al., 1981
; Rompré and Miliaressis, 1987
). Estimates
of conduction time between the two electrodes, based on 25% recovery
from refractoriness and collision block, ranged from 0.7 to 6.3 msec
(Table 1). The large variability in conduction times resulted mainly
from the wide range of collision intervals (1.5-7.3 msec).
Interestingly, straight-line interelectrode distances (1.0-3.8 mm)
varied little, and similar to refractory periods, fail to account for
the large variability in collision intervals. In fact, the negative
correlation (r =
0.56) between interelectrode distance and
conduction time suggests that the straight-line distance between the
two electrode tips may not describe accurately the trajectory of those
axons responsible for the present collision-like effects. One possible
explanation for this lack of correspondence is the presence of axonal
branching between the two stimulation fields. Stimulation of two
different axon collaterals, depending on the relative distance of each
electrode tip from the branch point separating the two stimulation
sites, can result in collision intervals that are greater than would be
predicted from knowledge of the refractory period and interelectrode
distance. The presence of axonal branches would also lead to an
underestimation of the axonal conduction velocity.
The present findings provide the first behavioral evidence that the PM
and VTA are directly linked by reward-relevant axons. In addition,
these findings place anatomical and physiological constraints on those
mesencephalic neurons that can be considered as possible carriers of
the reward signal. In effect, the trajectory of candidate neurons
should extend at least between the medial PM and the VTA, their
distribution should be diffuse in caudal regions and bilateral at the
level of the VTA, and they should have refractory periods as short as
0.4-0.7 msec.
FOOTNOTES
Received Nov. 7, 1995; revised Feb. 29, 1996; accepted March 4, 1996.
This work was supported by a grant from the Natural Sciences and
Engineering Research Council of Canada (NSERC, 0119057) to P.-P.
Rompré. S.M. Boye was supported by a National Sciences and
Engineering Research Council of Canada studentship, and P.-P.
Rompré is an FRSQ (Québec) chercheur-boursier. We thank Dr.
R. Anderson for helpful comments on the manuscript.
Correspondence should be addressed to P.-P. Rompré, Centre de
Recherche, Hôpital du Sacré-Coeur, 5400 Boulevard Gouin
ouest, Montréal, Québec, Canada H4J
1C5.
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