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The Journal of Neuroscience, February 15, 2003, 23(4):1206
Modulation of Spike-Mediated Synaptic Transmission by Presynaptic
Background Ca2+ in Leech Heart Interneurons
Andrei I.
Ivanov and
Ronald L.
Calabrese
Biology Department, Emory University, Atlanta, Georgia 30322
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ABSTRACT |
At the core of the rhythmically active leech heartbeat central
pattern generator are pairs of mutually inhibitory interneurons. Synaptic transmission between these interneurons consists of
spike-mediated and graded components, both of which wax and wane on a
cycle-by-cycle basis. Low-threshold Ca2+ currents
gate the graded component. Ca imaging experiments indicate that these
low-threshold currents are widespread in the neurons and that they
contribute to neuron-wide changes in internal background Ca2+ concentration (Ivanov and Calabrese, 2000 ).
During normal rhythmic activity, background Ca2+
concentration oscillates, and thus graded synaptic transmission waxes
and wanes as the neurons move from the depolarized to the inhibited
phases of their activity.
Here we show that in addition to gating graded transmitter release, the
background Ca2+ concentration changes evoked by
low-threshold Ca2+ currents modulate spike-mediated
synaptic transmission. We develop stimulation paradigms to simulate the
changes in baseline membrane potential that accompany rhythmic
bursting. Using Ca imaging and electrophysiological measurements, we
show that the strength of spike-mediated synaptic transmission follows
the changes in background Ca2+ concentration that
these baseline potential changes evoke and that it does not depend on
previous spike activity. Moreover, we show using internal EGTA and
photo-release of caged Ca2+ and caged
Ca2+ chelator that changes in internal
Ca2+ concentration modulate spike-mediated synaptic
transmission. Thus activity-dependent changes in background
Ca2+, which have been implicated in homeostatic
regulation of intrinsic membrane currents and synaptic strength, may
also regulate synaptic transmission in an immediate way to modulate
synaptic strength cycle by cycle in rhythmically active networks.
Key words:
central pattern generator; leech heart
interneurons; Ca currents; presynaptic background
Ca2+; synaptic transmission; short-term synaptic
plasticity; photo-release of caged
Ca2+/Ca2+ chelator
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Introduction |
Short-term modifications in synaptic
strength on the basis of previous activity are a hallmark of neuronal
networks that process sensory information and program motor outflow. In
rhythmically active networks that form the core of central pattern
generators, short-term synaptic modification has profound effects on
patterned output and confers multistability that can be accessed by
organizing synaptic input (Nadim et al., 1999 ).
Although it has been difficult to determine the precise mechanisms that
underlie the different forms of short-term depression at synapses
(Jiang and Abrams, 1998 ), various forms of short-term enhancement such
as post-tetanic potentiation and facilitation appear to be caused
presynaptically by the buildup of residual or background
Ca2+, which enhances vesicular release
(Zucker, 1999 ). With the removal of presynaptic residual
Ca2+, short-term enhancement subsides.
Thus, in rhythmically active networks, short-term synaptic enhancement
based on activity-dependent increases in presynaptic residual
Ca2+ provides a mechanism by which
synaptic strength can be continuously modified on a cycle-by-cycle basis.
In the rhythmically active leech heartbeat central pattern generator,
two segmental pairs of oscillator interneurons form mutual inhibitory
synapses that ensure alternating bursting and show cycle-by-cycle
waxing and waning in synaptic strength (Olsen and Calabrese, 1996 ).
Synaptic transmission between these interneurons consists of both
spike-mediated and graded components. Spike-mediated synaptic strength
depends on the membrane potential baseline from which a presynaptic
spike arises and not on previous spike activity (Nicholls and Wallace,
1978a ). The graded synaptic transmission depends on two low-threshold
Ca2+ currents: one rapidly inactivating
(ICaF) and the other slowly inactivating (ICaS) (Angstadt and
Calabrese, 1991 ). Ca imaging experiments (Ivanov and Calabrese, 2000 )
indicate that these low-threshold currents are widespread in the
neurons and that they contribute to neuron-wide changes in background
Ca2+ concentration, whereas spikes produce
no detectable widespread changes in Ca2+
concentration. During normal rhythmic activity, these widespread concentration changes wax and wane as the neurons move from the depolarized to the inhibited phases of their activity. Graded synaptic
transmission is correlated with the widespread changes in background
Ca2+ concentration brought on by these
low-threshold currents.
Here we test the hypothesis that in addition to gating graded
transmitter release, the presynaptic background
Ca2+ concentration changes evoked by
low-threshold Ca2+ currents modulate the
strength of spike-mediated synaptic transmission. We develop
stimulation paradigms to simulate the changes in baseline membrane
potential that accompany rhythmic bursting. These stimuli evoke graded
as well as spike-mediated postsynaptic responses and allowed us to
explore the influence of background Ca2+
on each. Using Ca imaging and concurrent electrophysiological measurements, we show that the amplitude of spike-mediated postsynaptic responses follows the increases in background
Ca2+ concentration that these baseline
potential changes evoke. Experiments using internal EGTA and
photo-release of caged Ca2+ and caged
Ca2+ chelator show that increases in
internal Ca2+ concentration evoke graded
and enhance spike-mediated synaptic transmission. Activity-dependent
changes in background Ca2+ concentration
have been implicated in the homeostatic regulation of intrinsic
membrane currents and potentially synaptic strength (Turrigiano, 1999 );
our results indicate that these changes in presynaptic background
Ca2+ concentration may regulate synaptic
transmission in an immediate way to modulate synaptic strength cycle by
cycle in rhythmically active networks.
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Materials and Methods |
Animals. Adult leeches (Hirudo
medicinalis) were obtained from Leeches USA and
Biopharm and maintained in artificial pond water (Leeches
USA) at ~15°C.
Preparation. Leeches were anesthetized in cold saline, after
which individual ganglia (midbody ganglion 3 or 4) were dissected and
pinned in a clear, Sylgard-coated open bath recording/imaging chamber
(RC-26, Warner Instrument Corp.) with a 150 µl working volume. The sheath on the ventral surface of the ganglion was removed
with microscalpels. Ganglia were superfused continually with normal
leech saline (Nicholls and Baylor, 1968 ) containing (in
mM): 115 NaCl, 4 KCl, 1.8 CaCl2, 10 glucose, and 10 HEPES acid buffer,
adjusted to pH 7.4 with NaOH or HCl. The preparation was mounted
ventral side up (unless noted otherwise) on the stage of an
Olympus BX50WI fluorescent microscope with an
Olympus 40×/0.80 W water immersion objective.
Heart interneurons were identified by the posterolateral position of
their somata on the ventral surface of the ganglion and by their
characteristic pattern of rhythmic bursting. Once the heart
interneurons in a ganglion were identified, one cell (presynaptic) was
iontophoretically filled with the
Ca2+-sensitive fluorescent dye Calcium
Orange, or with Calcium Orange in combination with either caged
Ca2+ (NP-EGTA) or caged
Ca2+ chelator (Diazo-2). In a small number
of preliminary experiments, presynaptic cells were filled
iontophoretically with the Ca2+-sensitive
fluorescent dye Fura-2. The opposite cell (postsynaptic) remained unfilled.
Calcium Orange [Molecular Probes, Calcium Orange,
tetrapotassium salt "cell impermeant"; excitation/emission:
549/576; molecular weight (MW) 1087.33; catalog #C-3013] is a
long-wavelength calcium indicator with a nominal
Kd of 185 nM (at
pH 7.2, 22°C) (Haugland, 2002 ). Eberhard and Erne (1991) measured a
Kd of 434 nM at
pH 7.2 and 457 at pH 7.4, a dissociation rate constant of 233 sec 1, and an association rate constant of
0.51 × 109
M 1sec 1. The fluorescence
of Calcium Orange increases linearly on its binding to
Ca2+ in the range of free
Ca2+ concentrations from 0.02 to at least
0.20 µM, with an approximately four- to
fivefold increase from 0 to 39.8 µM free
Ca2+ (Haugland, 2002 ).
Thomas et al. (2000) in experiments with HeLa cells, found that Calcium
Orange has a rather small dynamic range, compared with Fluo-3, Calcium
Green-1, and Oregon Green 488, and a prominent tendency to
compartmentalization that makes it "the least useful indicator." In
our preliminary experiments, Calcium Green-1, Oregon Green 488 BAPTA-1,
and Fluo-3 did not show any remarkable advantages over Calcium Orange.
Instead, use of Calcium Green-1 and Oregon Green 488 BAPTA-1 led to
unacceptable background fluorescence, and all three indicators
(especially Fluo-3) had a stronger tendency to photobleach than Calcium
Orange [see also Thomas et al. (2000) ].
NP-EGTA (Molecular Probes, o-nitrophenyl
EGTA, NP-EGTA, tetrapotassium salt, "cell impermeant"; MW 653.81;
catalog #N-6802) is a highly selective form of caged
Ca2+, releasing
Ca2+ during UV illumination. NP-EGTA has a
nominal Kd for
Ca2+ before UV illumination of 80 nM and after illumination of 1 mM (Ellis-Davies and Kaplan, 1994 ), with a ratio
of Kd for
Ca2+ after illumination/before
illumination of 1.2 × 104; NP-EGTA
has a nominal Kd for
Mg2+ of 9 mM, with a
ratio of Kd for
Mg2+ after illumination/before
illumination of 1 (Nerbonne, 1996 ; Haugland, 2002 ).
Diazo-2 (Derived from BAPTA, "caged BAPTA"; Molecular
Probes, Diazo-2, tetrapotassium salt, "cell impermeant"; MW
710.86; catalog #D-3034) is a photoactivatable
Ca2+ scavenger; the nominal
Kd of Diazo-2 for
Ca2+ changes during UV illumination from
2.2 µM to ~80 nM (Adams and Tsien, 1993 ;
Delaney, 2000 ). Both caged compounds used photo-release Ca2+/Ca2+
chelator during UV illumination at <360nm.
Fura-2 (Molecular Probes, Fura-2, pentapotassium salt
"cell impermeant"; MW 832.00; excitation: 340 and 380 nm, emission: 510 nm; catalog #F-1200) is a dual-wavelength calcium indicator with a
nominal Kd of 145 nM (Haugland, 2002 ). To obtain
Kd,
Rmin, Rmax,
F2free, and
F2bound, we calibrated the Fura-2
signal in vitro, using the imaging setup, described in
Intracellular Ca concentration evaluation, and a Calcium Calibration
Kit with Mg2+ #2 (Molecular
Probes; catalog #C-3722), which provides 11 prediluted buffers
with mixes of K2EGTA and CaEGTA, with
free Ca2+ concentration from 0 to 39 µM, containing 1 mM free
Mg2+. We estimated the Fura-2
Kd for
Ca2+ in the presence of 1 mM free Mg2+ to be
217 nM, which is close to the
Kd of 224 nM
provided by Grynkiewicz et al. (1985) .
To fill cells with Calcium Orange or with Fura-2, heart interneurons
were penetrated with thin-walled (1 mm outer diameter, 0.75 mm inner
diameter) borosilicate microelectrodes (A-M Systems). The
very tip of the electrode was filled with a solution of the desired
indicator (5 mM solution in 300 mM K-acetate),
and the rest of it was filled with 4 M K-acetate, 20 mM KCl (unbuffered, pH 8.4). To inject dye into the cells,
a negative current of 1 nA (50% duty cycle) for 10-20 min was used.
To fill cells with NP-EGTA or Diazo-2, the same techniques but
different microelectrode solutions were used. To fill cells with
NP-EGTA, the solution contained (in mM): 5 Calcium Orange,
40 NP-EGTA, 32 CaCl2, 40 KOH/HEPES, pH 7.2. To fill cells with Diazo-2, the solution contained (in
mM): 5 Calcium Orange, 40 Diazo-2, 40 KOH/HEPES, pH
7.2.
Electrophysiology. Recording microelectrodes filled with 4 M K-acetate, 20 mM KCl
(unbuffered, pH 8.4) of the same kind as used for dye injection were
inserted into both cells 5-15 min after the cells were filled with dye
or caged compounds or both. In some experiments, noted in
Results, the microelectrode used for recording from the presynaptic
cell contained additionally 0.2 M EGTA, the slow
Ca chelator. Microelectrodes were coated along their shanks with
Sylgard 186 (Dow-Corning) and had resistances of 20-45
M and time constants of 0.5-1.5 msec when capacity was compensated.
Once the cells were penetrated with recording microelectrodes, the
superfusate was switched to a high
Mg2+/high
Ca2+ saline that contained (in
mM): 80.5 NaCl, 4.0 KCl, 5.0 CaCl2, 20 MgCl2, 10.0 glucose, 10.0 HEPES acid buffer,
adjusted to pH 7.4 with KOH or HCl. This elevated divalent ion solution
effectively suppresses spontaneous spike activity in heart interneurons
but does not markedly affect their synaptic transmission (Nichols and
Wallace, 1978a ).
In all experiments, the activity of the presynaptic cell was recorded
in current-clamp mode, whereas the activity of the postsynaptic cell
was recorded either in current-clamp mode or in voltage-clamp mode.
Voltage-clamp recordings were made with an Axoclamp-2A amplifier (Axon Instruments, Foster City, CA) in single-electrode
voltage-clamp mode with a sampling rate of 2.5 or 5 kHz. Current-clamp
recordings were made with an Axoclamp-2A amplifier used in
discontinuous current-clamp mode with a sampling rate of 2.5 or 5 kHz.
In each case, the electrode potential was monitored on an oscilloscope to ensure that the potential settled between current injection cycles.
All recordings were referenced to a chlorided silver wire used
to ground the bath. All electrophysiological data were acquired, digitized, and stored on a Pentium or Pentium II (Intel) computer using
pCLAMP 7.0/8.0 software with a Digidata 1200 or 1320A interface from
Axon Instruments.
All stimulus protocols were generated using the pCLAMP program CLAMPEX.
During normal rhythmic activity (period of ~6-10 sec), oscillator
heart interneurons move from a potential of approximately 55 mV
during their inhibited phase to a burst phase during which the spikes
appear to arise from a potential of approximately 45 mV (Hill et al.,
2001 ). The elevated divalent cation concentration of the bathing
solution used in these experiments (5 mM
Ca2+, 20 mM
Mg2+) raised the threshold for spiking in
the interneurons to above 40 mV and suppressed rhythmic activity. To
simulate normal excursions in membrane potential, we developed a
depolarizing step protocol. The usual protocol mimicked the depolarized
burst phase of the presynaptic cell by a 2 sec current step to a
potential of approximately 40 mV, from and back to a holding
potential of 50 to 65 mV. During this current step, either a train
of brief (6 msec) suprathreshold current pulses was superimposed or
individual suprathreshold current pulses were superimposed at various
times (usually at 36, 422, 808, 1194, 1580, and 1966 msec from the
beginning of the depolarizing step). The trains of current pulses were
generated by an S48K Square pulse stimulator (Astro-Med,
Grass Instrument Division) that was triggered by CLAMPEX and in turn
gated the constant current source of the Axoclamp-2. In some
experiments, suprathreshold pulses were applied before and after the
depolarizing step. In some cases, the brief suprathreshold pulses were
applied without the long subthreshold depolarizing current. The
postsynaptic cell was typically held at approximately 40 mV in
voltage clamp or by current injection in current clamp.
Ca imaging. Changes in Calcium Orange fluorescence were
monitored continuously and recorded with an ICCD-350f CCD camera
(Video Scope International) connected to the fluorescent
microscope mentioned above, equipped with an Olympus U-MNG
(exciter filter BP 530-550 nm, dichroic mirror DM 570 nm, barrier
filter BA 590 nm) filter set, 10% neutral density filter, and
Olympus 40×/0.80 W water immersion objective and
Axon Imaging Workbench 2.1/2.2/4.0 software with a
Digidata 2000 interface (Axon Instruments) on a Pentium II
(Intel) computer. Intensifier gain and black (baseline) levels were
adjusted to achieve minimal background fluorescence, convenient visualization of the filled neuron, and sufficient dynamic range for
monitoring fluorescence changes.
Our setup permits the acquisition of full-frame images of 640 × 480 pixels at a resolution of 0.379 µm2
for 1 pixel (395 × 295 µm for full frame) with the
Olympus 40×/0.80 W water immersion objective. Changes of
fluorescence were recorded from one or more zones, which are numbered
in Figure 1B. Zones 1-3 were 20-60 pixels (7.58-22.74
µm2) and corresponded to single neuritic
branches, and zone 4 was 600-1200 pixels (235-470
µm2) and corresponded to the approximate
synaptic contact region of a heart interneuron. Only those parts of
interneurons in which the fluorescence measurement remained unsaturated
during the entire experimental protocol were used to monitor changes of
fluorescence. In all experiments, the maximal available acquisition
rate (video rate, 30 Hz) was used, yielding a time resolution of 33 msec. Video signals were accumulated for 33 msec per image, without any
kind of gating, using the DC mode of the camera.

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Figure 1.
A, Schematic of experimental setup.
Lines with arrowheads indicate control
communication lines and their direction. Dotted and
dashed lines indicate light paths and beams, and
lines ending in electrode symbols are
electrical connections. B, Simultaneous recordings
(ii) of electrophysiological activity and Ca
fluorescence changes ( F/F) in
fine branches. The preparation was mounted dorsal side up to image fine
branches (i). A step depolarization (stimulus
protocol used in several of the experiments reported) of the imaged
cell led to a widespread change in Ca fluorescence recorded at the
numbered circles/oval. Note that the
fluorescence signal recorded in the oval
(4), which covers a large portion of the synaptic
contact region, is very similar to that recorded in a much more
restricted portion of the synaptic contact region
(3) but is less noisy. The fluorescence signal
recorded near the main neurite (1) rises and
falls more slowly than in the synaptic contact region
(3, 4). In this and all subsequent
images, the location and relative size of the fluorescence recording
sites are indicated, but they are exaggerated in size for legibility,
and in all images presented the intensity of fluorescence is coded by a
linear gray/pseudocolor scale inset
(0-255). In this and subsequent figures, membrane
potential recordings (Vm) of heart
interneurons are labeled HN and indexed by body side and
ganglion number of the recorded cell. Vm
records labeled Pre were from cells that were stimulated
and thus functionally presynaptic. In each case, their Ca fluorescence
signals were recorded synchronized with the voltage recordings. The
current monitor trace for the Pre cell is labeled
CM. In all the experiments illustrated in subsequent
figures, postsynaptic responses to the Pre cell
stimulation were recorded in the opposite (Post) heart interneuron in
voltage clamp (IPSC) or current clamp (IPSP).
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To synchronize the acquisition of electrophysiological data and Ca
fluorescence recording, the Digidata 2000 and Digidata 1200/1320A were
connected using a DIO-3 cable interface (Axon Instruments)
that permits one program to trigger the other. In our experiments, we
used pCLAMP 7.0/8.0 protocols to trigger data acquisition by
Axon Imaging Workbench, which in turn controlled the
shutter for the imaging lamp.
Stored data were analyzed on the same computer using pCLAMP program
CLAMPFIT, Microcal Origin 6.1 and StatSoft
Statistica software. Illustrations were created using Adobe Photoshop
6.0 and Adobe Illustrator 10.0 software. Calcium fluorescence data are
presented mainly as changes in fluorescence
( F/F), but in some cases as
fluorescence (F); in this latter case (see Fig. 2),
the data are presented in units of absolute fluorescence on a scale
from 0 to 255 fluorescence units. Results of statistical analysis are
presented/plotted as mean ± SE.
Intracellular Ca concentration evaluation. Fluorescence of
Fura-2 was recorded using basically the same setup as above but equipped with filter set XF04 (Omega Optical),
which included exciter filters 340HT15 (center wavelength 340 nm) and
380HT15 (center wavelength 380 nm), dichroic mirror 430DCLP02 (cutoff wavelength 430 nm), emitter filter 510WB40 (center wavelength 510 nm),
and a 25% neutral density filter. All other details of the setup were
the same.
In these experiments only one cell was recorded. Cells were held at
different holding potentials for not less than 60 sec, after which the
emission at 510 nm for excitation at 340 nm and at 380 nm each was
recorded for 10 sec. The signal was acquired from zone 4 (see above).
For background subtraction the nearest region with little change in
fluorescence was used. The concentration of free intracellular
Ca2+ was calculated as
[Ca2+]i = Kd × (F2free/F2bound) × (R Rmin)/(Rmax R) (Grynkiewicz et al., 1985 ), using parameters obtained
during the in vitro calibration.
UV photolysis of caged
Ca2+/Ca2+
chelator. For experiments of this kind, the optical system
was modified (Fig. 1A). A 100 W mercury lamp (release
lamp), equipped with a UV transmitting fused-silica condenser, an
electronic shutter (Oriel Instruments), and a glass UV
filter (U-360, Edmunds Industrial Optics), was connected
by a UV transmitting fused-silica fiber (core diameter 1000 µm,
numerical aperture 0.22; Oriel Instruments) to an
"ablation laser unit" (Photonic Instruments) that was
attached to the microscope. To make the connection, the resonator block
of the ablation laser unit was removed, and the fiber, equipped with a
UV-transmitting fused-silica focusing beam probe (Oriel
Instruments), was connected to the port of the resonator block.
A second 100 W mercury lamp (imaging lamp), used for fluorescent
imaging, was attached to a lamp-house block of the ablation laser unit.
The UV-transmitting 50/50 beam splitter permitted us to deliver the
light of both mercury lamps through the optical system of the
microscope to the preparation, making it possible to monitor and record
Ca fluorescence and to photo-release caged compounds simultaneously. In
some of these experiments, we used the filter set described above. In others we used exciter filter XF1074 (525AF45, center wavelength 525 nm), dichroic mirror XF2032 (565DRLPXR, cutoff wavelength 565 nm), and
emitter filter XF3083 (595AF60, center wavelength 595 nm) from
Omega Optical. In each case, the exciter was installed not
in the microscope's standard filter cube, but between the imaging lamp
and the lamp-house block of the ablation laser unit. The location and
focusing of the spot of "uncaging" light were adjusted with
controls on the ablation laser unit so that the spot was centered in
the image plane. To estimate the area of effective uncaging of our
light spot, a water-glycerol solution of 4,5-dimethoxy-2-nitrobenzyl
(DMNB)-caged fluorescein (~100 µM)
(Molecular Probes, DMNB-caged fluorescein dextran anionic; MW 3000; catalog #D-3309) was placed on a slide under a coverslip, and
the ability of the system to uncage the fluorescein was tested (Wang
and Augustine, 1995 ; Parpura and Haydon, 1999 ). The intensity (neutral
density filter) and diameter (iris diaphragm) of the spot were then
adjusted so that fluorescein was uncaged in an area of 7400 pixels
(2800 µm2) (see Figs. 8, 11), as
measured from the first image, acquired after and during fluorescein
uncaging. Lateral diffusion of uncaged fluorescein in the
water-glycerol solution was rather slow, so our method provided a
reasonable estimate of the area of uncaging. Similar values were
obtained by measuring the area and diameter of the light spot, focused
on green paper.
All protocols used for photo-release of caged compounds were generated
using the pCLAMP program CLAMPEX, which controlled the shutter of the
release lamp through the Digidata 1200/1320A connected to the shutter
control unit. Typically,
Ca2+/Ca2+
chelators were photo-released for 200-800 msec during
electrophysiological and Ca fluorescence data acquisition.
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Results |
Changes in presynaptic background Ca2+ can
account for the modulation of spike-mediated synaptic transmission
between heart interneurons by membrane potential
During normal activity, heart interneurons burst rhythmically,
moving from an inhibited phase (approximately 55 mV) to a burst phase
(approximately 40 mV at the base of the action potentials). The
average burst period is ~6-10 sec, and average spike frequency during a burst is ~12 Hz (Hill et al., 2001 ). The amplitude of spike-mediated IPSCs varies smoothly with presynaptic membrane (slow
wave) potential as activity moves between these phases (Nicholls and
Wallace, 1978a ; Olsen and Calabrese, 1996 ). The general hypothesis, first put forth by Nicholls and Wallace (1978a) , that we wanted to test
was that level of background Ca2+ in the
neuron modulates the amplitude of spike-mediated synaptic transmission
and thus accounts at least in part for the effect of membrane
potential. Our previous results (Ivanov and Calabrese, 2000 ) had
indicated that Ca2+ entry through
low-threshold Ca channels determines this background level of
Ca2+ throughout the neuron. All
experiments reported here were performed in 20 mM
Mg2+/5 mM
Ca2+ saline, which blocks all spontaneous
activity in heart interneurons (see Material and Methods). This
solution has been used successfully to study the effect of membrane
potential on spike-meditated synaptic transmission (Nicholls and
Wallace, 1978a ).
Figure 2 illustrates this phenomenon
under steady-state conditions; the average amplitude of
spike-mediated IPSCs (smIPSCs) evoked by single spikes in heart
interneurons follows membrane potential over the range 50 to 35 mV
and saturates at more depolarized potentials. Background Ca
fluorescence, throughout the entire neuritic tree, increases over the
same range and shows similar saturation. IPSC amplitude and background
Ca fluorescence are well correlated (r = 0.98;
p < 0.005). At each baseline membrane potential, we
observed stochastic variation in IPSC amplitude but no tendency for
amplitude to vary systematically with spike number in our simulated
bursts. Similar results were obtained in three other preparations.
Although spike amplitude varied somewhat in these experiments, no
relationship between spike amplitude and smIPSC amplitude was apparent.
In a few cells (n = 4), we estimated the concentration
of free intracellular Ca2+ at 70 and
35 mV using the two-wavelength indicator dye Fura-2 under similar
conditions. Our results indicate a
[Ca2+]i of
61.0 ± 12.9 nM at 70 mV and 86.7 ± 10.1 nM at 35 mV.

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Figure 2.
The amplitude of spike-mediated postsynaptic
responses and the level of presynaptic background
[Ca2+]i both increase with the
presynaptic holding potential. A, Spikes were evoked at
five different holding potentials ( 50, 44, 39, 35, and 33 mV)
while we simultaneously recorded (near the main neurite) the
presynaptic level of background Ca fluorescence, presented in units of
absolute fluorescence (0-255 fu), and spike-mediated IPSCs.
B, Graph showing the relations of average spike-mediated
IPSC (smIPSC) amplitude and Ca fluorescence with
presynaptic holding potential. In this and in all subsequent figures,
data are plotted as mean ± SE. All of the recordings are from the
same preparation.
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To approximate the changes in the slow wave of presynaptic membrane
potential during a normal burst, we developed stimulation protocols in
which the membrane potential was stepped between a hyperpolarized level
( 70 to 50 mV) and a depolarized (but subthreshold because of the
increased divalent cations in the saline) level ( 45 to 35 mV) with
a current step (2-6 sec). Individual spikes were evoked by short
current pulses superimposed on this changing background potential.
Figure 3A illustrates such a
simulated burst and demonstrates that smIPSC amplitude first
dramatically increases and then decreases toward a steady state during
the 6 sec time course. The change in presynaptic Ca fluorescence
follows a similar time course. There is also prominent graded synaptic transmission, seen as a slowly changing postsynaptic current (gIPSC), which rises and declines during the simulated burst. In Figure 3B, individual spikes were evoked from a steady baseline
potential. At the beginning of the simulated burst, spikes evoked
small stochastically varying smIPSCs, but later the current pulses used
to evoke spikes elicited small Ca plateaus that were terminated when
the next pulse evoked a spike (three similar preparations were
recorded). The plateaus evoked large increases in presynaptic Ca
fluorescence, and smIPSCs were greatly enhanced. These observations
indicated that changes in presynaptic background
Ca2+ may account for the modulation of
smIPSP amplitude and its time course during slow-wave changes in
presynaptic membrane potential.

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Figure 3.
A, A simulated burst with
underlying depolarization (spikes are superimposed on a step
depolarization) produces an increase in Ca fluorescence
( F/F), graded synaptic
transmission, and modulation of spike-mediated transmission.
Spike-mediated IPSCs increase and then decrease during the simulated
burst. B, A simulated burst without underlying
depolarization (spikes superimposed on a steady holding potential) in
an unusual preparation. See Results for further explanation.
A and B show recordings from different
preparations.
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Comparison of the time course of changes in spike-mediated synaptic
transmission and background Ca fluorescence during step changes in
membrane potential
We wished to determine the time course of changes in
spike-mediated synaptic transmission during step changes in membrane potential in the absence of effects caused by the history of spike activity. Single presynaptic spikes were superimposed on long depolarizing steps (2 sec) at various times (one individual spike per
long depolarizing step) and, in addition, in some experiments before
and after the steps. Postsynaptic responses were monitored in either
current clamp (n = 16) or voltage clamp
(n = 7) as smIPSPs or smIPSCs, respectively. The
results of three such experiments are illustrated in Figure
4A-C. As
expected, the depolarizing steps evoked large increases in presynaptic
Ca fluorescence recorded near the main neurite, like site 1 in Figure
1. These changes in fluorescence rose and then began to fall slowly
during the step. The amplitude of the spike-mediated postsynaptic
responses (smIPSPs or smIPSCs) increased and decreased during the step
with a similar time course. There were no changes in Ca fluorescence associated with evoked spikes. The amplitude of the spike-mediated postsynaptic responses did not depend on the amplitude of presynaptic action potential or on the magnitude of graded postsynaptic response, which in some preparations was negligible (Fig.
4B).

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Figure 4.
Plasticity in spike-mediated synaptic transmission
evoked by a step depolarization follows the time course of changes in
Ca florescence measured near the main neurite and is independent of
previous spike activity. A-C, Single spikes were
superimposed on a step depolarization at different times. Presynaptic
recordings were superimposed, and Ca fluorescence
( F/F) signals were averaged.
Postsynaptic responses are presented as individual traces (see
insets for superimposed responses). A
illustrates experiments in which IPSPs were recorded
(n = 16), and B and C
illustrate experiments (n = 7) in which IPSCs were
recorded. In B no graded IPSC was recorded, but
spike-mediated plasticity followed a similar time course as when a
graded IPSC was recorded as in C. D,
E, Spike-mediated postsynaptic responses
(smIPSP in D and smIPSC in
E) and the change in the Ca fluorescence signal
( F/F), averaged across
experiments, are plotted versus the timing of the evoked spike from the
start of the step depolarization. In some experiments (7 for recorded
IPSPs and 5 for recorded IPSCs), a spike was evoked before the step
depolarization as in C. A single exponential time
constant was fitted to the rise of the postsynaptic responses
( IPSP/ IPSC) and the Ca
fluorescence signal ( F/F) in
D and E using
(t) = Aie t/ i + C. A and B show
recordings from the same preparation, and C shows
recordings from a different preparation.
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The amplitude of the postsynaptic responses appeared to depend only on
when a presynaptic spike was evoked during the depolarizing step, and
it followed a time course similar to evoked changes in Ca
fluorescence (Fig. 4D,E).
The time constants for a single exponential fit to the rise of the Ca
fluorescence change and the amplitude of the postsynaptic responses
were similar. Using a similar stimulus protocol, Nicholls and Wallace
(1978a) measured a time constant of ~900 msec for the rise in the
amplitude of spike-mediated IPSPs in response to a step depolarization.
There was a strong correlation (smIPSPs, r = 0.99, p < 0.005; smIPSCs, r = 0.99, p < 0.005) between the amplitude of the postsynaptic responses and the change in presynaptic Ca fluorescence.
Although in the previous experiments Ca fluorescence was recorded near
the main neurite, in subsequent experiments we additionally recorded Ca
fluorescence in fine neuritic branches and in the region of synaptic
contacts between heart interneurons as described in Materials and
Methods (Fig. 1B). Under the conditions of these experiments, Ca fluorescence changes evoked by depolarizing steps rise
and fall more rapidly in the synaptic region than in the main neurite.
Thus we were able to more precisely define the time course of changes
in background Ca2+ in the presynaptic
terminals. We also modified our stimulation protocol so that a series
of spikes were evoked during each depolarizing step to approximate more
closely natural bursts and to allow us to proceed more rapidly in our
experiments. Figure 5, A and
B, illustrates two such experiments (n > 25 each for postsynaptic current clamp and postsynaptic voltage clamp).
The time course of changes in postsynaptic responses during the step
(Fig.
6A1,A2) was
similar to the previous experiments in which only a single spike was
evoked during each step (Fig.
4D,E). There was a close correspondence between the time course of changes in presynaptic Ca
fluorescence recorded near the main neurite and spike-mediated postsynaptic responses (Fig. 6B1a,B2a)
that was similar to the previous experiments. This close correspondence
was not observed for Ca fluorescence changes in the synaptic
region (Fig. 6A1,A2). Therefore, if changes in background Ca2+
in the presynaptic terminals are causally related to the modulation of
postsynaptic responses, then binding and unbinding of
Ca2+ at an important modulatory site may
be rate limiting, or some slow process may follow this binding before
modulation occurs. For example, the modulatory
Ca2+ binding site, possibly a mobile
buffer, may have high affinity and slow kinetics, or the consequences
of Ca2+ binding at the modulatory site may
involve a slow process such as vesicle mobilization (cf. Blundon et
al., 1993 ; Winslow et al., 1994 ; Neher, 1998 ).

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Figure 5.
Plasticity in spike-mediated synaptic transmission
evoked by a step depolarization (simulated burst protocol) compared
with changes in Ca fluorescence. Ca fluorescence
( F/F) was measured at two sites
corresponding to the numbered areas in Figure
1B. Postsynaptic responses were measured as IPSPs
(A, C) or IPSCs (B,
D). E, F, Regression
analysis of the spike-mediated postsynaptic responses
(E, smIPSP; F,
smIPSC) versus Ca fluorescence
( F/F) in the synaptic contact
region (4) averaged across experiments shows
significant linear dependence only in the presence of internal EGTA.
Black lines represent the best fit from a linear
regression; gray dotted lines are 95% confidence
intervals. In A-D, all of the recordings are from
different preparations.
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Figure 6.
The time course of plasticity in spike-mediated
synaptic transmission evoked by a step depolarization (simulated burst
protocol) compared with the time course of changes in Ca fluorescence,
under control conditions and in the presence of internal EGTA. Data are
from the experiments illustrated in Figure 5. Changes in Ca florescence
( F/F) were measured in the main
neurite and synaptic contact region corresponding to sites
1 and 4 of Figure 1B.
Postsynaptic responses were measured as smIPSPs
(1) or smIPSCs (2).
A, Comparison of spike-mediated postsynaptic responses
(1, smIPSP; 2,
smIPSC) and Ca fluorescence changes
( F/F) averaged across
experiments under control conditions and in the presence of internal
EGTA. B, Spike-mediated postsynaptic responses
(smIPSP in 1 and smIPSC in
2) and the change in the Ca fluorescence signal,
averaged across experiments, are plotted versus the timing of the
evoked spike from the start of the step depolarization under control
conditions and in the presence of internal EGTA. A single exponential
time constant was fitted to the rise of the postsynaptic responses
( IPSP/ IPSC) and the Ca
fluorescence signal ( F/F) in
1 and 2 in the main neurite
(a) and the synaptic contact region
(b) using
(t) = Aie t/ i + C. Data presented here are from
A.
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The effect of the slow Ca2+ chelator EGTA on the
modulation of spike-mediated transmission by membrane potential
To test directly the dependence of synaptic modulation on
background Ca2+, we sought to reduce and
delay the buildup of changes in background Ca2+ in the presynaptic terminals by
introduction of EGTA presynaptically (n > 15 each for
postsynaptic current clamp and postsynaptic voltage clamp). The
experiments of Figure 5, A and B, served as
controls for these experiments. Diffusion of EGTA from the recording
microelectrode (200 mM) dramatically reduces both
background Ca fluorescence and changes in Ca fluorescence associated
with step depolarizations. Nevertheless, we were able to detect changes
in Ca fluorescence in response to step depolarizations, particularly in
the synaptic contact region. Figure 5, C and D,
shows the effect of EGTA on presynaptic Ca fluorescence and
postsynaptic responses using the same simulated burst protocol as in
the experiments of Figure 5, A and B. Even in the
absence of a detectable change in Ca fluorescence, the step
depolarization evoked a strong increase in spike-mediated synaptic
transmission and strong graded synaptic transmission. Intracellular
EGTA slows the buildup of spike-mediated synaptic transmission and
slightly reduces its amplitude compared with control conditions (Fig.
5, compare A, B with C,
D.). The time constants of buildup of synaptic plasticity
increased with respect to control, and the time constants of Ca
fluorescence buildup in the synaptic contact region were
correspondingly increased (Fig. 6B). Regression
analysis (Fig. 5E,F) showed
a significant linear relationship between the amplitude of the Ca
fluorescence signal in the synaptic contact region and the amplitude of
the postsynaptic response (smIPSP = 0.817 + 189.17 × F/F,
r2 = 0.96, p < 0.005; smIPSC = 0.054 + 2.523 × F/F,
r2 = 0.97, p < 0.005) in the presence of internal EGTA but not under control
conditions. We conclude that when the buildup of background Ca2+ in the presynaptic terminals is
delayed and reduced by EGTA, the background
Ca2+ concentration appears to be rate
limiting for synaptic modulation. Although spike amplitude varied
somewhat in these experiments and in other experiments using the
simulated burst protocol, no relation between spike amplitude and
smIPSC amplitude was apparent.
EGTA also had a dramatic effect on the time course but not on the
amplitude or the integral of the graded postsynaptic response (Fig.
7). In the presence of internal EGTA, the
integrated gIPSC was 95% of control. Under control conditions the time
course of the rise in graded transmission and the time course of the
buildup in Ca fluorescence in the synaptic contact region match closely (Fig. 7B, Control). This result is
expected on the basis of our previous analysis of graded synaptic
transmission (Ivanov and Calabrese, 2000 ). In the presence of internal
EGTA, this similarity in time course is preserved: both buildup in the
Ca fluorescence signal and the rise in graded transmission are delayed
(Fig. 7B, EGTA). The difference in time courses
for the rise in graded transmission and the modulation in
spike-mediated transmission under control conditions suggests that
these two processes involve different Ca-dependent mechanisms. The
buildup of background Ca2+ in the
presynaptic terminals appears to be rate limiting for graded
transmission but not for the modulation in spike-mediated transmission.

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Figure 7.
A, The time course of graded
synaptic transmission (measured as gIPSC) evoked by a step
depolarization (simulated burst protocol) compared with the time course
of changes in Ca florescence, under control conditions and with
internal EGTA. Data are averages from the experiments illustrated in
Figure 5. In this and subsequent figures, gIPSCs were obtained by
low-pass filtering of the total postsynaptic current at 1 Hz. Filtering
at 1 Hz provided realistic extractions of the data without significant
distortions in the time course or magnitude of the graded postsynaptic
responses (comparisons were made with filtering at 3, 5, and 10 Hz) and
eliminated all components of spike-mediated postsynaptic signals.
Changes in Ca fluorescence
( F/F) were measured in the main
neurite and synaptic contact region corresponding to sites
1 and 4 of Figure 1B.
F/F was smoothed over seven points by
an Origin 6.1 standard function, Adjacent Averaging, which calculates the smoothed value at
index i as the average of the data points in the interval
[i (n 1)/2, i+(n 1)/2],
inclusive. B, Superimposed time courses of average graded
postsynaptic response (gIPSC) and average Ca
fluorescence signal ( F/F) in the
synaptic contact region under control conditions and in the presence of
internal EGTA. Data are from A.
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Photo-release of caged Ca2+ (NP-EGTA) profoundly
alters the time course of depolarization-induced synaptic
plasticity
To assess more directly the role of increases in background
[Ca2+]i in graded
synaptic transmission and modulation in spike-mediated transmission, we
used photo-induced release of caged Ca2+.
In these experiments (Figs.
8-10)
and in subsequent experiments involving photo-release of caged
Ca2+ chelator (Fig.
11), our releasing light flash produced
a spot of ~60 µm in diameter, which we centered over the synaptic
contact region of the heart interneurons. Ca fluorescence signals were recorded from the main neurite and from two concentric regions, one
corresponding to the entire zone of photo-release (see Materials and
Methods) and the other to the very center of this
zone. Injection of NP-EGTA led to a strong reduction in Ca fluorescence
signals produced by step depolarizations. This reduction is consistent with the known ability of NP-EGTA to act as an effective
Ca2+ chelator with a nominal
Kd of 80 nM (to
be compared with a nominal Kd of 185 nM for Calcium Orange). In successful
photo-release experiments, light flashes of 800 msec caused noticeable
effects on synaptic transmission before the end of the flash (Figs.
8-10). For a period extending from the beginning of the flash to
~500 msec after the flash, we were unable to record a Ca fluorescence signal because of saturation of our camera; thereafter a clear Ca
signal was recorded in each case.

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Figure 8.
Photo-release of caged Ca2+
elicits graded transmission and enhances spike-mediated transmission
when spikes are evoked from a steady holding potential.
A, Ca fluorescence images of the presynaptic cell
before, during, and after photo-release of caged
Ca2+ (top insets from
left to right). The major
panel shows a combination of the before and during image at a
larger scale. The circles show zones in which Ca
fluorescence was monitored; the circle labeled
1 corresponds to the center of the releasing light beam,
the circle labeled 2 shows the zone of
photo-release as determined by the photo-release of caged fluorescein
in the absence of a ganglion preparation, and the circle
labeled 3 is in the main neurite. In all photo-release
experiments, similar monitoring and release zones were used.
B, Synaptic transmission in the absence
(1, Control) and during
photo-release of caged Ca2+ (2,
NP-EGTA) in the same preparation. C,
Plots of the time course of spike-mediated (1,
smIPSC) and graded synaptic transmission
(2, gIPSC) in the absence (blue
lines) and during photo-release of caged
Ca2+ (red lines). The green
bar shows the duration of the releasing light
flash.
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Figure 9.
Photo-release of caged Ca2+
elicits graded transmission and enhances spike-mediated transmission by
spikes superimposed on a step depolarization (simulated burst
protocol). A, Synaptic transmission in the absence
(1, Control) and during
photo-release of caged Ca2+ (2,
NP-EGTA) in the same preparation. B,
Plots of the time course of spike-mediated (1,
smIPSC) and graded synaptic transmission
(2, gIPSC) in the absence (black
lines) and during photo-release of caged
Ca2+ (gray lines). The
white bar shows the duration of the releasing light
flash. Detectable smIPSCs elicited by the brief current pulses are
indicated by asterisks (A). The
first spike elicited by a current pulse during the step in
A1 and A2 did not result in a detectable
smIPSC; thus a zero value appears in the plots of B1
where all responses to spikes elicited by pulses during the current
step are plotted. The step depolarization itself elicited a spike in
the control experiment (A1), but it elicited no
detectable smIPSC response and was not plotted
(B1).
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Figure 10.
Photo-release of caged Ca2+
elicits graded transmission and enhances spike-mediated transmission by
spikes superimposed on a step depolarization (simulated burst
protocol). A, Synaptic transmission in the absence
(1, Control) and during
photo-release of caged Ca2+ (2, 3,
NP-EGTA) in the same preparation. B,
Plots of the time course of spike-mediated (smIPSC,
gray lines) and graded synaptic transmission
(gIPSC, black lines) in the
absence (1, Control) and during
two subsequent photo-releases of caged Ca2+
(2, 3, NP-EGTA). The white
bars show the duration of the releasing light flash. Only the
smIPSCs elicited by the brief current pulses during the depolarizing
step are plotted. Plots correspond to panels 1-3 in
A.
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Figure 11.
Photo-release of caged Ca2+
chelator suppresses graded transmission and alters the time course of
plasticity in spike-mediated transmission by spikes superimposed on a
step depolarization (simulated burst protocol). A,
Synaptic transmission in the absence (1, 4,
Control Pre-release and Control
Post-release, respectively) and during two subsequent
photo-releases of caged Ca2+ chelator (2,
3, Diazo-2) in the same preparation.
B, Ca fluorescence images of the presynaptic cell
before, during, and after photo-release of caged
Ca2+ (left insets from
top to bottom corresponding to the
photo-release shown in A2). The major
panel shows a combination of the before and during image at a
larger scale. The circles show zones in which Ca
fluorescence was monitored; the circle labeled
1 corresponds to the center of the releasing light beam,
the circle labeled 2 shows the zone of
photo-release as determined by the photo-release of caged fluorescein
in the absence of a ganglion preparation, and the circle
labeled 3 is in the main neurite.
C, Plots of the time course of spike-mediated
(smIPSP, blue and red
lines for control and photo-release experiments, respectively)
and graded synaptic transmission (gIPSP,
black lines) in the absence (1,
Control Pre-release; 4, Control
Post-release) and during two subsequent photo-releases of caged
Ca2+ chelator (2, 3,
Diazo-2). The green bars show the
duration of the releasing light flash. Only the smIPSCs elicited by the
brief current pulses during the depolarizing step are connected by
lines. Plots correspond to panels 1-4 of
A.
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In our first experiments (n = 7), we elicited simulated
bursts superimposed on a flat but relatively depolarized ( 45 to 40 mV) baseline potential (Fig. 8). In the absence of a light flash, we
observed the expected stochastically varying postsynaptic responses. Photo-release of caged Ca2+ caused an
increase in both the spike-mediated postsynaptic responses and graded
transmission. These effects started before the end of the light flash
and peaked in amplitude after the light flash. These results show that
changes in background Ca2+ in the synaptic
contact region induced by photo-release of caged Ca2+ can substitute for depolarization in
mediating both graded synaptic transmission and modulation of
spike-mediated transmission.
In subsequent experiments (n = 4), we elicited
simulated bursts superimposed on a step depolarization from a
hyperpolarized level ( 70 to 60 mV). In the absence of a light
flash, we observed increases in the spike-mediated postsynaptic
responses associated with the step depolarization. Photo-release of
caged Ca2+ caused an increase in both the
spike-mediated postsynaptic responses and graded transmission. These
effects started before the end of the light flash. In the experiment of
Figure 9, the light flash was applied relatively late during the
depolarized step and both spike-mediated and graded responses peaked
near the end of the flash. In the experiment of Figure 10, the light
flash was applied both late and early during the depolarized step, and
in each case both spike-mediated and graded responses peaked during the
flash. Comparison of the time courses of spike-mediated synaptic
modulation under control conditions and during photo-release of caged
Ca2+ indicates that the released
Ca2+ profoundly alters the time course of
depolarization-induced modulation.
Photo-release of caged Ca2+ chelator Diazo-2
profoundly alters the time course of depolarization-induced synaptic
modulation
To test further the role of increases in background
Ca2+ in graded synaptic transmission and
modulation in spike-mediated transmission caused by step
depolarizations, we used photo-release of caged Ca2+ chelator Diazo-2. Injection of
Diazo-2 led to a slight reduction in Ca fluorescence signals produced
by step depolarizations. This reduction is consistent with the known
ability of Diazo-2 to act as a weak Ca2+
chelator with a nominal Kd of 2.2 µM (to be compared with a nominal Kd of 185 nM for
Calcium Orange). In successful photo-release experiments
(n = 23), light flashes of 800 msec caused noticeable effects on synaptic transmission before the end of the flash (Fig. 11).
For a period extending from the beginning of the flash to ~500 msec
after the flash, we were unable to record a Ca fluorescence signal
because of saturation of our camera; thereafter a reduced Ca signal was
recorded in each case. The released chelator has a nominal
Kd of 80 nM. In
these experiments, we elicited simulated bursts superimposed on a step
depolarization from a hyperpolarized level (approximately 70 mV)
(Fig. 11).
For 10 of 23 of these experiments (data not shown), in the absence of a
light flash, we observed greatly reduced graded synaptic transmission,
greatly reduced or eliminated spike-mediated synaptic transmission, and
greatly reduced Ca fluorescence signals associated with the step
depolarizations. The first photo-release of caged Ca2+ chelator eliminated all graded
synaptic transmission and further reduced spike-mediated synaptic
transmission. We assume that in these experiments the concentration of
Diazo-2 in the cell was sufficient to buffer all internal
Ca2+ involved in synaptic transmission and
its modulation.
For 13 of 23 of these experiments, in the absence of a light flash, we
observed the expected graded synaptic transmission, increases in the
spike-mediated postsynaptic responses, and strong Ca fluorescence
signal associated with the step depolarization. The first photo-release
of caged Ca2+ chelator caused a
precipitous decline in graded transmission, which started before the
end of the light flash. Thereafter graded transmission was greatly
suppressed (to no more than 5% of the preflash level), and Ca
fluorescence signals were also reduced for the duration of the
experiment. The effects of photo-release of caged
Ca2+ chelator on plasticity of
spike-mediated postsynaptic responses were small and transient by
comparison. During the light flashes, the time course of synaptic
plasticity was delayed. The maximal amplitude reached by the
spike-mediated postsynaptic responses during the simulated burst was
little affected, however, by the photo-release of the chelator. A
subsequent control simulated burst after two chelator photo-releases
displayed a normal time course for modulation of spike-mediated
synaptic responses, but a reduced Ca fluorescence signal and little or
no graded transmission. These results show that the released chelator
can compete better for the Ca2+ that
mediates graded synaptic release than for the
Ca2+ that mediates and modulates
spike-mediated synaptic release.
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Discussion |
During their normal rhythmic activity, oscillator heart
interneurons show cycle-by-cycle waxing and waning in the synaptic strength of their mutually inhibitory synapses (Thompson and Stent, 1976 ; Olsen and Calabrese, 1996 ). Synaptic transmission between these
interneurons consists of both spike-mediated and graded components.
Spike-mediated synaptic strength depends on the membrane potential
baseline from which a presynaptic spike arises and not on previous
spike activity; at a given baseline potential, postsynaptic responses
are nearly constant over a large spike-frequency range (0.1-50 Hz)
(Nicholls and Wallace, 1978a ). Quantal analysis has shown that this
effect of presynaptic baseline membrane potential is likely caused by
modulation of release (Nicholls and Wallace, 1978b ). The graded
synaptic transmission depends on two low-threshold Ca2+ currents: one rapidly inactivating
(ICaF) and the other slowly inactivating (ICaS) (Angstadt and
Calabrese, 1991 ). Ca imaging experiments indicate that these
low-threshold currents are widespread in the neurons and that they
contribute to neuron-wide changes in internal background
Ca2+ concentration (Ivanov and Calabrese,
2000 ). During normal rhythmic activity, background
Ca2+ concentration oscillates, and thus
graded synaptic transmission waxes and wanes as the neurons move from
the depolarized to the inhibited phases of their activity.
In this study, we sought to determine whether changes in presynaptic
background Ca2+ could account for the
modulation of spike-mediated transmitter release by membrane potential
and to define further the relationship of spike-mediated and graded
synaptic transmission. We showed that the amplitude of spike-mediated
postsynaptic responses correlates with the background concentration of
Ca2+ recorded in the presynaptic cell.
Furthermore, we showed that the modulation of spike-mediated
transmission is independent of previous spike activity. During step
changes in membrane potential, the time course of changes in
spike-mediated transmission lags behind the time course of
Ca2+ concentration changes in the synaptic
contact region. In contrast, graded transmission follows the time
course of Ca2+ concentration changes quite
well. Delaying the time course of background
Ca2+ buildup with internal EGTA delayed
the time course of both graded transmission and the modulation of
spike-mediated transmission and brought background Ca2+
buildup, graded transmission, and the modulation of spike-mediated transmission into close register. With internal EGTA, there was a
strong linear dependence of the amplitude of spike-mediated synaptic
responses on the changes in Ca2+
concentration recorded in the synaptic contact region. Photo-release of
caged Ca2+ augmented spike-mediated
responses and evoked apparent graded transmission. Photo-release of
caged Ca2+ chelator transiently delayed
the buildup of spike-mediated responses associated with step
depolarizations and strongly reduced graded synaptic transmission and
Ca fluorescence signals for the duration of our experiments.
The role of residual or background Ca2+ in
short-term synaptic enhancement
Current views of the mechanism of synaptic release involve a
secretory trigger or calcium-binding sites that are closely associated with primed and docked vesicles. For spike-mediated (synchronous) synaptic transmission, the secretory trigger appears to be
synaptotagmin 1 and is associated with synaptic vesicle membranes
(Sugita et al., 2002 ). This sensor is thought to have relatively low
affinity and fast binding dynamics for
Ca2+. Other synaptotagmins may also act as
secretory triggers; e.g., synaptotagmin 7, which is associated with the
presynaptic plasma membrane, has relatively high
Ca2+ affinity and slow dynamics and
appears to subserve asynchronous release (Sudhoff, 2002 ). At the
release sites for spike-mediated transmission, high-threshold Ca
channels are thought to be closely associated with a low-affinity
secretory trigger, and Ca2+ entering
through these channels during action potentials produces restricted
Ca2+ domains that trigger release
(Augustine et al., 1992 ; Stanley, 1993 , 1997 ; Llinas et al., 1995 ;
Neher, 1998 ). Augustine (2001) has coined the term nanodomains for the
Ca2+ around a single channel that triggers
the release of a single vesicle. Various forms of short-term synaptic
enhancement have been thought to arise from residual
Ca2+, left after an action potential, that
can bind to sites on the secretory trigger and thus augment the effects
of Ca2+ entry from ensuing action
potentials (Katz and Miledi, 1968 ; Magleby, 1979 ; Magleby and Zengel,
1982 ; Zengel and Magleby, 1982 ; Zucker, 1989 ). However, more recent
studies of synaptic facilitation (Swandulla et al., 1991 ; Yamada and
Zucker, 1992 ; Delaney and Tank, 1994 ; Kamiya and Zucker, 1994 ; Regehr
et al., 1994 ; Atluri and Regehr, 1996 ; Zucker, 1999 ; Tang et al., 2000 ;
Zucker and Regehr, 2002 ) have pointed to a high-affinity facilitation
site for Ca2+ binding that may be
spatially removed from the secretory trigger so that the
Ca2+ in microdomains near the secretory
trigger has restricted access to the facilitation site. Binding of
Ca2+ at this facilitation site somehow
readies vesicles for release, thus causing facilitation. Alternatively,
the facilitation binding site may be a mobile
Ca2+ buffer that is saturated by
buildup of residual Ca2+. Saturation of
this buffer makes background Ca2+
available to the secretory trigger (Neher, 1998 ; Rozov et al., 2001 ).
Modulation of spike-mediated synaptic strength and control of
graded synaptic transmission in leech heart interneurons: the role of
background Ca2+
Our previous work has indicated that two types of low-threshold Ca
channels, one rapidly (ICaF) and one
slowly (ICaS) inactivating, are widely
distributed throughout heart interneurons; these gate graded synaptic
transmission (Angstadt and Calabrese, 1991 ; Lu et al., 1997 ; Ivanov and
Calabrese, 2000 ). The Ca2+ concentration
changes that we record with our current methods appear to depend on
Ca2+ entry through these low-threshold
channels (Ivanov and Calabrese, 2000 ). There are also less well
characterized high-threshold Ca channels of unknown location that
apparently gate spike-mediated synaptic transmission (Simon et al.,
1994 ; Lu et al., 1997 ). Ca imaging in other invertebrate neurons has
demonstrated Ca2+ entry at restricted
sites with high-threshold activation (Kloppenburg et al., 2000 ).
Our results suggest that the release sites for spike-mediated
transmission in leech heart interneurons may be conventional, with
high-threshold Ca channels closely associated with a low-affinity secretory trigger. The synaptic modulation that we observed here, however, appears to involve a high-affinity sensor that is acted on by
background Ca2+ arising from low-threshold
Ca channels that are widely dispersed throughout the neuritic processes
of the cell. In contrast, in most models of enhancement, the
Ca2+ that enhances release enters by
high-threshold channels that are thought to be restricted to release
sites and only activated by spike activity. Thus we prefer the term
background Ca2+ to describe our results
rather than residual Ca2+, which has been
defined as resulting from spike activity.
Background Ca2+ also appears to control
graded synaptic transmission in heart interneurons. More tonic forms of
release, such as from sensory cells, involve microdomains of
Ca2+ from several channels (Augustine,
2001 ), and if the affinity of the secretory trigger is higher than
previously thought, as suggested by experiments in the calyx of Held
synapses (Schneggenburger and Neher, 2000 ), then the release machinery
need not be in close association with Ca channels. Our observations on
graded release are consistent with such a view;
Ca2+ entering through low-threshold
channels in these interneurons then may increase background
Ca2+ to a sufficiently high level that
release is mediated at sites with no closely associated Ca channels
(sites specialized for graded transmission) and indeed even at sites
with associated high-threshold channels (sites specialized for
spike-mediated transmission).
Functional implications of the modulation of spike-mediated
transmission by presynaptic background Ca2+ in leech
heart interneurons
The pairs of heart interneurons studied here make strong mutually
inhibitory synaptic connections to form half-center oscillators that
under normal conditions produce continuous alternating bursting (period
6-10 sec) (Calabrese et al., 1995 ). The dependence of spike-mediated
transmission on background Ca2+ levels in
the neuron endows the heart interneurons with the ability to adjust
synaptic strength in a continuous manner during rhythmic activity. The
continuous modulation of synaptic strength appears to be important in
determining the burst structure of the oscillator heart interneurons
(Hill et al., 2001 ). Moreover, the modulation of spike-mediated
transmission by background Ca2+ provides a
mechanism to assure reciprocity between the two interneurons of a
half-center oscillator. The low-threshold Ca currents that contribute
to background Ca2+ in the heart
interneurons also are critical in determining the burst activity.
ICaS in particular controls the
strength and duration of the burst phase (Hill et al., 2001 ). Synaptic
inhibition plays an important role in determining the amount of
ICaS available during the next ensuing
burst, because the associated hyperpolarization removes inactivation
from ICaS after a burst. Thus strong
synaptic inhibition from one interneuron will produce a strong
ICaS in the subsequent burst of the
inhibited neuron. The resultant increase in background
Ca2+ will thus ensure strong
spike-mediated and graded inhibition of the opposite interneuron.
Wider implications of modulation of synaptic strength by
background Ca2+
Activity-dependent changes in background
Ca2+ concentration have been implicated in
the homeostatic regulation of intrinsic membrane currents and
potentially synaptic strength (Turrigiano, 1999 ). Our findings
presented here indicate that these changes in presynaptic background
Ca2+ concentration also regulate synaptic
transmission in an immediate way to modulate synaptic strength cycle by
cycle in rhythmically active networks. Continuous activity-dependent
modulation of synaptic strength of this kind seems particularly well
suited to rhythmically active neuronal networks because it provides an
activity-dependent mechanism on which exogenous neuromodulators can act.
 |
FOOTNOTES |
Received July 16, 2002; revised Nov. 18, 2002; accepted Nov. 21, 2002.
This work was supported by National Institutes of Health Grant NS24072.
We thank Dr. Adam L. Weaver and Anne-Elise Tobin for their critical
reading of this manuscript.
Correspondence should be addressed to Andrei I. Ivanov, Biology
Department, Emory University, 1510 Clifton Road, Atlanta, GA 30322. E-mail: aivanov{at}biology.emory.edu.
 |
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