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The Journal of Neuroscience, September 1, 1998, 18(17):6650-6661
Inwardly Rectifying Potassium (IRK) Currents Are Correlated
with IRK Subunit Expression in Rat Nucleus Accumbens Medium Spiny
Neurons
Paul G.
Mermelstein,
Wen-Jie
Song,
Tatiana
Tkatch,
Zhen
Yan, and
D. James
Surmeier
Department of Anatomy and Neurobiology, College of Medicine,
University of Tennessee, Memphis Tennessee 38163
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ABSTRACT |
Inwardly rectifying K+ (IRK) channels are
critical for shaping cell excitability. Whole-cell patch-clamp and
single-cell RT-PCR techniques were used to characterize the inwardly
rectifying K+ currents found in projection neurons
of the rat nucleus accumbens. Inwardly rectifying currents were highly
selective for K+ and blocked by low millimolar
concentrations of Cs+ or Ba2+. In
a subset of neurons, the inwardly rectifying current appeared to
inactivate at hyperpolarized membrane potentials. In an attempt to
identify this subset, neurons were profiled using single-cell RT-PCR.
Neurons expressing substance P mRNA exhibited noninactivating inward
rectifier currents, whereas neurons expressing enkephalin mRNA
exhibited inactivating inward rectifier currents. The inactivation of
the inward rectifier was correlated with the expression of IRK1
mRNA. These results demonstrate a clear physiological difference in the
properties of medium spiny neurons and suggest that this difference
could influence active state transitions driven by cortical and
hippocampal excitatory input.
Key words:
ventral striatum; medium spiny neurons; single-cell
RT-PCR; voltage clamp; potassium channels; inward rectifier; enkephalin; substance P
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INTRODUCTION |
The nucleus accumbens (NAcc)
constitutes the major subdivision of the ventral striatum (Chronister
and DeFrance, 1981 ; Groenewegen et al., 1991 ). It is involved in both
limbic and extrapyramidal motor systems (Mogenson et al., 1980 ; Fibiger
and Phillips, 1986 ; Mogenson, 1987 ; Robbins et al., 1989 ) as well as
being the major site of action for many drugs of abuse (Swerdlow and
Koob, 1987 ; Koob and Bloom, 1988 ). GABAergic medium spiny projection
neurons constitute the vast majority (~95%) of neurons in the NAcc.
Based on peptide expression and efferent connections, neurons have been subdivided into two major classes. Substance P (SP)-expressing neurons
primarily project to the ventral tegmental area, whereas enkephalin (ENK) neurons mainly project to the ventral pallidum (Zahm
et al., 1985 ; Heimer et al., 1991 ; Le Moine and Bloch, 1995 ). Because
of their involvement in a variety of behaviors, understanding how the
excitability of NAcc neurons is regulated is of broad functional
significance.
One of the principal determinants of medium spiny neuron activity in
the NAcc (and dorsal striatum) is an inwardly rectifying K+ (IRK) current (Uchimura et al., 1989 ; Uchimura
and North, 1990 ; Wilson, 1993 ). K+ currents of this
type play an important role in a variety of cellular functions. For
example, they are crucial determinants of the resting potential and
synaptic integration (Hille, 1992 ; Wilson, 1993 ). The gating of
inwardly rectifying K+ channels (Kir) is strongly
dependent on extracellular concentrations of K+
(Hille, 1992 ). These channels rectify because they are blocked by
intracellular Mg2+ and polyamines at potentials
positive to the K+ equilibrium potential
(EK) (Matsuda, 1991 ; Fakler et al., 1994 ; Ficker et al., 1994 ; Lopatin et al., 1994 ; Lu and MacKinnon, 1994 ; Stanfield et al., 1994b ; Wible et al., 1994 ; Yang et al., 1995 ; Lopatin
and Nichols, 1996 ). Based on amino acid homology, there are several
subfamilies of Kir channels that differ in rectification properties and
activation determinants (Doupnik et al., 1995 ). The best characterized
Kir channels found in brain are the IRKs (Kir2.0) and G-protein coupled
IRKs (Kir3.0). Of these two channel types, neurons of the rat
NAcc express primarily members of the IRK gene family (Karschin et al.,
1996 ).
Although currents attributable to IRK channels have been reported in
NAcc neurons (Uchimura et al., 1989 ; Uchimura and North, 1990 ), they
have not been studied with techniques that would allow a careful
description of their kinetic and pharmacological properties (for
review, see Stanfield et al., 1985 ; Takano et al., 1995 ). Furthermore,
despite the fact that IRK1-3 subunits have been detected within the
NAcc, their distribution within single cells has yet to be determined.
Therefore, the goals of this study were threefold: first, to
characterize the properties of inwardly rectifying currents in NAcc
medium spiny neurons using voltage-clamp techniques; second, to
determine how IRK1-3 subunit mRNA expression was coordinated within
these neurons using single-cell RT-PCR; and third, to determine whether
there was a correlation between IRK expression and the physiological
properties of the inwardly rectifying currents.
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MATERIALS AND METHODS |
Acute dissociation. NAcc neurons from ~4-week-old
rats were acutely dissociated using previously described protocols
(Surmeier et al., 1992 ; Bargas et al., 1994 ). Rats were anesthetized
with methoxyflurane (Mallinckrodt Veterinary Incorporated, Mundelein, IL) and decapitated. Brains were quickly removed, blocked, and sliced
on a DSK microslicer (Ted Pella, Redding, CA) in a 1-2°C sucrose
solution (in mM: 234 sucrose, 2.5 KCl, 1 Na2HPO4, 11 glucose, 4 MgSO4, 0.1 CaCl2, and 15 HEPES,
pH 7.35, 300 mOsm/l). Coronal slices (400 µm) were incubated 0.5-4
hr at room temperature in a sodium bicarbonate-buffered Earle's
balanced salt solution bubbled with 95% O2/5%
CO2 and containing (in mM): 1 kynurenic acid, 1 pyruvic acid, 0.1 N-nitroarginine, and 0.005 glutathione, pH
7.4, 300 mOsm/l. Individual slices were then placed in a
Ca2+-free buffer (in mM: 140 Na-isethionate, 2 KCl, 4 MgCl2, 23 glucose, and 15 HEPES, pH 7.4, 300 mOsm/l), and under a dissecting microscope, the NAcc
was isolated. The NAcc was then placed into an oxygenated, HEPES-buffered HBSS containing 1.5 mg/ml protease (type XIV) at 35°C for 30 min. The enzyme chamber also contained (in
mM): 1 kynurenic acid, 1 pyruvic acid, 0.1 N-nitroarginine, and 0.005 glutathione, pH 7.4, 300 mOsm/l.
Unless otherwise stated, all chemicals were obtained from Sigma (St.
Louis, MO). After enzymatic treatment, the tissue was rinsed several
times in the Ca2+-free buffer and triturated with a
graded series of fire-polished Pasteur pipettes. The cell suspension
was placed in a 35 mm Lux Petri dish (Nunc, Naperville, IL), which was
mounted on an inverted microscope. Cells were then given several
minutes to settle before electrophysiological recording.
Whole-cell recordings. Whole-cell recordings were performed
using standard techniques (Hamill et al., 1981 ; Bargas et al., 1994 ).
Electrodes were pulled from Corning (Corning, NY) 7052 glass
(Flaming/Brown P-97 puller; Sutter Instrument Co., Novato, CA) and
fire-polished (MF-83 microforge; Narishige, Hempstead, NY) just before
use. For recording inward currents, the intracellular recording
solution typically contained (in mM): 55 K2SO4, 30 KF, 26 sucrose, 5 HEPES, 5 BAPTA, 3 MgCl2, 2.8 CaCl2, 0.1 spermine, 12 phosphocreatine, 3 Na2ATP, and 0.2 Na3GTP, pH 7.2, 275 mOsm/l. As noted, intracellular
Ca2+ and calcium chealator concentrations were
varied without significant effect ([Ca]i was
systematically varied from 1 pM to 135 nM). The
intracellular recording solution for recording outward potassium currents was (in mM): 60 K2SO4, 80 N-methyl-glucamine
(NMG+), 40 HEPES, 5 BAPTA, 12 phosphocreatine, 3 Na2ATP, 0.2 Na3GTP, 2 MgCl2,
and 0.5 CaCl2, pH 7.2, 275 mOsm/l. The external
recording solution for measuring the inward rectifier typically
contained (in mM): 20 K-gluconate, 10 HEPES, 10 glucose, 56 sucrose, 154 NMG+, 2 MgCl2, and
0.5 CaCl2, pH 7.35, 300 mOsm/l. Concentrations of
extracellular potassium were varied in several experiments and are
noted. NMG+ was also substituted with either
Na+ or sucrose without effect on inward current
inactivation as well as the addition of 400 µM
CdCl2. For recording outward currents, the extracellular
recording solution contained (in mM): 140 Na-isethionate, 10 HEPES, 12 glucose, 17.5 sucrose, 5 KCl, 2 MgCl2,
and 0.4 CdCl2, pH 7.35, 300 mOsm/l. All reagents
were obtained from Sigma except ATP and GTP (Boehringer Mannheim,
Indianapolis, IN) and BAPTA (Calbiochem, La Jolla, CA). In specific
experiments, terfenadine and haloperidol were dissolved in DMSO as
1000× stocks. Final concentrations of DMSO were matched in all
recording solutions. Extracellular recording solutions were applied via
one of a series of six glass capillaries (~150 µm inner diameter)
in which gravity-fed flow was regulated by electronic valves (Lee Co.,
Essex, CT). Solution changes were performed by altering the position of
the drug array using a DC drive system controlled by a
microprocessor-based controller (Newport-Klinger, Irvine, CA). The
background solution that bathed cells not being recorded contained (in
mM): 140 NaCl, 23 glucose, 15 HEPES, 2 KCl, 2 MgCl2, and 1 CaCl2, pH 7.4, 300 mOsm/l.
Recordings were obtained with an Axon Instruments (Foster City, CA)
200A patch-clamp amplifier, controlled, and monitored with a 486 PC
running pCLAMP (version 6.0) with a 125 kHz interface (Axon
Instruments). Electrode resistances were ~5-7 M in bath. After
formation of the gigaohm seal and subsequent cell rupture, series
resistance was compensated (70-80%) and periodically monitored. Recordings were only obtained from medium-sized neurons. Medium spiny
neurons are primarily the projection neurons of the NAcc. Whole-cell
capacitance (4-9 pF) was similar to that observed previously for
dorsal neostriatal projection neurons (Mermelstein et al., 1996 ).
Recordings were performed at room temperature. The liquid junction
potential (2 mV) was not compensated.
Single-cell RT-PCR. Single-cell RT-PCR was performed using
protocols similar to those previously described (Surmeier et al., 1996 ;
Mermelstein and Surmeier, 1997 ). For all experiments, electrode glass
was heated to 200°C for >4 hr before being pulled. Extracellular solutions were generated from nominally RNase-free water (Milli-Q PF;
Millipore, Bedford, MA). Intracellular recording solutions contained
diethyl pyrocarbonate (DEPC)-treated Milli-Q water. In some
experiments, cells were collected without recording. Under these
circumstances, the intracellular solution only contained DEPC-treated
water. Gloves were worn by the experimenter at all times during the
experiment.
After seal rupture (and recording for those cells in which inward
rectifier inactivation and channel and peptide expression were
compared) the cell was aspirated into the electrode. The electrode
solution (~5 µl) was ejected into a thin-walled PCR tube (MJ
Research, Watertown, MA) containing 5 µl of DEPC-treated water, 0.5 µl of RNAsin (28,000 U/ml), 0.5 µl of dithiothreitol (DTT; 0.1 M), and 1 µl of oligo-dT (0.5 µg/ml). The tube, which was kept on ice during the recording session, was heated to 70°C for
10 min to linearize mRNA and placed again on ice for 1 min. Single-strand cDNA was generated from mRNA by adding to the PCR tube 1 µl of SuperScript II reverse transcriptase (200 U/µl), 2 µl of
10× PCR buffer (200 mM Tris-HCl and 500 mM
KCl), 2 µl of MgCl2 (25 µM), 1 µl of
dNTPs (10 µM), 0.5 µl of RNAsin (28,000 U/ml), and 1.5 µl of DTT (0.1 M). The reaction was at 42°C for 50 min
followed by 70°C for 15 min. After reverse transcription, mRNA was
eliminated by the addition of 1 µl of RNase H (2 U/µl) and heating
the PCR tube to 37°C for 20 min. All reagents except for RNAsin
(Promega, Madison, WI) were obtained from Life Technologies (Grand
Island, NY).
PCR amplification was performed using a thermal cycler (P-200, MJ
Research). For detection of enkephalin and substance P, 2 µl of RT
template was added to a thin-walled PCR tube containing 5 µl of 10×
PCR buffer (100 mM Tris-HCl and 500 mM KCl), 5 µl of MgCl2 (25 mM), 1 µl of dNTPs
(25 mM), 2.5 µl of upstream primer for either enkephalin
or substance P (20 mM), 2.5 µl of downstream primer (20 mM), 31.5 µl of autoclaved water, and 0.5 µl of
Taq polymerase (5000 U/ml). The thermal cycling program for
peptide amplification was 94°C for 1 min, 59°C for 1 min, and
72°C for 1.5 min for 45 cycles. Because of the apparent low abundance
of mRNA for IRK1-3, two-round PCR using multiplex-degenerate primers for round 1 was necessary. For the first round, 15 µl of template was
added to a thin-walled PCR tube containing 5 µl of 10× PCR buffer
(100 mM Tris-HCl and 500 mM KCl), 5 µl of
MgCl2 (25 mM), 1 µl of dTNPs (25 mM), 1 µl of outer upstream primers for IRK1-3 (10 mM), 1 µl of outer downstream primers (10 mM), 19.5 µl of autoclaved water, and 0.5 µl of
Taq polymerase (5000 U/ml). The thermal cycling program for
first-round PCR was 94°C for 1.5 min, 54°C for 1.5 min, and 72°C
for 3 min for 35 cycles. For second-round PCR, 2 µl of the
first-round PCR solution was added to three separate thin-walled PCR
tubes containing 5 µl of 10× PCR buffer (100 mM Tris-HCl
and 500 mM KCl), 5 µl of MgCl2 (25 mM), 1 µl of dNTPs (25 mM), 2.5 µl of inner
upstream primer for IRK1, IRK2, or IRK3 (20 mM), 2.5 µl
of inner downstream primer (20 mM), 31.5 µl of autoclaved
water, and 0.5 µl of Taq polymerase (5000 U/ml). The thermal cycling program for peptide amplification was 94°C for 1 min,
59°C for 1 min, and 72°C for 1.5 min for 45 cycles. PCR products
were separated by electrophoresis in 1.5% agarose gels and visualized
by staining with ethidium bromide. Typical amplicons from single NAcc
neurons were sequenced with a dye termination procedure by the Center
for Biotechnology at St. Jude hospital (Memphis, TN) and found to match
published IRK and peptide sequences.
Negative controls for extraneous and genomic DNA contamination were run
during each experiment. To verify genomic DNA was not being amplified,
a single neuron was aspirated and processed using the protocols
described above, except reverse transcriptase was omitted. To verify
that working solutions were DNA-free, water was used as an RT-PCR
template. Consistently, these controls produced the expected results.
Positive controls were also performed during each experiment. cDNA
generated from whole NAcc tissue was used as a PCR template, resulting
in consistent amplification of peptide and IRK sequences.
To generate tissue cDNA, the NAcc was dissected from 400 µm coronal
slices and homogenized in Trizol reagent (1 ml/50-100 mg of tissue)
(Life Technologies). After a 5 min incubation at room temperature, 200 µl of chloroform was added (per milliliter of Trizol), and the tube
was shaken vigorously and incubated at room temperature for another
2-3 min. The solution was then centrifuged at 12,000 rpm for 15 min at
4°C. The aqueous phase was transferred to another 0.5 ml Eppendorf
tube containing 500 µl of isopropyl alcohol (per milliliter of
Trizol), and the tube was shaken and incubated at room temperature for
10 min. Afterward the solution was centrifuged at 12,000 rpm for 10 min
at 4°C. The supernate was then discarded, and 1 ml of 75% ethanol
(per milliliter of Trizol) was added. The tube was shaken and then
centrifuged at 7500 rpm for 5 min at 4°C. The ethanol was removed,
and the pellet was allowed to air dry. RNA was redissolved in 200 µl
of DEPC-treated water. The
A260/A280 ratio
was the expected 1.6-1.8 with a yield of ~0.5 µg/µl. Two
micrograms of RNA were added to a tube containing 2 µl of 10× DNase
I reaction buffer, 1 µl of DNase I (1 U/ml), and DEPC-treated water
for a final volume of 20 µl. The solution was incubated at room
temperature for 15 min. Afterward, 2 ml of EDTA (25 mM) was
added, and the tube was incubated at 65°C for 10 min. The RNA
generated by this procedure was then reverse-transcribed using the
methods described above.
The PCR primers were developed from GenBank sequences using OLIGO
software (National Biosciences, Plymouth, MN). Primers were synthesized
by Life Technologies. The primers for enkephalin and SP cDNA have been
published previously (Surmeier et al., 1996 ). Primers for IRK 1-3
subunits were designed for use in both mouse and rat, although only
data from rat are described here. Outer degenerate primers were used
for the first-round PCR. The upper primers were 5'-CGC TTT GTG AAG AAA
GAT GGT C-3' (nucleotides 136-157 for IRK 1) and 5'-GCT TYG TCA AGA
AGA ACG GYC A-3' (nucleotides 197-218 for IRK 2 and 59-80 for IRK 3),
and the lower primers were 5'-ATC TCC GAY TCY CGY CTK WAG G-3'
(nucleotides 1258-1280 for IRK 1 and 1322-1343 for IRK 2) and 5'-ATG
GCA GAC TCC CTG CGG TAA G-3' (nucleotides 1316-1337 for IRK 3). The
inner primers for IRK 1 cDNA [GenBank accession numbers X73052 and
L48490 (Kubo et al., 1993 ; Wischmeyer et al., 1995 )] were 5'-AAG CAG GAC ATT GAC AAT GCA GAC-3' (nucleotides 850-874) and 5'-AGG TGA GTC
TGT GCT TGT GCT CT-3' (nucleotides 1186-1209), yielding a predicted
PCR product of 359 bp. The inner primers for IRK 2 cDNA [GenBank
accession numbers X80417 and X78461 (Koyama et al., 1994 ; Takahashi et
al., 1994 )] were 5'-ATC ATC TTC TGG GTC ATT GCT GTC-3' (nucleotides
361-384) and 5'-CGT CTC GAG GTC CTG ACG GCT AAT-3' (nucleotides
910-933), yielding a predicted PCR product of 572 bp. The inner
primers for IRK 3 cDNA [GenBank accession numbers S71382, U11075, and
X83580 (Bond et al., 1994 ; Lesage et al., 1994 ; Morishige et al.,
1994 )] were 5'-AAG GAG GAG CTG GAG TCA GAG GA-3' (nucleotides
826-848) and 5'-ACT CAA GCA TCC GGA TAA TGC CTG-3' (nucleotides
1232-1256), yielding a predicted PCR product of 430 bp.
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RESULTS |
Isolation of IRK currents
Our initial obstacle in the characterization of currents
attributable to IRK channels was to identify a voltage range in which they could be studied in isolation. In heterologous expression systems,
recordings of IRK currents are typically made in isotonic K+ solutions by holding the membrane potential near
0 mV (EK) and stepping to hyperpolarized
potentials (Morishige et al., 1994 ; Taglialatela et al., 1994 ).
Attempts to use similar protocols in NAcc neurons were unsuccessful
because hyperpolarizing steps evoked large tail currents attributable
to depolarization-activated K+ channels (Ruppersberg
et al., 1991 ; Sanguinetti et al., 1995 ; Trudeau et al., 1995 ; Miller
and Aldrich, 1996 ). To identify a voltage range in which a contribution
from these channels could be minimized, the activation and inactivation
properties of these conductances were characterized. As previously
described in dorsal striatal neurons (Nisenbaum and Wilson, 1995 ;
Nisenbaum et al., 1996 ), NAcc neurons contain several A-type and
delayed rectifier channels based on 4-aminopyridine and
tetraethylammonium sensitivity (data not shown). Activation of
voltage-gated K+ channels began at approximately
50 mV (n = 14; data not shown). Therefore, voltage
clamping an NAcc neuron at 50 mV and stepping to more hyperpolarized
potentials was predicted not to evoke substantial current
from voltage-gated K+ channels, because they were
already deactivated. This conclusion was consistent with
pharmacological experiments designed to isolate IRK currents. Low
millimolar concentrations of Cs+ are known to block
inwardly rectifying K+ channels (Hille, 1992 ). As
shown in Figure 1, A and
B, Cs+ (1 mM) preferentially
blocked inward currents evoked by hyperpolarizing voltage steps,
leaving currents evoked by depolarizing steps relatively intact.
Isolation of the Cs+-sensitive currents by
subtraction (Fig. 1C) yielded relatively persistent currents
with a strongly rectifying current-voltage relationship (Fig.
1D).

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Figure 1.
Cs+ blocks inwardly rectifying
K+ currents in NAcc neurons. A, A
series of voltage steps ( 30 to 120 mV in 10 mV increments) from
50 mV (EK) produces an inwardly
rectifying K+ current. The asterisk indicates the
beginning of outward rectification at 30 mV, predicted by the
I-V relationship of voltage-gated K+
currents. B, Addition of 1 mM
Cs+ to the extracellular recording solution
preferentially eliminated the inward component of the current.
C, The Cs+-sensitive current
(subtraction of the traces in A from B)
isolates the inwardly rectifying K+ current.
D, Current-voltage relationship of the inwardly
rectifying K+ current (measured at the
arrow in C).
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To provide additional verification that holding at 50 mV allowed IRK
currents to be isolated, the Cs+-sensitive currents
at three holding potentials were compared. In these experiments,
voltage ramps rather than steps were used to rapidly get a picture of
the current-voltage relationship. As shown in Figure
2A,
Cs+ preferentially blocked inward currents at
negative membrane potentials. Isolation of the
Cs+-sensitive currents by subtraction revealed
strong inward rectification (Fig. 2B). These data are
equivalent to those obtained with voltage steps as shown by the
superposition of the ramp currents and those obtained from steps (Fig.
2B, plotted as open circles at the time points corresponding to the step voltage). As shown in Figure 2C, holding at 50 or 80 mV yielded very similar
Cs+-sensitive currents, whereas holding at 0 mV gave
rise to a tail current (n = 4). The equivalence of the
evoked currents when holding at 50 and 80 mV argues that
inactivated channels that have closed activation gates do not go
through an open state before deinactivating and, as a consequence, do
not complicate the interpretation of currents evoked by hyperpolarizing
voltage steps. Last, to eliminate the possibility that
Ca2+-dependent currents were responsible for the
observed currents, cells were examined with
Ca2+-free external solutions (n = 6). As shown in Figure 2D, this condition had little
or no effect on the appearance of Cs+-sensitive
inward currents.

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Figure 2.
Holding at or below 50 mV minimizes deactivating
tail currents. A, A depolarizing voltage ramp to 30 mV
after a brief (16 msec) step to 120 mV from a holding potential of
50 mV produces an inwardly rectifying K+ current.
The current is sensitive to 1 mM Cs+.
B, Subtraction of the traces in A
isolates the inward rectifier. The Cs+-sensitive
current when using ramp protocols is comparable to the current measured
with steps (the currents observed with a series of voltage steps are
displayed as overlaid circles). C,
Holding at either 50 or 80 mV produces a similar inwardly
rectifying current, whereas holding at 0 mV produces a tail current.
Similar results were seen in three other cells. The data suggest that
at 80 and 50 mV, voltage-gated K+ currents are
not contributing to the inward current. D, The inwardly
rectifying current is observed after removal of extracellular
Ca2+ and the addition of a intracellular calcium
chealator (5 mM EGTA), suggesting
Ca2+-dependent K+ currents are
also not responsible for this current. Similar results were seen in
five other cells.
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Characterization of IRK currents
The ionic selectivity of the Cs+-sensitive
K+ current was examined by altering the composition
of the extracellular solution. For a K+-selective
channel, alterations of extracellular concentrations of
K+ should shift the reversal potential in a manner
consistent with the Nernst equation. With an internal
[K+] of 140 mM, decreasing
extracellular [K+] from 20 to 7 mM
changes the predicted zero current potential for a
K+-selective channel from 50 to 75 mV;
decreasing extracellular [K+] to 2.6 mM changes the reversal potential to 100 mV. As shown in
Figure 3, A and B,
the observed zero current potentials closely matched those predicted by
the Nernst equation. For 20, 7, and 2.6 mM extracellular
[K+], the zero current potentials were 53.8 ± 2.4 mV (n = 8), 73.0 ± 1.9 mV
(n = 8), and 101.7 ± 1.3 mV (n = 6). Channel selectivity was also determined by extracellular ion
substitution. An example is shown in Figure 3C. Exchanging
extracellular K+ with either Rb+
or Na+ dramatically reduced the current. Summarized
data from six cells are shown in Figure 3D. With a step to
120 mV, the Cs+-sensitive inward current with
extracellular K+ was 198.7 ± 68.5 pA.
Exchanging K+ with Rb+ reduced
the current to 14.6 ± 3.8 pA. The inward current was further
reduced when extracellular K+ was replaced with
Na+ (0.2 ± 0.1 pA). The ratio of peak current
in external K+ to that in external
Rb+
(IRb/IK)
was 0.07, whereas the ratio with external
[Na+]o
(INa/IK)
was 0.001. The ratios are consistent with experiments examining the
inward rectifier in starfish egg (Hagiwara and Takahashi, 1974 ).

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Figure 3.
The inwardly rectifying current is
K+-selective. A, Decreasing
extracellular K+ shifts the zero current potential
of the inward rectifier in a manner consistent with a
K+-selective channel. B, Summarized
data in which the predicted zero current potential is compared with the
observed potential (n 6; mean ± SEM; error
bars are smaller than the circles). C,
Substitution of extracellular K+ with either
Rb+ or Na+ drastically attenuated
the inward current. D, Box plot summary of the inward
current (measured at the time indicated by the arrow in
C) in the presence of 20 mM
K+, Rb+, or
Na+ (n = 6). For selectivity
estimates,
IRb/IK = 0.07, whereas
INa/IK = 0.001, indicating a current highly selective for
K+.
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The dose dependence of the Cs+ block was also
consistent with that reported previously (Hille and Schwarz, 1978 ).
Figure 4A shows an
example in which inward current was measured in the absence and
presence of 10 µM to 10 mM extracellular
Cs+. Difference currents are shown in Figure
4B. Averaged dose-response data (n = 7) were well fit with an isotherm having an IC50
of 32 µM. The slope of the Hill plot for the
Cs+ block was 0.8. Ba2+ also
produced a time-dependent block of the inward current, with maximum
block occurring at 5 mM (n = 4; data not
shown).

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Figure 4.
The block of the inward rectifier by
Cs+ is dose-dependent. A, Increasing
concentrations of Cs+ from 10 µM to 10 mM increased the block of the inward rectifier.
B, Subtraction of the traces in A isolate
the inward rectifier. Maximal block was seen with low millimolar
concentrations of Cs+. Similar results were seen
with Ba2+ (n = 4; data not
shown). C, Summarized dose-response data for
Cs+ block (n = 7; mean ± SEM). The IC50 was 32 µM.
Inset, Hill plot of Cs+ block. Error
bars (±SEM) are smaller than the circles. The slope was
slightly <1 (0.8).
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Although in most cells a hyperpolarizing step to 120 mV from a
holding potential of 50 mV evoked a stable
Cs+-sensitive current, in a subpopulation of neurons
(~40%), a significant proportion of the inwardly rectifying
K+ current appeared to inactivate or exhibit a
time-dependent block (Fig.
5A,B). The current decay in
these neurons had an average time constant of 25.0 ± 2.9 msec
(n = 7). It had been reported previously that
extracellular monovalent cations other than K+ (such
as Na+) produced a time-dependent block of the
inward rectifier (Ohmori, 1978 ; Standen and Stanfield, 1979 ; Lindau and
Fernandez, 1986 ; Gallin and McKinney, 1988 ; Silver and DeCoursey, 1990 ;
Kelly et al., 1992 ). To determine whether the apparent inactivation
could be attributed to Na+ block, currents were
examined in extracellular recording solutions lacking
Na+. Although extracellular Na+
produced a block of the inward current consistent with previous descriptions, the inward rectifier still inactivated in the absence of
extracellular Na+ (n = 6)
(Fig. 5C).

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Figure 5.
The inwardly rectifying K+
current inactivates in a subpopulation of NAcc neurons.
A, In many neurons, a hyperpolarizing step to 120 mV
resulted in an inward current that displayed little inactivation.
B, However, in a subpopulation of cells (~40%), a
significant component of the inwardly rectifying K+
current inactivated. C, The inactivation cannot be
attributed to blockade of IRK channels by extracellular monovalent
cations other than K+, because inactivation was
still observed when these were replaced with sucrose. Similar results
were seen in five other cells. D, The ERG potassium
blocker terfenadine (3 µM) had no effect on the
inactivating inward current, demonstrating the IRK recordings were not
contaminated with other potassium channels. Inset, Box
plot summary of the teranadine effect in 12 neurons. Terfenadine
blocked 3.5 ± 1.1% of the whole-cell inward current.
|
|
Another possibility is that the apparent inactivation
K+ currents were attributable to deactivation of
depolarization-activated K+ channels. Although our
initial experiments argue that A-like K+ channels
were unlikely to have made a significant contribution to these currents
from a holding potential of 50 mV, ERG-class K+
channels may have been missed. These channels inactivate rapidly with
depolarization and produce a prominent tail current after hyperpolarization as channels move from inactivated to open and then
closed states (Sanguinetti et al., 1995 ; Trudeau et al., 1995 ; Spector
et al., 1996 ). Three erg genes have been cloned in the rat, two of
which (erg1 and erg3) are expressed in the brain (Shi et al., 1997 ).
Single-cell RT-PCR examination revealed a robust expression of erg1,
but not erg3, mRNA in every medium spiny neuron profiled
(n = 8; data not shown). Although the ubiquity of erg1
expression was inconsistent with the appearance of inactivation in only
a subset of neurons, pharmacological experiments were performed to
further test this hypothesis. ERG1 channels are sensitive to block by
terfenadine and haloperidol (Suessbrich et al., 1996 , 1997 ). However,
terfenadine (3 µM) blocked only 3.5 ± 1.1% of the
peak inward current (n = 12; Fig. 5D).
Haloperidol (3 µM) was also without effect on the inward
current (n = 5), suggesting ERG1 channels were not
responsible for the apparent inactivation of the inwardly rectifying
potassium current.
Additional experiments were performed to identify factors governing the
inactivation process. Altering EK failed to have
a clear effect on the kinetics of inactivation. In Figure
6A, the currents evoked
by steps to 120 mV in high [K+]
(EK = 50 mV) and low [K+]
(EK = 75 mV) are shown. Scaling the traces to compensate
for differences in driving force revealed the similarity in the closing kinetics (Fig. 6B; n = 5). Similar
results were found when EK was shifted to 30
mV from 50 mV (n = 4; data not shown). On the other
hand, closing kinetics were voltage-dependent. Stronger hyperpolarizations induced more rapid inactivation (n = 8). A comparison of the closing kinetics at 90 and 120 mV in one
neuron is shown in Figure 6C. The inset displays
the Cs+-sensitive current with a step to 120.
Because the onset of Cs+ block is voltage-dependent
( = 13.8 ± 1.3 msec at 120 mV vs 33.9 ± 2.5 msec at
90 mV; n = 4; p < 0.002, paired
t test), unsubtracted currents are provided. Although the
relative extent of channel closing is similar, the kinetics are faster
at 120 mV (Fig. 6D). Recovery from inactivation
occurred in a time-dependent manner with depolarization. As shown in
Figure 6E, holding the membrane potential at 50 mV
for progressively longer durations led to increasing recovery of the
transient part of the current. The recovery process was approximately
exponential with a time constant near 75 msec at 50 mV (Fig.
6F; n = 4).

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Figure 6.
Inactivation of the inward rectifier is dependent
on voltage and not EK. A,
Shifting EK had no effect on inactivation.
Comparison of the inward current in which EK
was either 50 or 75 mV. B, Adjusting for differences
in driving force, the lack of an effect of
EK is more easily resolved. Similar results
were observed in four other cells. C, Inactivation of
the inward rectifier was voltage-dependent. Although the inward current
inactivates at both 90 and 120 mV, stronger hyperpolarizations
produced more rapid inactivation kinetics (n = 8).
Because the onset of Cs+ block is voltage-dependent
(see Results for details) non-Cs+-subtracted traces
are provided. Inset, The
Cs+-sensitive current at 120 mV is provided for
comparative purposes. D, Adjusting for driving force,
the differences in inactivation kinetics between voltages is more
apparent. E, Recovery from inactivation was rapid,
occurring with progressively longer depolarizations to 50 mV.
F, In this example neuron, the time of recovery could be
fit with a single exponential with a tau equaling 75 msec. Similar
results were seen in three other neurons.
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|
IRK channel expression correlated with peptide expression
The next series of experiments attempted to determine whether the
variation in the apparent inactivation was correlated with expression
of mRNA for IRK channels or other phenotypic features of the cell. To
accomplish this, whole-cell patch-clamp recordings were performed in
conjunction with single-cell RT-PCR. In initial experiments, IRK1-3
and releasable peptide (ENK and SP) mRNAs were amplified from the
entire NAcc using RT-PCR. Amplification conditions were optimized,
yielding single bands of the predicted size for each primer set (Fig.
7A). The detection of all
three IRK mRNAs in the NAcc was consistent with previous in
situ hybridization data (Karschin et al., 1996 ).

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Figure 7.
IRK and peptide mRNA expression are correlated in
individual NAcc neurons. A, IRK1-3 PCR products are
detected using cDNA from whole NAcc tissue. ENK and SP peptide products
are also observed. B, IRK1-3 mRNA expression in
individual neurons varied (n = 39). The most common
phenotype expressed IRK2 and IRK3 (n = 13 of 39).
Notice the low percentage of cells displaying detectable levels of all
three subunit mRNAs (n = 3 of 39).
C, Single cells showing the correlation of IRK subunits
with peptide expression. The ENK mRNA-positive neuron
(top) expressed detectable levels of IRK1 and IRK2. On
the other hand, the SP-positive neuron (bottom)
expressed IRK2 and IRK3. D-F, Summarized
data comparing IRK mRNA subunit expression in SP-positive
(n = 7; D) and ENK-positive
(n = 15; E) neurons and neurons
expressing both ENK and SP (n = 5;
F). Coexpression of multiple IRK mRNA subunits
can be deduced by the extent of bar overlap. NAcc neurons typically
expressed IRK2, regardless of peptide expression. However, IRK1
expression was only found in ENK-positive neurons, although IRK3
expression was most often present in SP-positive cells.
|
|
Next, a similar analysis was performed on single NAcc neurons. The IRK
subunits that were detected in individual neurons varied (n = 39). In approximately two-thirds of the neurons,
multiple IRK mRNA transcripts were detected, although the detection of all three subunits in a single neuron was rare (Fig. 7B).
IRK mRNA expression in single neurons was clearly correlated with peptide mRNA expression. Shown in Figure 7C are two examples
of individual neurons differing in peptide and IRK expression. IRK expression summaries are shown in Figure 7D-F for the three
populations of NAcc neurons identified on the basis of peptide mRNA
expression. IRK1 mRNA was not detected in neurons expressing SP mRNA
alone (n = 7). On the other hand, IRK1 was found to be
expressed in approximately half of the neurons expressing only ENK
(n = 15) and nearly all of the neurons coexpressing ENK
and SP (n = 5). There were subtle differences between
the expression of peptide mRNAs between core (n = 10)
and shell (n = 11) regions of the NAcc. The shell
region contained a higher percentage of neurons expressing SP mRNA
alone (36 vs 20%), whereas the core contained a higher percentage of
neurons expressing ENK mRNA alone (60 vs 55%) or ENK and SP (20 vs
9%).
The final set of experiments examined whether inactivation of the
inwardly rectifying current was correlated with mRNA for a particular
IRK channel. Preliminary experiments attempting to directly correlate
IRK expression with the physiological properties of currents failed
because of the time-dependent degradation of cellular mRNA. Low
abundance templates, such as those for IRK subunits, frequently drop
below the detection threshold under these circumstances. Therefore,
those neurons subjected to detailed physiological analysis were only
profiled for SP and ENK mRNAs. These mRNAs are present in high copy
number in medium spiny neurons and, based on the data presented above,
are predictive of IRK gene expression. In neurons expressing ENK and SP
mRNAs, a substantial proportion of the current inactivated (44.8 ± 8.2%; n = 4; Fig. 8A). Neurons expressing
SP alone typically exhibited noninactivating current (only 11.6 ± 6.8% of the current inactivated; n = 5; Fig. 8B), although neurons only expressing ENK exhibited
intermediate levels of inactivation (25.7 ± 5.2%;
n = 8). These differences (Fig. 8C) were
statistically significant (F = 5.27; p < 0.02, ANOVA). Although there were significant differences in the
degree of inactivation in these different cell types, the initial
current amplitudes (measured at the beginning of the negative step)
were not different (F = 0.48; p > 0.05). Interestingly, the relative amount of inactivation found within
a population of cells expressing the same peptide(s) closely matched
the probability of detecting IRK1 mRNA in that neuronal type (Fig.
8D). As a final check of the hypothesis that IRK1
expression was predictive of current inactivation, IRK1 mRNA levels
were examined in a subset of neurons after voltage-clamp recording.
These recordings were kept brief, and the sensitivity of the
amplification step was increased by using nearly all of the cellular
cDNA in the IRK1 PCR reaction. In eight neurons exhibiting inactivating
currents, IRK1 mRNA was found in six of them. IRK1 was not seen in any
of the four cells exhibiting noninactivating currents. These data
confirm the strong correlation between IRK1 mRNA expression and the
presence of current inactivation at hyperpolarized membrane potentials
in NAcc neurons.

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Figure 8.
The inactivating, inwardly rectifying
K+ current is correlated with IRK1 mRNA expression.
A, An enkephalin- and substance P-positive neuron in
which a large proportion of the inwardly rectifying current
inactivated. B, Another neuron in which the inward
rectifier did not inactivate. This cell expressed substance P alone.
C, Box plot summary comparing the proportion of the
whole-cell current that inactivated in different NAcc neurons. Neurons
expressing ENK alone (n = 8) displayed more
inactivation than neurons only expressing SP (n = 5) but less than cells expressing both ENK and SP
(n = 4). D, Comparison between
different NAcc neurons (based on peptide expression) and their
probability of expressing detectable levels of IRK1. Peptide expression
was correlated with both IRK1 mRNA expression and the amount of current
inactivation.
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|
 |
DISCUSSION |
The properties of inwardly rectifying K+
currents are not attributable to depolarization-activated
K+ channels
As described previously (Uchimura et al., 1989 ; Uchimura and
North, 1990 ), rat NAcc projection neurons exhibit inwardly rectifying currents with hyperpolarizing steps when held at moderately negative potentials. The inward current did not appear to be attributable to
deactivation of depolarization-activated or
Ca2+-dependent K+ channels. These
channels were found to make a significant contribution to currents
evoked from more depolarized membrane potentials (greater than 50
mV). From these more depolarized potentials, channels exhibiting N-type
inactivation transiently open as they move from inactivated to
deactivated states and give rise to a tail current (Zagotta et al.,
1990 ; Demo and Yellen, 1991 ; Ruppersberg et al., 1991 ). The strategy
used to eliminate these voltage-gated K+ channels
from contributing to the inward current was to hold at the foot of the
activation curve ( 50 mV). Although a significant proportion of the
voltage-gated K+ channels was in an inactivated
state at this potential, this was most likely caused by C-type
inactivation that is largely independent of activation gating (Iverson
and Rudy, 1990 ; Hoshi et al., 1991 ). Hence, channels that were closed
and inactivated at 50 mV recovered to a closed state with a
hyperpolarizing step to 120 mV without passing through an open
state.
From a holding potential of 50 mV, hyperpolarizing steps or ramps
evoked inwardly rectifying currents with properties similar to those
originating from IRK channels in heterologous expression systems (Kubo
et al., 1993 ; Morishige et al., 1993 ; Wischmeyer et al., 1995 ).
These currents were highly K+-selective, with
reversal potentials shifting as predicted by the Nernst equation with
alterations in extracellular [K+]. The channels
underlying these currents also displayed little permeability to
Rb+ or Na+ and were blocked by
micromolar concentrations of Cs+ or
Ba2+. All of these properties are consistent with
the hypothesis that IRK channels were responsible for the observed
currents.
However, in a substantial fraction of neurons, currents appeared to
inactivate at hyperpolarized potentials. This type of gating has not
been a consistent feature of IRK channels in heterologous expression
systems (Omori et al., 1997 ). Voltage-dependent K+
channels could be the origin of this inactivating current if over a
period of holding at 50 mV, a significant percentage of the
voltage-gated K+ channels transiently open and move
into an N-type inactivation state. However, there are several
observations that argue against this possibility. One is that
depolarization-activated currents were not discernibly different in
neurons displaying the apparent inactivation and those that did not.
Moreover, one would predict that the presence of a significant
population of inactivating channels would have created a
"hook"-shaped current trajectory after hyperpolarization
(Ruppersberg et al., 1991 ; Miller and Aldrich, 1996 ) and a larger
initial peak current. Neither of these predictions were borne out in
the data. Last, the recovery of the inactivating component at 50 mV
was too fast ( , ~75 msec) to be accounted for by the development
of N-type inactivation in A-like K+ channels
(Ruppersberg et al., 1991 ).
Another channel type that exhibits substantially faster inactivation at
relatively hyperpolarized membrane potentials is the ERG channel type
(Sanguinetti et al., 1995 ; Trudeau et al., 1995 ; Spector et al., 1996 ).
These channels contribute to inward rectification in several cell types
by producing a tail current as channels move from inactivated to open
and then closed states (Wymore et al., 1997 ). Although erg1 mRNA was
robustly expressed by medium spiny neurons, its detection was not
correlated with the presence of the inactivating phase of the
hyperpolarization-evoked currents. All medium spiny neurons expressed
erg1 mRNA, whereas the inactivation was only observed in medium spiny
neurons expressing ENK and IRK1 mRNA. Furthermore, the kinetic
characteristics of the observed currents are not consistent with ERG1
channel mediation. In particular, the decay phase of the
hyperpolarization-activated currents had a time constant of ~25 msec
at 120 mV. This is four times faster than would be predicted by the
deactivation rates of ERG1 channels (Wang et al., 1997 ). Similarly, the
recovery time constant of the inactivating phase of our currents was
~75 msec at 50 mV; this is fourfold to fivefold slower than would
be predicted from the inactivation rates of ERG1 channels at similar
potentials (Wang et al., 1997 ). Last, two known blockers of ERG1
channels, terfenadine and haloperidol, failed to significantly reduce
the inactivating phase of the hyperpolarization-evoked currents. Taken together, these observations strongly argue against the hypothesis that
the decay of currents at hyperpolarized membrane potentials is
attributable ERG K+ channels.
The expression of IRK mRNA is correlated with cell type and the
properties of inwardly rectifying K+
currents
The properties of the inwardly rectifying K+
currents were strongly correlated with releasable peptide and IRK
subunit mRNA expression. Neurons possessing noninactivating, inwardly
rectifying K+ currents invariably expressed SP (but
not ENK) mRNA. These neurons also expressed IRK2 and/or IRK3 subunit
mRNA but not IRK1 mRNA. In contrast, neurons with inactivating
rectifier currents typically expressed ENK and IRK1 mRNAs.
It must be noted that the correlation between peptide and IRK subunit
mRNA detection was not perfect. It is our working hypothesis that the
probability of detecting mRNAs using single-cell RT-PCR techniques is
directly related to mRNA abundance. Within a homogeneous population of
neurons, high-abundance mRNAs will be detected frequently, whereas
low-abundance mRNAs will be detected less frequently (despite the fact
that all cells may express both types of mRNA). For example, IRK1 mRNA
was never detected in SP-expressing neurons. This finding argues that
IRK1 mRNA was present at very low levels or absent in this group of
neurons. On the other hand, IRK1 mRNA was detected in approximately
half of the neurons expressing ENK mRNA. Our interpretation of these
results is not that half of the ENK neurons express IRK1 and the other
half do not. Rather, IRK1 mRNA is expressed at intermediate levels by
this class of cells, which leads to some variation in detection
probability (Surmeier et al., 1996 ; Song et al., 1998 ; Tkatch et al.,
1998 ). Similarly, because the detection probability of IRK1 mRNA was
higher in neurons coexpressing ENK and SP, our inference is that IRK1
mRNA is present at higher levels of abundance in this group of
neurons.
The strong correlation between IRK1 expression and the apparent
inactivation of currents at negative membrane potentials provides little insight at present into potential underlying mechanisms. It is
well known that positively charged, extracellular cations such as
Na+ produce a time-dependent block of inwardly
rectifying channels (Ohmori, 1978 ; Standen and Stanfield, 1979 ; Lindau
and Fernandez, 1986 ; Gallin and McKinney, 1988 ; Silver and DeCoursey,
1990 ; Kelly et al., 1992 ). Our results are consistent with these
observations. However, inactivation was still present in the absence of
Na+ or other monovalent cations other than
K+. Therefore, the inactivation cannot be completely
explained by blocking impermeant monovalent cations. This conclusion is
consistent with the independence of inactivation kinetics on external
[K+] or current amplitude. This fact also argues
against a model in which another ion, such as Mg2+,
might act as a blocking particle. The kinetics of inactivation were,
however, voltage-dependent, increasing with greater hyperpolarization. In heterologous expression systems, IRK1 channels have been found to
exhibit a voltage-dependent inactivation after removal of extracellular Na+ (Stanfield et al., 1994a ; Taglialatela et al.,
1995 ), although the inactivation is less pronounced in some
preparations (Kubo et al., 1993 ; Morishige et al., 1993 ; Wischmeyer et
al., 1995 ; Omori et al., 1997 ). Additional studies will be necessary to
establish whether IRK1 subunits are the principal determinants of this
behavior in NAcc neurons.
Functional significance
These data suggest that there are significant differences in the
way intrinsic conductances regulate the activity of NAcc projection
neurons. As in dorsal medium spiny neurons (Wilson, 1994 ), NAcc neurons
move between quiescent, hyperpolarized states and depolarized, active
states (O'Donnell and Grace, 1995 ). The transition between these
states is driven by extrinsic excitatory synaptic input. However,
intrinsic conductances play an important role in determining the
efficacy of this input (Wilson and Kawaguchi, 1996 ). In the quiescent
state, the inwardly rectifying IRK channels are the principal
determinants of input resistance. These conductances tend to stabilize
the membrane close to EK, opposing
excitatory inputs. As a consequence, alterations in the magnitude of
this conductance can have a significant impact on the response to
excitatory inputs (Wilson and Kawaguchi, 1996 ). Our results suggest
that in ENK and ENK/SP neurons, prolonged sojourns in the quiescent state will be opposed by progressive inactivation of IRK channels, effectively lessening the magnitude of the excitatory input required to
produce a state transition. On the other hand, there should be no such
tendency in SP neurons. In agreement with this hypothesis, neurons in
the SP-rich shell region have been reported to be less excitable than
neurons in the ENK-rich core region (O'Donnell and Grace, 1993 ).
 |
FOOTNOTES |
Received May 15, 1998; accepted June 9, 1998.
The work was supported by United States Public Health Service Grants
NS-34696 and MH-40899 (D.J.S.) and NS-10028 (P.G.M.). We thank Drs.
Richard Aldrich and Bertil Hille for their helpful comments.
Correspondence should be addressed to Dr. D. James Surmeier, Department
of Physiology/Northwestern University Institute for Neuroscience, Northwestern University Medical School, Searle
5-474, 320 East Superior Street, Chicago, IL 60611.
Dr. Mermelstein's present address: Department of Molecular and
Cellular Physiology, Beckman Center for Molecular and Genetic Medicine,
Stanford University School of Medicine, Stanford, CA 94305.
Dr. Song's present address: Division of Biophysical Engineering, Osaka
University, Toyonaka, Osaka 560 Japan.
Dr. Yan's present address: Department of Cellular and Molecular
Neuroscience, Rockefeller University, 1230 York Avenue, New York, NY
10021.
 |
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