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1 Queensland Brain Institute, School of Biomedical Sciences, University of Queensland, Australia and Division of Neuroscience, John Curtin School for Medical Research, Australian National University, Canberra, Australia
| Abstract |
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(Received 3 October 2004;
accepted after revision 11 November 2004;
first published online 18 November 2004)
Corresponding author P. Sah: Queensland Brain Institute, School of Biomedical Sciences, St Lucia, Queensland 4072, Australia. Email: pankaj.sah{at}uq.edu.au
| Introduction |
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Neurones express a large diversity of voltage-gated Ca2+ channels that have been divided into low-voltage-activated (LVA) and high-voltage-activated (HVA) channels (Ertel et al. 2000). LVA (T-type) channels mediate rapidly inactivating currents that provide a transient Ca2+ influx in response to subthreshold depolarizations (Magee & Johnston, 1995; Perez-Reyes, 2003) whereas HVA (L, P/Q, N and R types) channels (Ertel et al. 2000) generate sustained currents that activate at suprathreshold membrane potentials (Magee & Johnston, 1995). These Ca2+ channels can also be distinguished pharmacologically, with LVA channels being selectively sensitive to low concentrations of nickel. Among the HVA channels, L-type channels are sensitive to dihydropyridines, N-type channels are blocked by
-conotoxin, P/Q-type channels by agatoxin, while the R-type channels are insensitive to these agents. Functionally, LVA channels have been proposed to be involved in the generation of burst firing (Huguenard, 1996). Of the HVA channels, L-type voltage-dependent Ca2+ channels (L-VDCCs) have been implicated in the regulation of synaptic plasticity and gene transcription (Finkbeiner & Greenberg, 1998; Dolmetsch et al. 2001; West et al. 2001). A low-voltage-activated, voltage-dependent Ca2+ current that activates with pharmacological properties similar to that of L-type Ca2+ channels has also been described in hippocampal neurones (Avery & Johnston, 1996; Magee et al. 1996). These currents have now been described in a number of cell types (Lipscombe, 2002); however, their functional role in central neurones is not known.
Long-term synaptic plasticity within the basolateral amygdala (BLA) has been proposed as the cellular mechanism that underlies the storage of fear-related memory (Blair et al. 2001; Davis & Whalen, 2001; Sah et al. 2003). Infusion of L-VDCC antagonists into the BLA impairs acquisition of the fear-conditioned response in rats (Bauer et al. 2002; Shinnick-Gallagher et al. 2003) (but see Cain et al. 2002). Long-term potentiation induced by pairing trains of action potentials with synaptic stimulation is blocked by the dihydropyridine nicardipine (Weisskopf et al. 1999; Bauer et al. 2001, 2002). It has therefore been proposed that activation of high-voltage-activated L-VDCCs is in part necessary for the induction of synaptic plasticity in the amygdala (Blair et al. 2001). Here, we show that projection neurones in the BLA express a low-voltage-activated L-VDCC. Activation of this current at subthreshold membrane potentials refills inositol 1,4,5 trisphosphate (IP3)-sensitive intracellular Ca2+ stores.
| Methods |
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In Ca2+-imaging experiments, patch pipettes (25 M
) were filled with an internal solution containing (mM): 135 KMeSO4, 8 NaCl, 10 Hepes, 2 Mg2ATP, 0.3 Na3GTP (pH 7.3 with KOH, osmolarity 280290 mosmol l1) and the Ca2+ indicator Oregon Green BAPTA-1 (Molecular Probes; 50 µM for whole-field and 100 µM for confocal experiments). Ca2+ currents were measured using an with an internal solution containing (mM): 135 Cs-MeSO4, 8 NaCl, 10 Hepes, 2 Mg2ATP, 0.3 Na3GTP (pH 7.3 with KOH, osmolarity 280290 mosmol l1) in the presence of 510 mM CsCl, 510 mM 4-aminopyridine (4AP), 510 mM TEACl, 500 nM TTX, 10 µM CNQX, 30 µMD-aminophosphonovalerate (APV), 10 µM bicuculline. The addition of TEA, CsCl and 4AP was accompanied by an iso-osmotic reduction of NaCl. Ca2+ current experiments were performed at near room temperature (23°C). Capacitive transients and leak currents were subtracted using a series of 5 mV hyperpolarizing steps of equal duration. In some experiments phosphocreatine (7 mM) and spermine (0.1 mM) were also added to the internal solution. Junction potentials were not corrected for. Electrophysiological signals were recorded with either an Axopatch 1D amplifier or a Multiclamp 700 amplifier (Axon Instruments), digitized at 10 kHz with an ITC-16 board (Instrutech), and controlled using Axograph (Axon Instruments). Electrophysiological data were analysed using Axograph. Trains of action potentials were evoked by repetitive injection of a suprathreshold (12 nA, 12 ms) current injection at the indicated frequency.
Whole-field fluorescence measurements were made using a monochromator-based imaging system, Polychrome II (TILL Photonics). Neurones were visualized using a BX50 microscope (Olympus) equipped with a x60 water immersion objective (NA 0.9, Olympus) and illuminated with 488 nm light. IP3 was uncaged using a pulsed xenon arc lamp (TILL Photonics), which illuminated the entire field of view and discharged
80 J in 2 ms. Light from both the monochromator and the flash were delivered to the BX50 microscope via a quartz light guide and a custom epiflourescence attachment provided by TILL photonics. Images were acquired with an in-line transfer, cooled CCD camera (TILL photonics) in which the scan lines were binned by two in both horizontal and vertical directions giving a spatial resolution of 0.33 µm pixel1. Frames were collected at 2533 Hz with an exposure time of 1020 ms per frame. Images were analysed off line using Vision (TILL Photonics). Small regions of interest were selected over the extranuclear soma and the proximal dendrite (2050 µm from the soma), and the fluorescence over this region was averaged.
Single- and two-photon confocal fluorescence images were obtained using a Zeiss Axioskop 2FS (x63 objective) with a 510 laser scanning head, and equipped with an argon laser for single-photon illumination, and a Verdi solid-state pump laser and a Mira 900-F femptosecond Ti:S pulsed laser (Coherent Scientific) for two-photon excitation. The excitation wavelengths were 488 nm for single-photon excitation, and 800 nm for two-photon excitation. When acquiring single-photon confocal data, the detector pinhole aperture was set to give a vertical resolution of <1.5 µm. Small segments were selected over each subcellular region, and the fluorescence over this region was averaged. Single- and two-photon confocal data were pooled.
Kinetic sequences were constructed over time for each of the selected regions. Kinetic sequences were calculated as the relative change in fluorescence over baseline fluorescence (
F/F).
F/Ft= (FtF0)/(F0B) where Ft is the fluorescence at time t, F0 is the average baseline fluorescence prior to the stimulus, and B is the background fluorescence measured in an adjacent extracellular region. In some cases the Ca2+ concentration was estimated using methods published by Maravall et al. (2000). To estimate Ca2+ changes (
[Ca2+]) and resting Ca2+ (
[Ca2+]0), we used the following formulae:
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Fmax were obtained by measuring the amplitude of a saturating fluorescence plateau evoked by a high-frequency train of action potentials (500 ms, 100 Hz).
-Conotoxin GVIA was purchased from Alomone Labs (Jerusalem, Israel). Caged myo-inositol 1,4,5-trisphosphate (caged IP3) was purchased from Molecular Probes. All other drugs were purchased from Sigma. Stock solutions of nicardipine were prepared in ethanol. Stock solutions of caffeine, ryanodine and BayK 8644 were prepared in DMSO. Caged IP3 and ruthenium red were added to the internal solution. Muscarine (10 µM) was applied by picospritzer (1520 p.s.i., 300600 ms; Parker Hannifin Fairfield, NJ, USA) application through a patch pipette. All other drugs were bath applied.
-Agatoxin IVA and
-conotoxin GVIA were coapplied with 0.1 mg ml1 cytochrome C (Sigma).
Statistical analyses were made using StatView (SAS Institute). Statistical comparisons were made using ANOVA or as otherwise indicated. Data are presented as means ±S.E.M.
| Results |
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F/F in the proximal dendrite (n= 49) and 0.13 ± 0.01
F/F in the soma (n= 67), with an onset time constant of 131 ± 13 ms in the dendrite and 433 ± 43 ms in the soma for projection neurones in the basal nucleus. We estimated the resting [Ca2+]i in the proximal dendrite to be 79 ± 10 nM, and depolarization of cells from 80 to 50 mV raised cytosolic Ca2+ by 38 ± 7 nM(n= 5). For comparison, projection neurones in the lateral amygdala showed a steady-state rise of 0.16
F/F in the proximal dendrite (n= 2), and 0.12 ± 0.03
F/F in the soma (n= 4). In CA1 pyramidal neurones, where sustained low-voltage-activated Ca2+ currents have been previously described (Magee et al. 1996), a depolarizing step from 80 to 50 mV evoked a steady-state rise in fluorescence of 0.09 ± 0.03
F/F in the proximal dendrite, and 0.07 ± 0.02
F/F in the soma (n= 4). Assuming that resting cytosolic Ca2+ is similar in all three cell types, these data suggest that subthreshold rises in Ca2+ are larger in projection neurones of the BLA. The voltage-dependent rise in Ca2+ was persistent as shown by the decrease in cytosolic Ca2+ when neurones were hyperpolarized from a steady holding potential of 50 mV (Fig. 1D). To examine the spatial extent of the voltage-dependent Ca2+, rise we used confocal imaging to follow the dendrites distally (Fig. 2A). Subthreshold depolarization evoked a rise in cytosolic Ca2+ in all compartments of the neurone, including nucleus and dendritic spines (Fig. 2B), with the largest rise observed in the proximal dendrites. Due to the slow time course of the response, it was not possible to determine whether these low-voltage-activated Ca2+ channels are located on the spines themselves, or whether Ca2+ in the spines diffused from the dendrite into the spine.
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-conotoxin had no effect on the subthreshold Ca2+ rise (15 ± 14%), while greatly attenuating the EPSP evoked by external capsule stimulation (80%; n= 2). In contrast, the P/Q-type Ca2+ channel blocker
-agatoxin IVa (200 nM) reduced the subthreshold Ca2+ rise by 30 ± 3% in the soma (P < 0.001; n= 6) and 21 ± 3% in the proximal dendrite (P < 0.01; n= 5). The partial block of the Ca2+ rise by
-agatoxin suggests that P/Q-type channels may also be activated in the subthreshold voltage range in BLA neurones. However, dihydropyridine block of low-threshold L-type Ca2+ channels has been shown to be incomplete (Xu & Lipscombe, 2001). When
-agatoxin was applied in the presence of nicardipine, the reduction in the amplitude of the residual Ca2+ rise was only 15%(n= 2). These results suggest that the pharmacology of voltage-gated Ca2+ channels is not as well defined as generally thought.
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To isolate low-voltage-activated Ca2+ currents, wholecell recordings were made using a caesium-methanesulphonate-based internal solution in the presence of TTX, CsCl, 4AP, TEA, CNQX, APV and bicuculline. When neurones were held at 80 mV, depolarizing voltage steps to 50 mV evoked a small sustained inward current (Fig. 4). In some instances we observed that a small transient component, reminiscent of T-type Ca2+ current, was also present. The sustained component was reduced by nicardipine (45 ± 17%; n= 6; P < 0.05) and augmented by BayK 8644 (113 ± 67%; n= 5; P < 0.001) (Fig. 4D). We next tested whether L-VDCCs are necessary for subthreshold Ca2+ entry in the soma and proximal dendrite or are simply favoured during prolonged depolarizations which would inactivate T-type channels. To promote Ca2+ entry via T-VDCCs, neurones were voltage clamped at 80 mV, and 20 ms depolarizing pulses to 50 mV were given at 20 Hz. The subthreshold pulse train evoked a Ca2+ rise that was smaller than that evoked by the sustained depolarization (47 ± 18 and 33 ± 18% of the sustained step in soma and dendrite; n= 4). These results suggest that in BLA neurones, like other neurones, T-VDCCs may be preferentially located on more distal dendrites (Perez-Reyes, 2003). Together, these results show that the rise in cytosolic Ca2+ during subthreshold depolarizations is mediated principally by activation of a non-inactivating, low-threshold, dihydropyridine-sensitive, voltage-dependent Ca2+ channel.
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F/F increased from 33 ± 14 to 205 ± 97% of the initial Ca2+ response in the soma (n= 9; Wilcoxon signed rank, P < 0.05) and from 72 ± 27 to 334 ± 238% of the initial Ca2+ response in the proximal dendrite (n= 8; Wilcoxon signed rank, P < 0.05). Furthermore, when neurones were voltage clamped at 50 mV to tonically activate L-type channels (Fig. 1), release of Ca2+ could be repetitively evoked (e.g. Figure 7D).
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F/F increased from 33 ± 8 to 52 ± 11% of the initial Ca2+ response in the soma (n= 7), and from 45 ± 13 to 71 ± 13% of the initial Ca2+ response in the proximal dendrite (n= 6). Application of nicardipine reduced the somatic AP-evoked Ca2+ response by 31 ± 10%(n= 4). However, unlike subthreshold depolarization, store reloading following action potentials was not blocked by nicardipine (Fig. 6C). Thus, Ca2+ entry via other Ca2+ channels can contribute to AP-mediated store filling.
Ca2+ can also be released from intracellular Ca2+ stores via activation of ryanodine receptors, which are abundant in neurones (Sharp et al. 1993). Caffeine activates ryanodine receptors (Zucchi & Ronca-Testoni, 1997) and antagonizes the actions of IP3 (Parker & Ivorra, 1991). Focal application of caffeine evoked a rise in free intracellular Ca2+ in the soma and proximal dendrites (Fig. 7A), indicating the presence of ryanodine-sensitive Ca2+ stores. At hyperpolarized potentials, the caffeine-evoked Ca2+ response ran down with repeated stimulation, and was augmented by subthreshold depolarization (Fig. 7A and B). Following a subthreshold depolarization, the caffeine-evoked
F/F increased from 41 ± 9 to 84 ± 26% and from 51 ± 14 to 81 ± 42% of the initial Ca2+ response in soma (n= 6) and proximal dendrite (n= 4), respectively. We next tested whether ryanodine receptors (RyR) and IP3 receptors share a common pool of Ca2+. At low concentrations, ryanodine depletes RyR-sensitive Ca2+ stores by locking the RyR in the open state (Rousseau et al. 1987). Application of ryanodine (10 µM) reduced the muscarine-evoked Ca2+ rise to 9.4% of control (n= 4; Fig. 7C). However, the muscarine-evoked Ca2+ rise did not require RyR activation, since robust muscarine-evoked Ca2+ rises were observed when the RyR antagonist ruthenium red was included in the patch pipette (Fig. 7D). Furthermore, ruthenium red also occluded the action of ryanodine (96.4% of control; n= 2; Fig. 7D). Thus, the blockade of the IP3-mediated response by ryanodine was due to store depletion, and, as in hippocampal pyramidal neurones (Power & Sah, 2002), ryanodine and IP3 receptors in BLA neurones share a common Ca2+ pool.
Synaptic activation of metabotropic receptors on cortical and hippocampal neurones, and the subsequent release Ca2+ from IP3-sensitive intracellular Ca2+ stores, also lead to the generation of propagating Ca2+ waves (Nakamura et al. 1999; Power & Sah, 2002; Larkum et al. 2003). Similarly, tetanic subthreshold stimulation of inputs to BLA neurones also generated a focal rise in Ca2+ in the proximal dendrite (1050 µm from the soma) that began 3001000 ms after the first stimulus and propagated as a wave toward the soma (Figs 8 and 9B). This Ca2+ wave closely resembled those described in hippocampal and cortical pyramidal neurones (Nakamura et al. 1999; Power & Sah, 2002; Larkum et al. 2003). In hippocampal and cortical pyramidal neurones, multiple trains of action potentials have been reported to replenish the generation of Ca2+ waves (Jaffe & Brown, 1994). However, in vivo, projection neurones in the basolateral complex are largely silent (Paréet al. 1995), and recordings during some forms of fear conditioning have indicated that most projection neurones do not reach threshold during the induction of fear conditioning (Rosenkranz & Grace, 2002). We therefore asked whether Ca2+ stores could be replenished solely by subthreshold Ca2+ entry. When neurones were voltage clamped at 70 mV, synaptically evoked Ca2+ waves ran down with repeated stimulation, consistent with a reduction in store Ca2+ content (Fig. 9A). Brief (1 min) subthreshold depolarization of the neurone to 50 mV resulted in a transient restoration of the synaptically evoked Ca2+ rise (Fig. 9A and D). Following the depolarizing voltage step,
F/F increased from 29 ± 12 to 569 ± 429% of the initial Ca2+ response in the soma (n= 10; Wilcoxon signed rank; P < 0.01), and from 33 ± 12 to 192 ± 57% of the initial Ca2+ response in the proximal dendrite (n= 10; Wilcoxon signed rank, P < 0.01). In some neurones, synaptic stimulation at resting membrane potentials was unable to generate Ca2+ waves, but a brief depolarization of the cell to 50 mV enabled the neurones to generate waves (Fig. 9C). This finding suggests that in acute brain slices, basal store content is low in some neurones.
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| Discussion |
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Subthreshold depolarization of BLA pyramidal neurones, either by current injection or summating synaptic potentials, caused a sustained Ca2+ influx. This rise in Ca2+ was not due to influx via NMDA receptors or to activation of low-voltage-activated, T-type Ca2+ channels (Magee et al. 1995), since it was insensitive to APV and low concentrations of nickel. However this Ca2+ rise was blocked by the dihydropyridine nicardipine and potentiated by BayK 8644 showing that it is due activation of an L-type voltage-dependent Ca2+ current. Under voltage clamp we have identified a small persistent inward current with similar dihydropyridine sensitivity. While, L-type Ca2+ channels generally activate at suprathreshold membrane potentials, a low-threshold L-type Ca2+ current has previously been described in hippocampal pyramidal neurones (Avery & Johnston, 1996; Magee et al. 1996). Currents with these properties have recently been shown be due to the Cav1.3 gene product (
1D) (Koschak et al. 2001; Xu & Lipscombe, 2001). In agreement with our data,
1D transcripts are also expressed in the BLA (Shinnick-Gallagher et al. 2003). These currents are involved in transmitter release in hair cells and in setting the threshold for action potential generation in the sinoatrial note (Platzer et al. 2000). However, the physiological role of this current in central neurones is not known.
Our results show that Ca2+ influx via low-threshold Ca2+ channels is sequestered within the ER, and is necessary to maintain the filling status of IP3-sensitive Ca2+ stores. Filling of internal Ca2+ stores in neurones has been previously demonstrated during suprathreshold depolarizations that open high-threshold, voltage-dependent Ca2+ channels, and lead to large rises in cytosolic Ca2+ (Pozzo-Miller et al. 1996, 1997). In cultured hippocampal neurones, L-type VDCCs have been shown to contribute to the filling status of IP3-sensitive Ca2+ stores (Rae et al. 2000). However, in those studies Ca2+ channels were activated by either increasing extracellular K+ or suprathreshold depolarization for several minutes. In BLA neurones, repetitive release of IP3-sensitive Ca2+ stores at negative membrane potentials led to a clear decline in store content. A subthreshold depolarization caused only a modest rise in cytosolic free-Ca2+, but significantly replenished IP3-sensitive Ca2+ stores. The rise in cytosolic Ca2+ during subthreshold depolarization was largely, but not fully blocked by nicardipine, consistent with the incomplete block of
1D channels by dihydropyridines (Xu & Lipscombe, 2001). However, the refilling of internal stores was abolished by nicardipine, showing that Ca2+ entering the cytosol via low-threshold L-type Ca2+ channels is in part sequestered within the ER.
Action potentials also activate high-threshold, voltage-dependent Ca2+ channels leading to large, brief rises in cytosolic Ca2+ (Markram et al. 1995). This Ca2+ is in part buffered by uptake into the ER. In BLA neurones, while trains of action potentials could reload intracellular stores, it was less robust than subthreshold-depolarization-evoked store loading. It is notable that while action potential trains are capable of filling IP3-sensitive Ca2+ stores, projection neurones in the basolateral complex are largely silent in vivo (Paréet al. 1995). This suggests that, in BLA projection neurones, store content is largely controlled by subthreshold activation of dihydropyridine-sensitive Ca2+ channels.
The amygdala has been consistently implicated in fear conditioning, and long-term synaptic plasticity within the basolateral amygdala has been proposed as the cellular mechanism that underlies the storage of fear-related memory (LeDoux, 2000; Davis & Whalen, 2001). It is becoming increasing apparent that synaptic plasticity requires activation of intracellular Ca2+ stores (Rose & Konnerth, 2001; Barbara, 2002; Fitzjohn & Collingridge, 2002). These rises in Ca2+ have been suggested to have a role in the mechanisms that underlie synaptic plasticity and the initiation of gene transcription (West et al. 2001). In the BLA, dihydropyridine-sensitive, voltage-dependent Ca2+ channels and metabotropic receptor activation are necessary for fear conditioning and some forms of long-term potentiation (Weisskopf et al. 1999; Bauer et al. 2002; Fendt & Schmid, 2002; Rodrigues et al. 2002). Intracellular recordings during some forms of fear conditioning have shown that most projection neurones do not reach threshold during the induction of fear conditioning (Rosenkranz & Grace, 2002). Furthermore, action potentials which are evoked would be riding upon depolarizations. Our results show that brief subthreshold depolarizations, similar to what has been reported during the conditioned stimulus (Rosenkranz & Grace, 2002), can refill IP3-sensitive Ca2+ stores. These channels are therefore well suited to provide a cellular memory trace of prior subthreshold synaptic activity. Thus, neurones that are sufficiently depolarized by the conditioned stimulus would be more apt to show an augmented Ca2+ response to the subsequent unconditioned stimulus due to release from intracellular stores. This may be the basis of the dyhydropyridine sensitivity of fear conditioning and LTP in the lateral amygdala.
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