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The Journal of Neuroscience, March 1, 2000, 20(5):1791-1799
NMDA Receptor-Mediated Subthreshold Ca2+ Signals in
Spines of Hippocampal Neurons
Yury
Kovalchuk1, 2,
Jens
Eilers1,
John
Lisman1, and
Arthur
Konnerth1, 2
1 Physiologisches Institut, Universität des
Saarlandes, 66421 Homburg, Germany, and 2 Institut
für Physiologie, Technische Universität München,
80802 München, Germany
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ABSTRACT |
We have used rapid confocal microscopy to investigate the mechanism
of Ca2+ signals in individual dendritic spines of
hippocampal CA1 pyramidal cells. The experiments focused on the signals
that occur during single weak synaptic responses that were subthreshold
for triggering postsynaptic action potentials. These
Ca2+ signals were not strongly affected by blocking
the EPSPs with the AMPA receptor antagonist CNQX. The signals
were also not strongly reduced by blocking T-type voltage-gated
Ca2+ channels (VGCCs) with Ni2+
or by blocking a broad range of VGCCs with intracellular D890. The
spine Ca2+ signals were blocked by NMDA receptor
channel (NMDAR) antagonist and had the voltage dependence
characteristic of these channels. Neither ryanodine nor cyclopiazonic
acid (CPA), substances known to deplete intracellular
Ca2+ stores, substantially reduced the amplitude of
synaptically evoked Ca2+ signals. CPA slowed the
recovery phase of Ca2+ signals in spines produced by
synaptic stimulation or by backpropagating action potentials,
suggesting a role of intracellular stores in Ca2+
reuptake. Thus, we find that Ca2+ release from
intracellular stores is not required to produce spine
Ca2+ signals. We conclude that synaptic
Ca2+ signals in spines are primarily caused by
Ca2+ entry through NMDARs. Although these channels
are largely blocked by Mg2+ at voltages near the
resting potential, they can nevertheless produce significant
Ca2+ elevation. The resulting
Ca2+ signals are an integral component of individual
evoked or spontaneous synaptic events and may be important in the
maintenance of synaptic function.
Key words:
dendritic spines; NMDA; Ca2+ channels; Ca2+ stores; subthreshold Ca2+
signals; hippocampus; ryanodine; CPA; confocal microscopy
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INTRODUCTION |
Dendritic spines are the sites of
excitatory synaptic input into many types of neurons of the mammalian
CNS (Harris and Kater, 1994 ). Recent advances in
Ca2+ imaging have made it possible to
detect Ca2+ concentration changes in
individual spines during single action potentials or synaptic responses
(Yuste and Denk, 1995 ; Eilers and Konnerth, 1997 ; Köster and
Sakmann, 1998 ). Depending on how many synaptic inputs into the cell are
activated, the EPSP may be either subthreshold or suprathreshold for
action potentials. Work on hippocampal neurons has shown that the large
depolarization that occurs during suprathreshold stimulation leads to
activation of NMDA receptor channels (NMDARs) and that the resulting
Ca2+ signals depend on this activation
(Regehr and Tank, 1990 ; Müller and Connor, 1991 ; Alford et al.,
1993 ; Malinow et al., 1994 ). These signals are important in triggering
the long-term synaptic potentiation (LTP) produced by strong afferent
stimulation (Bliss and Collingridge, 1993 ).
If fewer synapses are activated, action potentials do not occur, but
smaller Ca2+ signals in active spines can
still be detected (Denk et al., 1995 ; Eilers et al., 1995 ; Yuste and
Denk, 1995 ; Finch and Augustine, 1998 ; Köster and Sakmann, 1998 ;
Takechi et al., 1998 ; Mainen et al., 1999 ). These are termed
subthreshold signals and have been observed in a variety of cells. In
cortical pyramidal cells there have been two very different proposals
about their mechanism. According to one proposal, the dominant source
of Ca2+ is caused by voltage-gated calcium
channels (VGCCs) activated by the depolarization caused by NMDA
channels (Schiller et al., 1998 ). According to the other proposal, the
dominant source is Ca2+ entry through the
NMDA channel itself (Köster and Sakmann, 1998 ), an entry that can
occurs at resting potential, even when the large AMPA receptor-mediated
component of EPSP is blocked. Recent high-resolution imaging work on
hippocampal spines has also led to conflicting views. One group has
argued that most of the Ca2+ elevation is
attributable to Ca2+ entry through NMDARs,
but that this entry requires the EPSP to open the NMDA channels (Yuste
et al., 1999 ). Another group has argued that the
Ca2+ that enters through NMDARs is very
small and must be greatly amplified by intracellular
Ca2+ release to be detected (Emptage et
al., 1999 ). Yet another group, using imaging methods with lower spatial
resolution, has argued that the subthreshold
Ca2+ signal in dendrites is attributable
to Ca2+ entry through VGCC, but not
through the NMDA channels (Magee et al., 1995 ).
These apparent disagreements may arise in part because different groups
have used somewhat different preparations, different approaches, and
have focused on particular mechanisms. There is therefore a need for a
systematic examination of all possibilities in the same preparation. It
has previously been difficult to identify the component of
Ca2+ entry that is directly through NMDARs
because blocking these channels blocks both the
Ca2+ entry and the depolarization caused
by these channels. This depolarization may normally activate VGCC. Here
we introduce a method for blocking VGCC from the cytoplasmic side, a
method that greatly simplifies the dissection of the signals.
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MATERIALS AND METHODS |
Experiments were performed on CA1 pyramidal neurons from
300-µm-thick hippocampal slices from 10- to 21-d-old [postnatal day 10 (P10)-P21] Wistar rats (Edwards et al., 1989 ). Slices were incubated at 33°C in oxygenated standard solution (see below) for at
least 40-60 min before transferring them into the recording chamber.
The standard solution contained (in mM): 125 NaCl, 2.5 or
3.5 KCl, 2 CaCl2, 1 MgCl2,
1.25 NaH2PO4, 26 NaHCO3, 20 glucose, and 0.01 bicuculline, bubbled
with 95% O2 and 5% CO2.
In some experiments 50 µM
DL-2-amino-5-phosphopentanoic acid (DL-APV), 5 µM 6-cyano-7-nitroquinoxaline-2,3-dione (CNQX), 40-50
µM Ni2+, 20-25
µM ryanodine (Calbiochem, La Jolla, CA), or 30 µM cyclopiazonic acid (CPA) were added to the
extracellular solution. Combined electrophysiological recordings and
confocal Ca2+ imaging were performed with,
respectively, an EPC9 patch-clamp amplifier (Heka, Lambrecht, Germany)
and a confocal laser-scanning system (Noran Oz or Noran Odyssey, on
Olympus BX50WI microscope, 60× water immersion objective, numerical
aperture 0.9). The pipette solution contained (in mM): 140 KCl or K-gluconate, 10 NaCl, 4 Mg-ATP, 0.4 Na-GTP, 10 K-HEPES,
0.10-0.25 Oregon Green 488 BAPTA-1 (Oregon Green;
Kd, ~200 nM;
Molecular Probes, Eugene, OR). The pH was adjusted to 7.3 with KOH. In
some recordings, the low-affinity calcium indicator dye Magnesium Green
(0.3 mM; Kd,
~6 µM, Molecular Probes) was used. Mg-ATP was
replaced by Na2-ATP when Magnesium Green was
used. In some experiments 1-2 mM D890 (Knoll,
Ludwigshafen, Germany) was added to the pipette solution. At this
concentration, in addition to blocking completely currents through
voltage-gated Ca2+ channels (Hescheler et
al., 1982 ), D890 also partially blocks voltage-gated
Na+ and K+
channels, thus allowing a voltage control that is comparable to that
obtained when using intracellular Cs+ (O. Garaschuk and Y. Kovalchuk, unpublished observations). The pipette resistance ranged from 2.5 to 3.5 M and the series
resistance from 12 to 25 M . No series resistance compensation was
applied. Whole-cell recordings were performed at room temperature
(21-22°C, if not otherwise indicated) or at 30-32°C (see figure
legends). For synaptic stimulation of afferent fibers, voltage pulses
(5-20 V, 100 µsec duration) were delivered through a glass pipette
that was positioned extracellularly under visual control close to the dendrites under study. The stimulation strength selected was weak and
produced Ca2+ signals that were detectable
just in a small number of spines (Malinow et al., 1994 ). Active
dendritic spines were identified by imaging the fluorescence increase
in response to a burst of three stimuli given at 50 Hz. Generally, the
synaptic Ca2+ signals were evoked
repeatedly every 2-4 min, and the laser intensity was set to <2-8
µW (measured under the objective). This allowed us to obtain stable
Ca2+ recordings over a period of at least
1 hr. In addition, the viability of the dendritic segments under study
was tested throughout the experiment by monitoring AP-evoked
Ca2+ transients (evoked by short
depolarization through the somatic patch pipette). Caffeine (20 or 40 mM) was puffed locally to dendrites from
fine-tipped pipettes (Garaschuk et al., 1997 ). Unless otherwise indicated, chemicals were purchased from Sigma (St. Louis, MO). Fluorescence data are expressed as background-corrected changes in
Ca2+-dependent fluorescence divided by the
prestimulus fluorescence, F/F. Computer-based data analysis was
performed by using Image 1 (Universal Image, West Chester, PA), Igor
Pro (Wavemetrics, Lake Oswego, OR), and SigmaStat 2.0 (Jandel
Scientific, San Rafael, CA) software.
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RESULTS |
Experiments were performed on CA1 pyramidal cells in acute rat
hippocampal slices. Somatic whole-cell recordings were obtained from
visually identified cells near the top surface of the slice. A
fluorescent Ca2+ indicator dye (see
Materials and Methods) was introduced into the cytosol by diffusion
from the patch pipette (concentration range, 100-250
µM). After a period of 30 min, dendrites became highly
fluorescent, and single spines on apical dendrites could be easily
resolved by confocal imaging (Fig.
1A,B). To evoke
synaptic responses by focal stimulation, a fine-tipped stimulation
pipette was introduced into the stratum radiatum near the dendrite of choice. By adjusting the pipette position, it was possible to find a
position at which a brief current pulse evoked a
Ca2+ transient in one or more spines.
Under these conditions, the EPSP is generally caused both by
transmission at the spine in which Ca2+
transients were observed and to other synapses not in the field of
view. The size of the EPSP was in the range of 1-12 mV and was always
below the amplitude required to fire an action potential (AP). We
therefore term the Ca2+ signals
"subthreshold Ca2+ signals" to
distinguish them from the more complex
Ca2+ signals that occur when action
potentials are involved.

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Figure 1.
Subthreshold synaptic Ca2+
signals in individual dendritic spines of CA1 hippocampal pyramidal
neurons. A, Camera lucida drawing of a CA1 pyramidal
cell (P20), injected with the calcium indicator dye Oregon Green (100 µM) through the recording patch pipette. Afferent fibers
were stimulated with an extracellular stimulation electrode located in
the stratum radiatum, as shown schematically. B,
Confocal image of the boxed dendritic region shown in
A. The dashed box indicates the dendritic
region that was active during synaptic stimulation, see C-E.
C, Left, pseudocolor image of the fluorescence
change ( F/F) that occurred during the first 150 msec after a single
shock synaptic stimulation. Right, Grayscale image of
the active dendrite with indicated regions of interest that were
analyzed in D. D, waveform of the
Ca2+-dependent fluorescence change ( F/F) from a
spine (trace 1) and two dendritic regions (traces 2 and 3) during
single-shock stimulation. The associated EPSP is shown in the
inset. Same recording as in C. E,
averaged fluorescence transients (n = 6) recorded
in the spine and the parent dendrite (region 1 and 2 in
C, respectively). Both traces have been fitted with
monoexponential functions that had almost identical decay time
constants but clearly different amplitudes. The holding potential was
65 mV; recordings were made at 30°C. In this and the following
figures arrowheads mark the time points of synaptic
stimulation.
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The signals evoked by single shocks were highly localized. In the
experiment illustrated in Figure 1, the largest signals were observed
in the spine at position 1, but there was also a smaller signal in the
parent dendrite (position 2). At a distance of ~4 µm along the
dendrite (position 3), there was no detectable signal (Fig.
1C,D). With the relatively low indicator concentrations used
in this experiment (100 µM Oregon Green), the
decay time constant of the signals was ~200 msec in both the active
spine and nearby regions of the parent dendrite (Fig.
1E). In other cells, when using higher indicator
concentrations (up to 250 µM), decay times of
up to 750 msec were encountered (480 ± 260 msec; n = 18; mean ± SD). This signal is similar to
that reported by Yuste and Denk (1995) using two-photon microscopy in
the line-scanning mode. The rapid confocal imaging (60-120 frames/sec)
used here provides information not only about the spine head, but also
about nearby regions of the dendrite and reveals a dendritic signal, linked to the spine signal. The peak amplitude of the dendritic signal
was ~20-70% of that recorded in the spine. The amplitude was
largest in the immediate neighborhood of the spine and gradually decreased up and down the dendrite. In general, with single-shock stimulation, no Ca2+ signal was detected
at distances >4-5 µm from the spine.
To study the mechanism of subthreshold
Ca2+ signals, we first investigated the
role of the AMPA and NMDA receptor type of glutamate channels. It was
useful in this experiment, performed at room temperature, to use a
burst of stimulation as the standard stimulus (typically two or three
stimuli at 33 or 50 Hz; repetition time, 2 min). This reduced the
variability of the response, because we and others have found that at
room temperature, the responses to individual stimuli have a
significant fraction of failures, presumably because of failure of
vesicle release (Hessler et al., 1993 ; Allen and Stevens, 1994 ). Figure
2 shows that CNQX, an antagonist of AMPA
receptor channels, produced at resting membrane potential ( 65 mV)
only a small (~30%) reduction in the average spine signal even
though the EPSP was almost totally abolished. When the NMDAR antagonist
APV was added in addition, the average spine
Ca2+ signal was almost totally abolished.
Removal of both antagonists restored both the EPSP and the spine
signal. Figure 2C summarizes similar results from six
experiments. In a separate series of experiments, we found that
addition of APV alone greatly reduced the spine signals (by 89 ± 10%; n = 6), but a small residual signal remained.

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Figure 2.
Subthreshold Ca2+ signals in
spines require activation of NMDARs. A, Confocal image
of a dendritic segment containing an active spine
(arrow). B, EPSPs (left
traces) and associated spine Ca2+ signals
( F/F, right traces). Afferent fibers were stimulated
with a short burst consisting of three stimuli given at 50 Hz.
Bath-applied CNQX (5 µM) blocked the fast component of
the EPSPs, whereas it reduced the Ca2+ transient
only by ~30%. Additional application of APV (50 µM)
completely and reversibly blocked the EPSP as well as the associated
Ca2+ signal. Each trace is an average of three or
four consecutive recordings. Membrane potential was 65 mV.
C, Bar graph comparing the effects of CNQX
(n = 6) and APV (n = 6) on
spine Ca2+ signals (triplet stimulation, mean + SD).
F/F amplitudes were normalized to control values.
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NMDARs are controlled by Mg2+, which
produces a voltage-dependent block of these channels (Mayer et al.,
1984 ; Nowak et al., 1984 ). Consistent with this, we and others find
that in the absence of extracellular Mg2+,
the spine signals become very large and saturate the high-affinity calcium indicator dye (data not shown). Together these results clearly
indicate that the subthreshold spine Ca2+
signals require the NMDAR. The fact that CNQX produced only a small
reduction in the spine signal, even though it almost completely blocked the EPSP, indicates that depolarization is not critical for
triggering Ca2+ entry. The results are
difficult to reconcile with the view that the
Ca2+ entry is primarily through VGCC
because such signals would be greatly reduced when the EPSP amplitude
is reduced by CNQX. It is also important to note that in many cases,
spine Ca2+ signals can be recorded when
the somatically recorded EPSP is so small (1-2 mV, as in Fig. 1; see
also Zamanillo et al., 1999 ) that activation of VGCC should be minimal.
To directly test the role of voltage-gated
Ca2+ channels, we attempted to eliminate
their contribution. It has been reported that local dendritic signals
can be blocked by low concentrations of
Ni2+ (Markram and Sakmann, 1994 ; Magee et
al., 1995 ), and it was therefore of interest to test the effect of this
blocker on spine signals. Figure 3 shows
that Ni2+ produced only a small reduction
in the average synaptically evoked Ca2+
signal in the spines (note also a small reduction in the EPSP; Fig.
3B, left). A summary of 10 experiments is given in Figure 3C. These results indicate that
Ca2+ entry through
Ni2+-sensitive channels makes at most a
small contribution to spine signals. To examine the role of a wider
range of voltage-gated Ca2+ channels, we
used a patch pipette solution containing D890, a compound that blocks
voltage-gated Ca2+ channels from the
inside (Hescheler et al., 1982 ). Intracellular application is vital for
the analysis of synaptically induced signals because extracellular
application would interfere with transmitter release. Figure
4, A and B,
illustrates the ability of D890 to block depolarization-induced
Ca2+ elevation. The top traces in Figure
4B show the Ca2+ signals
in the spine and parent dendrite (Fig. 4A) induced by a 500 msec depolarizing voltage-clamp pulse to 0 mV. This signal was
detected at 5 min after the onset of whole cell recording (Fig.
4B, top). At this time sufficient dye had
diffused into the dendrites to make Ca2+
detection possible, but the dendritic concentration of D890 was insufficient to block VGCC. Ten minutes later, D890 was in sufficient concentration to block the Ca2+ transient
produced by an even longer depolarizing pulse (Fig. 4B,
bottom). During this period there was no decrease in synaptic electrical responses. In separate experiments, it was observed that
D890 reduces the inward Na+ currents
evoked by depolarizing pulses and also prevents action potentials (O. Garaschuk, F. Tempia, and A. Konnerth, unpublished observations). Thus, D890 provides a tool for eliminating VGCC and
reducing other voltage-dependent conductances without inhibiting the
synaptic response. Figure 4C-E shows that synaptically
evoked spine Ca2+ signals can be detected
in cells, in which D890 has blocked depolarization-induced Ca2+ entry. Under these conditions, the
amplitudes of spine Ca2+ signals were
within the normal range ( F/F = 86 ± 37%,
n = 11 in D890; F/F = 100 ± 46%,
n = 8 in control; mean ± SD, Fig.
4F). These experiments with D890 strongly argue
against a major role of VGCC in generating spine signals during
synaptic stimulation.

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Figure 3.
Low-threshold voltage-gated
Ca2+ channels are not required for the generation of
Ca2+ transients in spines. A,
Confocal image of a dendritic segment containing an active spine
(arrow). B, EPSPs (left
traces) and associated spine Ca2+ signals
( F/F, right traces). Afferent fibers were stimulated
with a short burst consisting of three stimuli given at 50 Hz.
Application of nickel (40 µM), a blocker of T-type
voltage-gated Ca2+ channels, reversibly reduced the
spine Ca2+ signal only by ~30%. Note that
Ni2+ also slightly reduced the EPSP amplitude. The
traces represent averages of three to five individual recordings.
Membrane potential was 69 mV. C, Bar graph summarizing
the effect of Ni2+ (40-50 µM) on the
peak amplitude of the subthreshold Ca2+ responses
(n = 10, mean + SD). In each of these experiments,
five responses in control conditions and 10 min after wash in of
Ni2+ were averaged.
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Figure 4.
D890 blocks VGCC, but not the spine
Ca2+ signal. A, C, confocal images of
dendritic segments from two different cells containing active spines.
Traces from regions of interest in A and
C are displayed in B and
D/E, respectively. B, Top
traces, Within 5 min of whole-cell recording with a pipette
solution containing 1 mM D890, somatic depolarization (from
60 to 0 mV) evoked a large Ca2+ elevation in
spines and dendrites. Bottom traces, Ten minutes later,
even longer depolarization failed to evoke any Ca2+
transient. D, E, Current-clamp recording, otherwise
identical conditions as in B. In the presence of D890, a
strong somatic current injection failed to induce any
Ca2+ transient in the spine or dendrite
(D), whereas a single EPSP induced a clear spine
Ca2+ signal (E).
F, The mean peak amplitude of synaptic spine
Ca2+ signals recorded with D890 containing
intracellular solution (n = 11, mean + SD) was
similar to the mean value obtained in control conditions
(n = 8, mean + SD) Responses were evoked by two
stimuli given at 50 Hz.
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If the subthreshold Ca2+ signals in spines
are attributable to NMDARs, the Ca2+
signals should be increased by depolarizations that relieve the Mg2+ block and decreased by
hyperpolarizations that enhance the Mg2+
block. To test this prediction we studied synaptically mediated signals
using D890 to block VGCC. To minimize errors caused by dye saturation,
we used a low-affinity Ca2+ indicator,
Magnesium Green (Kd, ~6
µM). Furthermore, it was necessary to use a
brief burst of stimuli (3 pulses, 50 Hz) to obtain a sufficiently large
and reproducible Ca2+ signal (Fig.
5A). Despite these
precautions, such experiments are difficult to quantify because of
several additional potential sources of error [for example,
modulations of NMDARs permeability by Ca2+
and Na+ accumulations (Rosenmund and
Westbrook, 1993 ; Yu and Salter, 1998 ) and possible dye
nonlinearities]. Thus, although we trust the basic qualitative
observation concerning the voltage dependence, one has to be cautious
when interpreting the results quantitatively. The main conclusion we
draw from Figure 5B is that the spine
Ca2+ signal is very large at a holding
voltage of ~0 mV and becomes smaller at more negative and more
positive membrane potentials, consistent with the voltage dependence of
NMDA receptor-mediated currents (Mayer et al., 1984 ; Nowak et al.,
1984 ; Garaschuk et al., 1996 ). The voltage dependence of the
synaptically evoked spine Ca2+ signal is
similar to that of Ca2+ transients evoked
by NMDA receptor activation through agonist application. Thus, at
holding voltages of approximately 80 mV, the spine
Ca2+ signal was virtually abolished. At
very positive holding voltages, the Ca2+
signals also become smaller, as expected because of the decrease in the
driving force for Ca2+ (Mayer et al.,
1987 ; Schneggenburger et al., 1993 ; Garaschuk et al., 1996 ). Under
these conditions, we also measured the voltage dependence of the late
component of the EPSC (Fig. 5D). This component is blocked
by APV (Fig. 5C) and can thus be attributed to the NMDA
channel (Fig. 5C). The current-voltage curve is consistent with that reported previously (Hestrin et al., 1990 ; Keller et al.,
1991 ) and indicates that neither the Ca2+
indicator nor D890 has substantially altered the behavior of NMDARs.
These results further support the idea that the spine Ca2+ signals are attributable to
Ca2+ entry through the NMDARs.

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Figure 5.
Fluorescence-voltage relationships
(F-V) of synaptic Ca2+
transients in spines. A, Representative example of a
transient evoked by a brief burst stimulation recorded at
Vh = 40 mV. The inset
shows the associated EPSC, traces are averages of five individual
recordings. The intracellular solution contained D890 (2 mM) and the low-affinity calcium indicator dye Magnesium
Green (Kd, ~6 µM, 300 µM). B, F-V relations of
the peak amplitude of the spine Ca2+ signals as
measured with Magnesium Green (n = 3-6
measurements from 6 cells). Data were normalized to the values obtained
at 40 mV. The line represents a polynomial fit of the
data. C, EPSCs recorded at
Vh = 30 mV. Bath application of APV
reversibly abolished a late component (shaded area) that
was quantified (D) by integrating the EPSC
between 60 and 160 msec (indicated by broken lines)
after the last peak of the EPSC. EPSCs are averages of three
consecutive responses evoked by triplet stimulation. D,
Charge-voltage relationship (Q-V) of the late
EPSC component, measured as indicated in C. Data were
obtained from the cells that were analyzed in B. Error
bars represent SD (n = 3-6 measurements from 6 cells). The intracellular solution contained 2 mM of D890
(A-D). Synaptic responses were evoked by two or
three stimuli at 50 Hz.
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Although the spine signals may be attributable to the NMDARs, it
remains possible that the role of actual
Ca2+ entry through the channel is to
trigger a more massive release of Ca2+
from intracellular stores. Indeed, it has recently been proposed that
the direct entry through NMDARs is undetectable and that the signals
are attributable to Ca2+-induced
Ca2+ release (Emptage et al., 1999 ). This
proposal was based on the observation that spine
Ca2+ signals are blocked by ryanodine, a
drug that has been rigorously shown in skeletal muscle to be an
antagonist of Ca2+-induced
Ca2+ release from internal stores, and by
CPA, a drug that blocks the ATP-dependent uptake into stores and
therefore leads to their depletion (Ehrlich et al., 1994 ). Figure
6A-C shows the results of experiments in which we bath-applied either ryanodine or CPA. Neither agent produced a dramatic inhibition of either synaptic transmission (see also Fig. 7) or the
size of the spine signals. The summary of experiments in Figure
6D shows that, at most, the reduction in
Ca2+ signals was 30%. Critical to the
interpretation of these experiments is verification of the efficacy of
the applied drugs. Two results establish this efficacy. First, in the
same set of experiments in which we looked for effect of ryanodine and
CPA on spine signals in the outer region of the stratum radiatum, we
applied caffeine to more proximal dendritic regions. In CA1 pyramidal
cells, caffeine releases Ca2+ from
intracellular stores that contain ryanodine receptors (Garaschuk et
al., 1997 ). We locally applied caffeine from a pipette by pressure and
were able to detect a local Ca2+ elevation
in proximal dendrites. This caffeine-induced signal was almost
completely blocked within 10-20 min of either ryanodine or CPA
application (Fig. 6D).

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Figure 6.
Contribution of internal Ca2+
stores to synaptic Ca2+ signaling in spines.
A, EPSP-associated spine Ca2+ signal
(color-coded image and top trace) was
reduced by ~30% in the presence of ryanodine (25 µM,
bottom trace). B, Time course of the
effect of ryanodine (indicated by the bar) on the peak
amplitudes of Ca2+ transients. Same experiment as in
A. Single-shock stimuli were repeatedly delivered every
4 min, each data point represents a single trial. Note that there was
no failure of the Ca2+ signal with such stimulation
protocol. The dashed lines represent the values during
control conditions (1.0) and in the presence of ryanodine (0.72). The
numbers point to the individual recordings displayed in
A. C, Application of CPA (30 µM, indicated
by the bar) reduced the amplitude of synaptic
Ca2+ signals in spines by ~36%. D,
Bar graph summarizing the effects of ryanodine (20 or 25 µM) and CPA (30 µM). Data points were
normalized to control conditions. The first two bars represent the
effect on synaptically evoked Ca2+ signal in spines
(n = 7 and 9 cells for ryanodine and CPA,
respectively). The last two bars show that both drugs effectively
abolish dendritic Ca2+ responses evoked by local
application of caffeine (20-40 mM, n = 5 for ryanodine and for CPA). Data points were normalized to the mean
control value. Experiments were done at 30°C.
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Figure 7.
Clearance of spine Ca2+
involves internal stores. A, Synaptically evoked
Ca2+ signals in spines (top traces)
and the underlying EPSPs (bottom traces) during control
conditions and in the presence of ryanodine (20 µM). The
decay of the Ca2+ transients was not affected by
ryanodine. The solid lines represent exponential fits
with = 196 msec during control and = 183 msec in the
presence of ryanodine. B, Application of CPA (30 µM) markedly prolonged the decay of synaptic
Ca2+ signals (different cell than in
A). was estimated to be ~490 msec during control
conditions and ~720 msec in the presence of CPA. C, D,
The two drugs showed similar effects on AP-induced
Ca2+ signal in spines (same cells as in
A and B, respectively). The decay time
constants were 155 and 170 msec for ryanodine application and 507 and
1098 msec for CPA application (control and drug application,
respectively). E, F, Bar graphs summarizing the effects
of ryanodine (E, 20 or 25 µM,
n = 7) and CPA (F, 30 µM, n = 9) on the decay time constant
of Ca2+ transients induced either by synaptic
stimulation (EPSP) or by single AP (AP).
Asterisks denote significant changes compared to the
control conditions. All traces are averages of four or five consecutive
responses. Temperature was 30°C.
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A second set of experiments provided further support for the efficacy
of CPA and also provided evidence for a role of
Ca2+ stores in determining the time course
of spine signals. Previous work on dendritic signals in cortical
(Markram et al., 1995 ) neurons indicated that CPA slows the falling
phase of the AP-induced Ca2+ signals,
consistent with the idea that reuptake into stores contributes strongly
to Ca2+ clearance. Figure 7 shows that CPA
similarly slows the falling phase of the spine
Ca2+ signals caused either by synaptic
stimulation (Fig. 7B) or backpropagating action potentials
(Fig. 7D) (see also Mainen et al., 1999 ). The summary of
experiments is shown in Figure 7E. In contrast, ryanodine, which does not affect reuptake, did not slow the falling phase of the
signals (Fig. 7A,C,E).
 |
DISCUSSION |
Mechanism of subthreshold spine
Ca2+ signals
Our experiments indicate that the subthreshold
Ca2+ signals in dendritic spines are
primarily attributable to Ca2+ entry
through NMDARs. The signals are blocked by the NMDA receptor antagonist
APV and have a voltage dependence of the general form expected of the
NMDAR. Although the Ca2+ signals can be
enhanced by depolarization that relieves the
Mg2+ block of the NMDAR, the signals do
not require significant depolarization; they occur even when the EPSP
amplitude is only a few millivolts and they are only slightly reduced
when the EPSP is blocked with CNQX. It thus appears likely that the
signals occur because the NMDARs are in fact not completely blocked by
Mg2+ at resting potential. This
incompleteness is also apparent by the fact that current through the
NMDAR can be detected at resting potential. Thus, when the glutamate
from an individual vesicle is released it partially activates NMDARs
and thereby generates a significant Ca2+
signal in the postsynaptic spine.
Other sources of Ca2+ appear to contribute
to subthreshold spine signals in a minor way. For example, hippocampal
spines contain VGCC channels (Westenbroek et al., 1995 ). These could be
activated by the EPSP and contribute to the subthreshold spine
Ca2+ signals (Schiller et al., 1998 ).
Under our conditions, this component must be small because there is
only a small reduction of the spine signals when the EPSP is nearly
abolished with CNQX. Furthermore, the size of spine signals is not
substantially smaller if VGCC are blocked with
Ni2+ or D890. It remains quite possible,
however, that T-type Ca2+ channels, which
are known to be present in hippocampal neurons (Johnston et al., 1996 )
and to be sensitive to voltage in the range of resting potential, could
contribute significantly to spine signals under other conditions. It is
known that these channels are largely inactivated under resting
conditions, under hyperpolarized conditions this inactivation would be
removed, and they might then contribute significantly to synaptically
evoked spine signals (Magee et al., 1995 ; Magee and Johnston,
1995 ).
The finding that Ca2+ signals are not
significantly reduced by CNQX argues against the possibility that a
significant component of the signals is attributable to
Ca2+ entry through AMPA channels. This
conclusion is in line with earlier observations that CA1 pyramidal
cells express AMPA receptor channels with a low
Ca2+ permeability (Jonas and Sakmann,
1992 ), through which the fraction of Ca2+
is only one 20th of the Ca2+ charge
flowing through NMDARs (Garaschuk et al., 1996 ). Nevertheless, at
extremely hyperpolarized voltages (150-200 mV), the
Ca2+ entry through AMPA channels may be
significant and become detectable (Yuste et al., 1999 ).
The contribution of intracellular stores to the spine signals is also
small. We find that spine signals are only slightly reduced by
ryanodine and CPA, drugs that impair Ca2+
release from intracellular stores (Garaschuk et al., 1997 ). Analysis of
the kinetics of the spine signals shows that CPA slows the return of
Ca2+ to baseline levels after elevation of
Ca2+ by synaptic stimulation or by
eliciting a postsynaptic action potential. This slowing would be
expected if one of the mechanisms mediating this return was
Ca2+ pumping into internal stores
(diffusion into the dendrite and extrusion through the plasma membrane
are other likely mechanisms). Previous work in cortical neurons has
shown that CPA can produce such slowing of the falling phase of the
dendritic Ca2+ signal (Markram et al.,
1995 ). Our work shows that this is also true for spine signals (see
also Mainen et al., 1999 ). This slowing is not produced by ryanodine,
because pumping of cytoplasmic Ca2+ into
internal stores is not abolished by ryanodine.
Comparison to other studies on hippocampal and
cortical neurons
The study of the mechanism of subthreshold spine signals is in its
infancy, and it is of interest to discuss the points of agreement and
disagreement in the relatively small number of studies thus far. The
one point on which all studies of both hippocampal and cortical spine
signals agree is that the signals are blocked by NMDA receptor
antagonists. However, there is substantial disagreement about whether
the NMDAR can be activated at resting potential and the mechanism by
which the NMDAR contributes to the spine signal. With regard to the
question of whether the NMDAR can be activated at resting potential,
the critical experiment is whether CNQX, which nearly abolishes the
EPSP, abolishes the Ca2+ signal. We and
Köster et al. (1998) find little effect of CNQX. In contrast,
Yuste et al. (1999) found that signals are virtually abolished by CNQX.
The reasons for this discrepancy is unclear, but subtle differences in
methodological details, such as the holding voltage or the
Mg2+ concentration could conceivably be important.
The specific role of VGCCs in generating spine
Ca2+ signals in hippocampal cells has been
examined by us, by Yuste et al. (1999) , and by Emptage et al. (1999) ,
and there is agreement that these channels are not important in
generating subthreshold signals. Yuste et al. (1999) omitted ATP from
the internal solution and produced "washout" of VGCC, but observed
little change in spine signals. In our studies, blocking VGCC from
inside with D890 produced little change in the signals. It has been
previously argued that local subthreshold signals in dendrites could be
blocked by Ni2+, but the experimental
methods did not have sufficient resolution to resolve spines (Magee et
al., 1995 ). We and Emptage et al. (1999) have not detected a
substantial effect of Ni2+ on spine
signals, but this might depend strongly on the size of the EPSP, which
was much larger (20 mV) in the study of Magee et al. (1995) than in our
work (<10 mV).
Our study and that of Emptage et al. (1999) are the only to
specifically examine the role of intracellular
Ca2+ release in generating the
subthreshold Ca2+ signals, and our results
are in complete disagreement. Emptage et al. (1999) argue that the
Ca2+ that enters directly through the
NMDARs is too small to be measured and that the only detectable signals
are ones that have been enormously amplified by rapid intracellular
Ca2+ release. We argue that the direct
entry is detectable and that it is not substantially amplified.
Possible reasons for this discrepancy is the differences in electrical
recording methods (patch vs microelectrodes) and differences in slice
preparation (acute vs culture). The following rough calculation
indicates that even though 95% of the NMDAR conductance is blocked at
resting potential, the remaining Ca2+
entry should be sufficient to generate a detectable signal. The peak
NMDAR conductance during a quanta at +60 mV is 100 pS (estimated from
the peak current of 6 pA; Liao et al., 1995 ). This would yield a
current at 60 mV of 4 pA in the absence of
Mg2+ block (Spruston et al., 1995 ) (Fig.
4C). From Figure 4, C and F, of the
same paper it can be estimated that Mg2+
block at 60 mV produces a 94% reduction in current. Given that ~10% of the current is carried by Ca2+
(Garaschuk et al., 1996 ), taking the spine volume as 0.5 × 10 16 l (Harris and Stevens, 1989 ) and
assuming that 0.5% of the Ca2+ that
enters is free (Helmchen et al., 1996 ), a period of 50 msec of current
through the NMDARs would yield a rise of >500 nM
free Ca2+, well about the resting level of
60 nM (Regehr et al., 1989 ). Although our results
indicate that Ca2+ stores are not an
important source of Ca2+ during
low-frequency synaptic transmission, the stores do have importance as a
sink of Ca2+. We found that the return of
spine Ca2+ levels to baseline after
elevation by either action potentials or subthreshold synaptic events
was slowed when the pumping of Ca2+ into
intracellular stores was slowed by CPA.
Possible physiological implications of subthreshold
Ca2+ signals
Recent work raises the possibility that subthreshold signals may
be important in synaptic strengthening processes that occur under
certain neuromodulatory conditions. It has been found that activation
of the tyrosine kinase src can lead to the upregulation of the NMDAR
conductance and to long-term enhancement of AMPA-mediated transmission,
an enhancement that occludes with LTP (Lu et al., 1998 ). Interestingly,
this src-induced potentiation can occur without significant synaptic
stimulation, the only stimulation being infrequent (subthreshold) test
pulses. Nevertheless, this enhancement can be blocked by NMDAR
antagonists and by intracellular Ca2+
buffers. These results suggest that NMDAR-mediated
Ca2+ entry evoked by weak synaptic
stimulation may under certain conditions be able to trigger synaptic strengthening.
Subthreshold Ca2+ signals may also play a
role during higher frequency synaptic events that induce synaptic
plasticity. One clear example is long-term depression (LTD) and
depotentiation, which can be triggered by subthreshold stimulation
(Stevens and Wang, 1994 ; Stäubli and Ji, 1996 ) and which are
known to be dependent on an activity-dependent rise in intracellular
Ca2+ concentration. In most laboratories,
LTD can be blocked by NMDA receptor antagonists, suggesting that
Ca2+ entry is the trigger for LTD (for
review, see Bear and Abraham, 1996 ). The
Ca2+ signals we have detected may thus be
the signal that triggers LTD. However, further work is required to
establish this point because LTD induction requires repetitive synaptic
stimulation in the 1-5 Hz range, whereas we have only examined
responses at lower frequencies. Another possible function of
subthreshold signals that needs to be considered in view of recent work
is a role in receptor "homeostasis". It has been shown that when
all basal glutamatergic synaptic activity is abolished, profound
changes in glutamate sensitivity (O'Brien et al., 1998 ; Turrigiano et al., 1998 ), the number of glutamate receptors (Rao and Craig, 1997 ;
Lissin et al., 1998 ), and the number of spines (McKinney et al., 1999 )
can occur. Thus, it is possible that subthreshold Ca2+ signals in spines are part of a
maintenance process of the basal functional properties (e.g., through
Ca2+-dependent phosphorylation of receptor
channels) at the level of individual synaptic inputs.
 |
FOOTNOTES |
Received Aug. 17, 1999; revised Dec. 8, 1999; accepted Dec. 10, 1999.
This work was supported by grants from Human Frontier Science
Program and Deutsche Forschungsgemeinschaft to A.K. and J.E. and
National Institutes of Health Grant NS 35083 to J.L. We thank O. Garaschuk for comments on the manuscript and N. Rothgerber and E. Eilers for technical help.
Correspondence should be addressed to A. Konnerth, TU München,
Institut für Physiologie, 80802 München, Germany. E-mail: konnerth{at}physiol.med.tu-muenchen.de.
Dr. Lisman's present address: Department of Biology, Brandeis
University, Waltham, MA 02254.
 |
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