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The Journal of Neuroscience, February 1, 2000, 20(3):929-936
Somatostatin Modulates Voltage-Gated K+ and
Ca2+ Currents in Rod and Cone Photoreceptors of the
Salamander Retina
Abram
Akopian1,
Juliette
Johnson3,
Robert
Gabriel1,
Nicholas
Brecha3, 4, 5, and
Paul
Witkovsky1, 2
Departments of 1 Ophthalmology and
2 Physiology and Neuroscience, New York University School
of Medicine, New York, New York 10016, 3 Department of
Neurobiology, University of California, Los Angeles, School of
Medicine, Los Angeles, California 90095, 4 Department of
Medicine, Jules Stein Eye Institute and Center for Ulcer Research and
Education, Division of Digestive Diseases, University of
California, Los Angeles, School of Medicine, Los Angeles, California
90095, and 5 Veterans Administration Medical
Center-West Los Angeles, Los Angeles, California 90073
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ABSTRACT |
We investigated the cellular localization in the salamander retina
of one of the somatostatin [or somatotropin release-inhibiting factor
(SRIF)] receptors, sst2A, and studied the
modulatory action of SRIF on voltage-gated K+ and
Ca2+ currents in rod and cone photoreceptors. SRIF
immunostaining was observed in widely spaced amacrine cells, whose
perikarya are at the border of the inner nuclear layer and inner
plexiform layer. sst2A immunostaining
was seen in the inner segments and terminals of rod and cone
photoreceptors. Additional sst2A immunoreactivity was
expressed by presumed bipolar and amacrine cells. SRIF, at concentrations of 100-500 nM, enhanced a delayed outwardly
rectifying K+ current
(IK) in both rod and cone
photoreceptors. SRIF action was blocked in cells pretreated with
pertussis toxin (PTX) and was substantially reduced by intracellular
GDP S. Voltage-gated L-type Ca2+
currents in rods and cones were differently modulated by SRIF. SRIF
reduced Ca2+ current in rods by 33% but increased
it in cones by 40%, on average. Both effects were mediated via
G-protein activation and blocked by PTX.
Ca2+-imaging experiments supported these results by
showing that 500 nM SRIF reduced a
K+-induced increase in intracellular
Ca2+ in rod photoreceptor terminals but increased it
in those of cones. Our results suggest that SRIF may play a role in the
regulation of glutamate transmitter release from photoreceptors via
modulation of voltage-gated K+ and
Ca2+ currents.
Key words:
somatostatin; retina; Ca2+ channel; K+ channel; G-protein; patch clamp
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INTRODUCTION |
Somatostatin, also called
somatotropin release-inhibiting factor (SRIF), initially was identified
as a hypothalamic peptide but subsequently has been shown to be widely
distributed in the nervous system and in peripheral endocrine organs
(Delfs and Dichter, 1985 ). The cellular actions of SRIF are mediated
via five distinct G-protein-coupled receptors,
sst1-5 (Hoyer et al., 1995 ). In addition, there
are two sst2 isoforms resulting from alternative mRNA splicing (Vanetti et al., 1992 ). SRIF has been shown to modulate K+ and Ca2+
currents in neurons, endocrine cells, and some cell lines. Many classes
of K+ current are reported to be increased
by SRIF, including a K+ leak current
(Schweitzer et al., 1998 ), an inward rectifier (Takano et al.,
1997 ), a delayed rectifier K+
current (Wang et al., 1989 ), and a Ca-activated
K+ current (White et al., 1991 ). The
effect of SRIF on Ca current is inhibitory, and it acts on high
voltage-activated Ca2+ currents of the
L-type (Rosenthal et al., 1988 ) and N-type (Shapiro and Hille, 1993 ).
In axonal terminals, the combined action of SRIF on
K+ and Ca2+
currents has been reported to reduce transmitter release (Katayama and
Hirai, 1989 ; Boehm and Betz, 1997 ).
In the vertebrate retina, SRIF-containing neurons typically are
amacrine (Yamada et al., 1980 ; Li and Lam, 1990 ; Rickman et al.,
1996 ) or interplexiform cells (Smiley and Basinger, 1988 ). SRIF-immunoreactive fibers are predominantly distributed to selected laminae of the inner plexiform layer (IPL). Physiological data on the
role of SRIF in retinal function, however, are scant. Zalutsky and
Miller (1990) reported that SRIF was excitatory to most ganglion cells
tested in rabbit retina, but whether the peptide acted directly on
ganglion cells or via circuitry that is presynaptic to ganglion cells
was not determined. More recently, sst2A
immunostaining was localized to a variety of rat and rabbit retinal
neurons, including bipolar cells and cone photoreceptors (Johnson et
al., 1998 , 2000). The location of sst2A receptors
on photoreceptor terminals suggested a possible role of SRIF in
regulating the release of glutamate, the identified neurotransmitter of
photoreceptors (Marc et al., 1990 ; for review, see Thoreson and
Witkovsky, 1999 ).
In the present study we examined the action of SRIF on rod and cone
photoreceptor terminals in the salamander retina. We showed, by
immunocytochemistry, that in the salamander retina, both rods and cones
express sst2A receptors. Using the whole-cell
patch-clamp technique, we found that SRIF had a differential action on
the high voltage-activated L-type Ca2+
currents of rods and cone inner segments; it reduced the
Ca2+ current of rods but increased that of
cones. In addition, SRIF increased the delayed rectifier
K+ current of rods and cones. These data
suggest that, like dopamine (for review, see Witkovsky and Dearry,
1991 ), SRIF may play a role in governing the balance of information
flow through rod and cone circuits.
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MATERIALS AND METHODS |
Animals. Salamanders (Ambystoma tigrinum)
were obtained from a commercial supplier (Charles Sullivan, Nashville,
TN) and kept at 4°C until used. The handling and maintenance of
animals met the National Institutes of Health guidelines and were
approved by the animal research committees of New York University
School of Medicine and University of California, Los Angeles, School of
Medicine (UCLA).
Tissue preparation for immunohistochemical experiments.
After decapitation, the eyes were removed, the anterior segment was dissected away, and the posterior eyecup containing the retina was
immediately immersed in 4% paraformaldehyde (PFA) in 0.1 M phosphate buffer (PB). The eyecup was fixed for 1 hr at room
temperature and then stored in 25% sucrose in 0.1 M PB at
4°C. Vertical sections of the retina were cut perpendicular to the
vitreal surface with a cryostat at 12-16 µm, mounted onto
gelatin-coated slides, and then air-dried and stored at 20°C.
Cell isolation procedure. The retinas were removed from the
salamander eyecups, exposed to 20 U/mg papain (Worthington, Freehold, NJ) for 30 min, and then washed several times with Ringer's solution [composition (in mM), NaCl 100; KCl 2.5;
CaCl2 1.8; MgCl2 1.0; and
NaHCO3 25, pH 7.4]. The remaining procedures for
cell isolation are identical to those reported previously (Akopian and
Witkovsky, 1996 ). Dissociated cells were plated onto concanavalin A
(Sigma, St. Louis, MO)-coated coverslips. Isolated cells were used in immunocytochemical and Ca2+-imaging
experiments. For immunocytochemical experiments, cells were fixed in
4% PFA for 10 min followed by three washes with 0.1 M PB.
Antibodies. The SRIF antibody and the tyrosine hydroxylase
monoclonal mouse antibody were obtained from Chemicon (Temecula, CA). A
rabbit affinity-purified polyclonal antibody (#9431) directed against
the C terminus of mouse sst2A 361-369 was a
generous gift of Drs. J. Walsh and Helen Wong of UCLA. After a blocking
step in an antibody diluent solution, the primary antibodies were
placed on the tissues or isolated cells for 12-36 hr at 4°C and then washed in 0.1 M PB. The immunoreaction was visualized with
fluorescein-isothiocyanate-coupled goat anti-rabbit antibodies
(American Qualex, La Mirada, CA) or rhodamine donkey anti-mouse
(Jackson ImmunoResearch, West Grove, PA) for 1-2 hr at room
temperature. Sections were coverslipped with a glycerol phosphate or
carbonate buffer containing 2% potassium iodide to retard fading.
The specificity of the sst2A antibody was
evaluated by preadsorbing it with 10 5
M synthetic sst2A peptide, which
completely abolished labeling. In addition, the
sst2A antiserum has been characterized
extensively in a previous study using transfected cell lines, Western
blotting, and immunohistochemistry on tissue sections (Sternini et al., 1997 ).
Image processing. Images were photographed using T-Max 400 or Ektachrome 1600 film. The photographic images were scanned at 2700 dpi with a SprintScan 35/Plus scanner (Polaroid, Cambridge, MA) and
saved as TIFF files. Images were adjusted to the final size,
corrected for contrast and brightness, and labeled using Adobe
Photoshop 5.0 (Adobe Systems, Mountain View, CA). Images were saved at
320 dpi.
Ca2+ imaging. Retinal cells were
isolated, incubated for 10-15 min at room temperature in darkness with
the membrane-permeable fluorescent dye fura-2 AM (Molecular Probes,
Eugene, OR) at a concentration of 5-10 µM, and then
washed in Ringer's solution. Rods and cones were identified by their
characteristic morphology. A coverslip with the cells was transferred
to a stage mounted on a Zeiss 135 Axiovert inverted microscope on which
the cells were superfused with Ringer's solution containing either 50 or 100 mM K+ alone or with
0.2-0.5 µM SRIF. Fluorescence measurements were performed on photoreceptor inner segments with a 40× 1.3 numerical aperture fluar objective, using an Attofluor-imaging
system (Atto Instruments, Rockville, MD). Optical excitation was
accomplished using 340 and 380 nm wavelengths with an emission at 510 nm. The intensity of the fluorescence was minimized to prevent dye
bleaching during experiments. Fluorescence measurements were acquired
using Attofluor Ratiovision software and graphed with Attograph and Sigma Plot. The Attofluor system was calibrated using high (1 µM) and low (Ca-free solution containing 1 mM
EGTA), and the gray scale intensities were adjusted to avoid
saturation. The concentration of fura-2 in the calibration tests was
8.8 µM, similar to the 5-10 µM
concentration of fura-2 AM used in the experiments.
Electrophysiology: slice preparation. The procedures for
obtaining retinal slices were similar to those described by Lukasiewicz et al. (1994) . Briefly, the eyes were enucleated and hemisected, and
the cornea, lens, and iris were removed. The retina was transferred, vitreal side down, to a Millipore filter paper (0.22 µm pore) and
then sectioned manually into 150- to 200-µm-thick slices, which were
mounted in a chamber and superfused at 2 ml/min during the experiment.
Solutions. Whole-cell voltage-clamp recordings of
K+ currents were made using patch
electrodes containing (in mM): K gluconate 100, MgCl2 2, HEPES 10, ATP 2, and GTP 0.1, adjusted
to pH 7.3 with KOH. The bath solution contained (in mM):
NaCl 100, KCl 3, CaCl2 2, MgCl2 2, and HEPES 10, adjusted to pH 7.6 with
NaOH. To isolate Ca2+ currents, the K
gluconate of the intracellular solution was replaced by equimolar CsCl,
while tetraethylammonium (TEA, 20 mM) was added to the bath
solution, replacing an equimolar amount of NaCl. No Ca2+ chelator was included in the
intracellular solution used to record either
K+ or Ca2+
currents. Somatostatin-14 (Bachem Bioscience, King of Prussia, PA) was applied to the bathing solution through the superfusion system
at concentrations of 0.1-0.5 µM. Rods and cones were
identified by their shape and location and by their characteristic
hyperpolarization-activated Ih current. In
some experiments 3 mM CsCl was included in the bath solution to block Ih. To test for a
possible involvement of
Gi/Go proteins in the
somatostatin-induced response, the eyecups were incubated 16-20 hr in
Ringer's solution containing 400 ng/ml pertussis toxin (PTX) at 7°C
in darkness.
Recording procedures. Whole-cell voltage- and current-clamp
recordings were obtained in a conventional way (Hamill et al., 1981 )
using an Axopatch 200B amplifier. Recording pipettes were made from
borosilicate glass tubing (1.2 mm outer diameter; 0.6 mm inner
diameter). Electrode resistance was typically 5-8 M in the bath
solution. After seal rupture the series resistance (10-15 M ) was
compensated (70-80%) by a standard circuit. Whole-cell K+ and Ca2+
currents were typically <1 nA, and the voltage errors resulting from
inadequate compensation were estimated to be at most 3-5 mV. The
average input resistance for rods, estimated from the steady-state
current induced by a 10 mV voltage step from 60 mV, was 1.0 ± 0.1 G (n = 10). Currents were filtered at 1 kHz by a
low-pass Bessel filter and were sampled at 5-10 kHz. The pClamp
software package (Axon Instruments) was used for data acquisition and
analysis. Summary data are presented as means ± SE. The
statistical comparison between groups was made with paired t
tests; the corresponding p values are given in the text. In
voltage-clamp experiments the membrane potential usually was held at
70 mV.
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RESULTS |
Localization of SRIF and the sst2A receptor
SRIF immunostaining was observed in widely spaced amacrine cells,
whose perikarya are at the border of the inner nuclear layer (INL) and
the IPL. Immunolabeled amacrine cell processes were distributed
within two narrow strata: sublamina 1 at the border of the INL and the
IPL and sublamina 5 at the border of the IPL and the ganglion cell
layer (GCL) (Fig. 1a). Because
the morphology of these cells resembled that of the dopaminergic
amacrine cells in tiger salamander (Watt et al., 1988 ), we conducted
double-labeling experiments and determined that SRIF and tyrosine
hydroxylase were found within two distinct cell populations
(data not shown).

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Figure 1.
Retinal distribution of SRIF and somatostatin
sst2A immunoreactivity. a, A
SRIF-immunoreactive amacrine cell body whose processes extend into both
distal and proximal portions of the IPL. b,
sst2A receptor immunoreactivity that is located in both
plexiform layers. Arrows indicate positive staining of
photoreceptor bases. c, Absence of sst2A
immunoreactivity when antibody was preabsorbed with a blocking peptide.
Labels indicate retinal layers: gcl,
ganglion cell layer; inl, inner nuclear layer;
ipl, inner plexiform layer; opl, outer
plexiform layer; and pl, photoreceptor layer. Scale bar:
a-c, 5 µm.
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sst2A receptor immunoreactivity was localized to
both the inner and outer retina, including cell bodies in the
photoreceptor layer, and to processes in both plexiform layers (Fig.
1b). sst2A-immunoreactive photoreceptors with prominent staining throughout the inner segment and
synaptic terminals were observed (Fig. 1b,
arrows). sst2A receptor
immunoreactivity also was expressed by isolated rod and cone
photoreceptors, with strong staining of the inner segments and synaptic
terminals, similar to the staining pattern observed in retinal sections
(data not shown).
sst2A-immunoreactive bipolar and amacrine cell
bodies also were noted in which immunostaining was characterized by a
thin rim of immunoreactivity at, or adjacent to, the plasma membrane. A
dense network of immunostained processes was present in the outer
plexiform layer and in all laminae of the IPL (Fig.
1b). Diffuse immunostaining was observed in the GCL.
Immunostaining was completely eliminated in sections incubated in
antibody that was preadsorbed with 10 5
M sst2A 361-369 (Fig.
1c)
Effect of SRIF on voltage-gated currents in photoreceptors
Characteristics of outward K+ current
in photoreceptors
In the retinal slice preparation, rods were stepped for 50 msec to
depolarizing voltages between 60 and +40 mV in 20 mV increments from
a holding potential of 70 mV (Fig.
2A, left).
Outward current was reliably observed for voltage steps positive to
40 mV. The tail current reversal potential for the outward current
recorded was near 75 mV (data not shown), which is positive to the
equilibrium potential of K+ of 88 mV,
assuming that the intracellular concentration of
K+ was equal to that in the pipette. The
current was blocked in the presence of 20 mM TEA
(data not shown).

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Figure 2.
Effect of SRIF on delayed outward
K+ current (IK) in
rods. A, SRIF increased voltage-activated
K+ current. IK was evoked
by holding cells at 70 mV and applying depolarizing steps from 60
to +40 mV in 20 mV increments in control external solution
(left) and after a 4 min exposure to 0.5 µM SRIF (striped horizontal
bar; right). B,
I-V relationship of IK
obtained from the experiment described in A is
shown. Inset, Somatostatin increased
IK amplitude without substantially changing
the current-voltage relation. , Control; , somatostatin. The
y-axis of the inset is normalized
current. C, CTX reduced outward currents
(left) but did not prevent a somatostatin-induced increase
in IK. D, I-V
relationship of outward current in the presence of CTX ( ), or CTX + somatostatin ( ); n = 3.
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Effect of SRIF on IK
To examine the effect of SRIF receptor activation on
IK, various concentrations of SRIF
from 0.1 to 1 µM were applied to rods. Even at
the holding potential of 70 mV, 0.5 µM SRIF
induced a steady outward current of 16 ± 3 pA (n = 3). This steady current is not reflected in the current-voltage
plots of IK (Fig. 2), because it was
subtracted as a baseline current. Exposure to SRIF progressively
increased the IK evoked by
depolarizing pulses (Fig. 2A, right) compared with
those recorded in control Ringer's solution (Fig. 2A,
left). Partial recovery was observed after a 10-15 min wash in
SRIF-free Ringer's solution (data not shown). The corresponding I-V relationships are illustrated in Figure
2B, showing that an increase in
IK amplitude is not accompanied by a
shift of the current-voltage relation along the voltage axis (Fig.
2B, inset). The threshold dose at which
SRIF increased IK was near 0.1 µM, and the maximum effect was obtained at ~1
µM. In subsequent experiments, we used
concentrations of 0.1-0.5 µM. The mean
increase of IK (at +30 mV voltage
step) induced by 0.5 µM SRIF was 58 ± 13% (n = 20; p < 0.001). The effect
of SRIF was observed after ~1 min of application and reached a
maximum in 2-4 min. A dose-response function for SRIF could not be
obtained on a single cell because of incomplete recovery of
IK, even after a 10-15 min wash in
normal Ringer's solution. A similar enhancement of
IK by SRIF was observed in cones (0.5 µM SRIF; mean increase, 37 ± 8%;
n = 5; p < 0.001). In separate
experiments (n = 3) done in the absence of
Cs+ in the bath solution, we found that
the hyperpolarization-activated current
(Ih) was not affected by SRIF in the same
cells that showed a substantial increase in
IK current (data not shown).
Previous studies indicate that, in salamander photoreceptors,
depolarization activates at least two types of
K+ current: a delayed rectifier and a
Ca2+-dependent
K+ current IK-Ca)
(Barnes and Hille, 1989 ). We used charybdotoxin (CTX; 20 nM) to block IK-Ca
(Knaus et al., 1994 ). This reduced the outward current evoked by a
depolarizing step from 70 to 0 mV (Fig. 2C, mean
reduction, 36 ± 17%; n = 3). Thereafter the slice was superfused with a mixture of charybdotoxin and SRIF (500 nM), resulting in a 49 ± 19% increase in
outward current (Fig. 2C,D), which is the same degree of
enhancement noted without charybdotoxin treatment. Thus, on the basis
of its kinetic and pharmacological characteristics we identify the
SRIF-sensitive outward current (Fig. 2A) as a delayed
rectifier K+ current
(IK).
Previous studies in other preparations have demonstrated that the
action of SRIF on voltage-gated K+ and
Ca2+ currents is sensitive to PTX,
indicating the participation of a PTX-sensitive G-protein (White et
al., 1991 ; Ishibashi and Akaike, 1995 ; Delmas et al., 1998 ). We found
that in slices obtained from eyecups after a 16-20 hr incubation with
PTX (400 ng/ml), IK of either rods or
cones was not augmented by SRIF (Fig.
3a). The mean change of peak
IK by SRIF in PTX-pretreated cells was
8 ± 7% (n = 3; p > 0.1).
There were no significant differences in the I-V
characteristics of the IK current
recorded in control Ringer's solution or in the presence of SRIF (Fig.
3b). The histogram of Figure 3c summarizes the
data obtained in control and PTX-treated slices.

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Figure 3.
Sensitivity to PTX of SRIF effect on
IK. By the use of a voltage protocol similar
to that in Figure 2, a family of IK currents
was recorded in rods pretreated for 16-20 hr with PTX (400 ng/ml).
a, Exposure to 0.5 µM SRIF for 5 min
failed to enhance IK. b,
There was no significant difference in the I-V
relationship of IK recorded in control
solution and in the presence of SRIF. c, The histogram
summarizes the effects of SRIF on IK in
control and PTX-pretreated rods. Numbers in
parentheses in this and subsequent figures are the
sample size.
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Another test of G-protein involvement was the addition to the pipette
solution of GDP S (500 µM), a
compound that blocks the G-protein-mediated effects of
neurotransmitters on neuronal Ca2+
currents (Holtz et al., 1986 ). After rupturing the cell membrane, a
period of 4-5 min was allowed to ensure adequate dialysis with GDP S. Inclusion of
GDP S in the patch pipette substantially abolished the SRIF-induced enhancement of
IK. In many cases we observed even a
slight reduction of IK after exposure
to SRIF. In the experiment illustrated in Figure
4a,
IK was first recorded in control
Ringer's solution and then after a 4 min exposure to 0.5 µM SRIF. The corresponding I-V
relationships are illustrated in Figure 4b. The mean change
of IK induced by exposure to SRIF in
the presence of GDP S was 6 ± 10%
(n = 8; p > 0.1). Figure 4c
summarizes these results, which indicate that a G-protein is implicated
in the cascade underlying a SRIF-induced enhancement of
IK in retinal photoreceptors.

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Figure 4.
The effect of GDP S on SRIF-induced
changes in IK. a,
K+ currents were recorded with a patch pipette
containing 500 µM GDP S in control solution
and after a 5 min exposure to 0.5 µM SRIF.
b, The I-V relationship of
IK obtained from the experiments described
in a indicates that SRIF failed to alter
IK in the presence of GDP S.
c, The histogram summarizes SRIF-induced changes in
IK when the internal solution contained GTP
(open bar) and when GTP was replaced by
GDP S (hatched bar) to
block G-protein activation.
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SRIF reduces Ca2+ current in rods
Ca2+ currents were isolated from
other voltage-gated currents using ion substitution and channel
blockers and were recorded in rods and cones under whole-cell voltage
clamp. From a holding potential of 70 mV, depolarizing pulses of 70 msec duration were applied from 60 to +60 mV, in 10 mV increments,
using 20 mM Ba2+ as the
current carrier. For depolarizing steps positive to 40 mV, rods
responded with a sustained inward current, which was completely blocked
by application of 100 µM Cd
2+, increased by 10 µM BAY K
8644, and reduced in the presence of 50 µM
nifedipine (data not shown), indicating that the
Ca2+ current is mediated by
dihydropyridine-sensitive, L-type Ca channels. In general, the kinetic
and voltage-dependent characteristics of the
Ca2+ current were similar to those
described previously for salamander photoreceptors (Bader et al., 1982 ;
Barnes and Hille, 1989 ). Figure 5a illustrates a
representative experiment in which Ca2+
current was evoked by a depolarizing step from 70 to 0 mV in control
external solution (1), after a 1 min exposure to 0.2 µM SRIF (2), and 2 min after the washout of
drug (3). The SRIF-induced reduction of
Ca2+ current was accompanied by a slowing
of its activation kinetics. In control solution the time constant of
activation was 2.2 ± 0.3 msec (n = 6), increasing
significantly (p < 0.05; n = 6)
to 3.4 ± 0.3 msec in the presence of SRIF. SRIF (0.2 µM) reversibly reduced peak
Ca2+ current in rods by 33 ± 3%
(n = 10; p < 0.05). Figure
5b illustrates the steady-state I-V relationship
of Ca2+ current recorded in control
external solution (open circles), and in the
presence of SRIF (closed circles). It shows that
the reduction of peak current is not accompanied by a significant shift
of the voltage dependence of the calcium current.

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Figure 5.
The inhibitory effect of SRIF on high
voltage-activated Ca2+ currents in rods. The test
solution contained 0 CaCl2 and 20 mM
BaCl2 substituted for equimolar NaCl. a, A
depolarizing step to 0 mV from a holding potential of 70 mV was
applied to record whole-cell Ca2+ current in control
external solution (1), after a 1 min exposure to 0.2 µM SRIF (2), and after a wash (3).
b, The I-V relationship of
Ca2+ currents evoked by depolarizing voltage steps
from 50 to +50 mV in 10 mV increments in the absence
(open circles) and the presence of 0.2 µM SRIF (closed circles) is
shown. c, The time course of SRIF blockade was evaluated
by applying 70 msec depolarizing pulses to a test potential of 0 mV
from a holding potential of 70 mV each 5 sec. The time of SRIF
application is shown by the hatched
horizontal bar. The
numbers correspond to the traces in
a.
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The time course of SRIF blockade was evaluated, using the following
protocol. We applied 70 msec depolarizing pulses to a test potential of
0 mV from a holding potential of 70 mV each 5 sec (Fig.
5c). In other experiments a voltage ramp (from 70 to +50
mV) was applied every 10 sec. After obtaining five to six stable
sequential responses, SRIF-containing solution was perfused into the
bath, and the recordings continued another 2-3 min. Figure 5c illustrates that the actions of SRIF on
Ca2+ current developed relatively rapidly
(<1 min) and complete recovery was observed within a 1-2 min wash in
control external solution, unlike the incomplete recovery of
IK even after a 10-15 min wash.
SRIF enhances Ca2+ current in cones
Surprisingly, we found that in contrast to its inhibitory action
on Ca2+ current in rods, SRIF enhanced
ICa in cones. Figure
6A illustrates an
experiment in which a cone was held at a membrane potential of 70 mV,
and depolarizing pulses were applied from 40 to +40 mV in 10 mV
increments. A family of whole-cell Ca2+
currents was recorded in control Ringer's solution, in the presence of
0.5 µM SRIF and after a wash in control
Ringer's solution. In the presence of SRIF, the peak
Ca2+ current was increased by 40 ± 8% (n = 5; p < 0.005). Figure
6B illustrates the I-V characteristics
that show that SRIF enhanced Ca2+ current
more dramatically at negative voltage steps (e.g., at 30 mV compared
with 0 mV), resulting in a shift of peak
Ca2+ current toward negative potentials.
The data of Figures 5 and 6 are summarized in the histogram of Figure
6C that illustrates that SRIF enhances
ICa in cones but decreases
ICa in rods.

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Figure 6.
Excitatory effects of SRIF on the
Ca2+ current in cones. A, Cones were
held at 70 mV, and depolarizing pulses were applied from 40 to +40
mV in 10 mV steps. Responses were recorded in 20 mM Ba
solution as described for Figure 5. Left, In control Ba
Ringer's solution. Middle, In 0.5 µM
SRIF. Right, After a wash in Ba Ringer's solution.
B, Current-voltage plot of the data in A
is shown. C, A summary of the changes induced in
the peak Ca current of rods and cones by SRIF is shown.
Cntr, Control ( ), wash ( ).
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The SRIF-induced inhibition of ICa is
G-protein coupled
sst2A receptors are coupled to
Gi or Go proteins in
different systems (Law et al., 1991 , 1993 ; Gu and Schonbrunn, 1997 ).
Some forms of G-protein-mediated inhibition of
Ca2+ currents by neuromodulators are
voltage dependent, being relieved by strong depolarizations (Bean,
1989 ; Hille, 1994 ). For example, in hippocampal neurons, the
SRIF-induced inhibition of an N-type Ca2+
current has been shown to be highly sensitive to PTX and to
depolarizing prepulses (Ishibashi and Akaike, 1995 ). To test for the
possible involvement of a G-protein in the SRIF-induced inhibition of
ICa, we performed experiments on
eyecups pretreated with 400 ng/ml PTX. We found that PTX attenuated the
inhibitory action of SRIF on ICa. The
mean inhibition of ICa by somatostatin
in PTX-pretreated rods was 8 ± 2% (n = 3;
p > 0.1), compared with the 33% reduction observed in
untreated rods.
A G-protein-dependent inhibition of
ICa by SRIF may be mediated via an
intracellular second messenger system or by a direct membrane-delimited
mechanism. G-protein-dependent inhibition of ICa has been found to use either
pathway, depending on the neurotransmitter involved (Beech et al.,
1991 ; Shapiro and Hille, 1993 ). We tested whether intracellular
Ca2+ might serve as a second messenger by
changing the pipette solution to one containing 0 Ca2+/10 mM BAPTA.
The mean reduction of ICa by SRIF in
the presence of BAPTA was ~37% (n = 3), the same
degree of inhibition observed in rods not treated with BAPTA (data not
shown). We concluded that SRIF-induced inhibition of
ICa in rods is not mediated via changes in intracellular [Ca2+].
Effect of SRIF on intracellular
Ca2+ accumulation
We used Ca2+-imaging techniques to
examine whether SRIF altered a depolarization-induced elevation of
[Ca2+]i in
isolated photoreceptor synaptic endings. In these experiments, 50-100
mM K+ (substituted for an
equivalent amount of NaCl) was used to depolarize the cells and to
stimulate Ca2+ entry through voltage-gated
Ca2+ channels. Exposure to elevated
[K+]o induced a
sustained increase of
[Ca2+]i in the
synaptic terminals of isolated rods and cones (Fig. 7a,c). This effect was
substantially reduced (~80%) in the presence of nifedipine (50 µM) and completely blocked in the presence of Cd2+ (100 µM),
indicating that elevation of intracellular
[Ca2+] was caused by activation of
voltage-gated L-type Ca2+ channels,
although release of Ca2+ from
intracellular stores may also have contributed to the
Ca2+ signal (Krizaj and Copenhagen, 1998 ).
We found that, in rods, SRIF (0.2-0.5 µM)
significantly reduced the
[Ca2+]i
accumulation induced by high K+ (Fig.
7a). The mean reduction of Ca2+
entry by 0.5 µM somatostatin was 55 ± 18% (n = 5; p < 0.05). In agreement
with electrophysiological results, we noted that in cones, 0.5 µM SRIF enhanced intracellular
Ca2+ accumulation induced by high
K+ (Fig. 7c). The mean increase
of [Ca2+]i by 0.5 µM SRIF in cones was 50 ± 15%
(n = 5; p < 0.05). Figure 7,
b and d, summarizes these data that show that
SRIF differentially affects Ca2+ signals
in rods and cones. In control experiments we observed that two pulses
of 90 mM K+ elicited
approximately equal increases in [Ca]i, when
separated by the same 1-2 min used for the experiments illustrated in
Figure 7 (data not shown). Second, it was found that preexposure to PTX abolished the SRIF-induced increase in
[Ca2+]i in cones
( 4 ± 1%; n = 4; p > 0.1; data
not shown). Those cells that still possessed synaptic terminals after
isolation manifested the most extensive changes in intracellular
Ca2+ induced both by high
K+ and SRIF, indicating that SRIF
receptors and/or Ca2+ channels may be
concentrated in the photoreceptor synaptic terminals (Bader et al.,
1982 ).

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|
Figure 7.
Effects of somatostatin on
K+-induced Ca2+ accumulation in
rods and cones. a, c, KCl (100 mM) was used
to stimulate Ca2+ entry in the absence and the
presence (hatched horizontal
bar) of 0.5 µM somatostatin in rods
(a) and cones (c).
Somatostatin reduced Ca2+ accumulation in rods but
increased it in cones. b, d, Histograms summarize the
somatostatin-induced inhibition of Ca2+ accumulation
in rods (b; n = 5) and its
enhancement in cones (d; n = 5).
Vertical bars show the mean values ± 1 SE.
|
|
 |
DISCUSSION |
Cellular distribution of SRIF-containing neurons and SRIF receptors
in the vertebrate retina
SRIF immunoreactivity has been described in the retinas of a
variety of cold-blooded and homeotherm vertebrates (for review, see
Brecha, 1983 ). The SRIF-containing cells are inner retinal neurons,
typically amacrine or interplexiform cells (Yamada et al., 1980 ; Li et
al., 1986 ; Smiley and Basinger, 1988 ; Rickman et al., 1996 ), with
perikarya located either in the GCL or at the border of the INL and
IPL. SRIF-containing neurons in mammals often are displaced amacrines,
i.e., with cell bodies in the GCL (Engelmann and Peichl, 1996 ; Rickman
et al., 1996 ). The retinal density of SRIF neurons is low [<100 cells
mm 2 (Rickman et al., 1996 )] in most
parts of the retina but may reach a few thousand cells per square
millimeter in restricted retinal regions (Engelmann and Peichl, 1996 ;
Rickman et al., 1996 ). In spite of the low cellular density, SRIF
processes create a continuous network in the IPL. Within the IPL the
distribution of SRIF processes varies; in chicken retina, it is diffuse
(Ishimoto et al., 1986 ), whereas in rabbit and salamander retinas, SRIF
processes extend horizontally in laminae 1 and 5 of the IPL (Rickman et
al., 1996 ) (present report). sst2A receptors, on
the other hand, are found in both the inner and outer retina (Johnson
et al., 1998 , 1999 ) (present report). The wider retinal distribution of
SRIF receptors in relation to SRIF cells and processes indicates that
SRIF reaches some targets by diffusion. Thus in general outline, the
retinal SRIF system resembles closely that of the dopamine system
(Witkovsky and Schutte, 1991 ), a resemblance that is heightened by the
presumption that SRIF will affect synaptic transmission between rod and
cone photoreceptors and second-order retinal neurons, as shown
previously for dopamine (Witkovsky et al., 1988 ).
In the absence of antibodies against other forms of the SRIF receptors,
we cannot conclude with certainty that the SRIF-induced physiological
effects we have described were mediated by the
sst2A receptor, although this is a reasonable
supposition because of the high density of sst2A
receptors on rod and cone terminals. The finding that these effects
were blocked by PTX is not diagnostic, because all forms of SRIF
receptor are reported to act via subtypes of either
Gi or Go proteins (Law et
al., 1991 ; Takano et al., 1997 ), all of which are blocked by PTX.
SRIF-induced modulation of Ca2+ and
K+ currents in photoreceptors
K+ current
Photoreceptors possess a mixture of voltage-dependent
K+ currents, including a delayed
rectifier, IK (Bader et al., 1982 ), a
Ca2+-dependent
K+ current, IK-Ca
(Corey et al., 1984 ), and Ih, a mixed
cation current (Fain et al., 1978 ; Barnes and Hille, 1989 ). Our data indicate that SRIF selectively augments the delayed rectifier K+ current. The enhancement of outward
currents remained in the presence of charybdotoxin that blocks
IK-Ca, and it increased with
depolarizing steps (Fig. 2) at which potentials
Ih is inactivated (Akopian and Witkovsky,
1996 ). Exposure to SRIF also elicited a non-inactivating outward
current that was 16 pA at the holding potential of 70 mV. This steady
current is not attributable to Ih that has
a reversal potential near 30 mV and so would generate an inward
current at 70 mV. If the steady current were a leakage current, it
would add a linear component to the total outward current, whose
magnitude can be estimated by a regression line passing through
EK ( 88 mV) and 16 pA at 70 mV. Because this putative current was not observed (Fig. 2), we conclude that the action
of SRIF on K current is mediated primarily by
IK in salamander rods and cones.
The SRIF-induced steady K+ current would
be expected to hyperpolarize photoreceptors. At the resting potential
of the photoreceptor in darkness ( 40 mV) and with a value of 100 M
resistance to ground for rods in an intact retina (Owen and Copenhagen,
1977 ), photoreceptors will be hyperpolarized 1 mV for each 10 pA of
steady current.
We noted that the SRIF-induced increase in
IK was blocked by PTX and by
GDP S, consistent with the general finding that SRIF acts via PTX-sensitive G-proteins (Law et al., 1991 ; Rens-Domiano and Reisine, 1992 ). Our data agree with the demonstration by Wang et
al. (1989) that in rat neocortical neurons, the enhancement by SRIF of
a delayed rectifier current was antagonized by PTX. Takano et al.
(1997) found that Kir was activated by SRIF via G i 1 or 2 proteins, and Gu and Schonbrunn
(1997) showed that the sst2A receptor complexed
specifically with G i 1-3 proteins, all of
which are PTX-sensitive. Thus our data are consistent with the
hypothesis that they were mediated by the sst2A
receptor that rod and cone photoreceptors express (Fig. 1), but a more
compelling proof would require showing that SRIF receptors other than
the sst2A subtype are absent on salamander photoreceptors.
Ca2+ currents
The Ca2+ currents of salamander rods
and cones have been investigated intensively (Bader et al., 1982 ; Corey
et al., 1984 ; Barnes and Hille, 1989 ; Wilkinson and Barnes, 1996 ). They
are of the L-type (dihydropyridine-sensitive, high voltage-activated,
and nondesensitizing). Studies in several systems show that L-type currents are reduced by SRIF in a rapid and reversible manner (Ikeda
and Schofield, 1989 ; Dryer et al., 1991 ; Shapiro and Hille, 1993 ;
Ishibashi and Akaike, 1995 ). Our data on the fast, reversible inhibition of ICa in rods by SRIF and
the independence of SRIF-induced effects on changes in intracellular
[Ca2+] suggest that the SRIF-induced
inhibition of ICa is mediated by a
membrane-delimited pathway. This possibility is consistent with the
demonstration by Delmas et al. (1998) that a
G unit underlies the inhibition, by
noradrenaline and SRIF, of an N-type Ca2+
current in rat sympathetic neurons.
The finding that the ICa of cone
photoreceptors is enhanced by SRIF is novel. The enhancement consisted
of a shift toward negative voltage of the activation function. This
shift will be functionally important for cones, because their operating
range extends for 20-30 mV negative to the membrane potential of
approximately 40 mV in darkness (for review, see Attwell, 1990 ). The
voltage-clamp records of ICa in cones
are buttressed by the data from Ca2+
imaging that show that SRIF augments the increase in
[Ca2+]i. It is
possible that the differential action of SRIF on rod and cone calcium
currents indicate a difference in the underlying Ca channel. Wilkinson
and Barnes (1996) classified the cone L-Ca channel as the D subtype on
the basis of its pharmacological profile, but we are unaware of a
comparable study on the rod Ca channel.
Significance for retinal function of SRIF-induced alterations in
photoreceptor K+ and Ca2+
currents
The photoreceptor synapse is unusual in that rods and cones
release glutamate tonically in darkness. Light, by hyperpolarizing the
photoreceptor, reduces the rate of glutamate release (for review, see
Attwell, 1990 ). Because glutamate release by photoreceptors is a
Ca2+-dependent process, it requires a
sustained, voltage-dependent Ca2+ current,
in accord with the demonstration that rods and cones use an L-type Ca
current to mediate transmitter release (Rieke and Schwartz, 1996 ;
Schmitz and Witkovsky, 1997 ; Witkovsky et al., 1997 ). A growing number
of studies document that transmitter release from photoreceptor
terminals is subject to multiple sources of neuromodulation. These
include pH (Barnes et al., 1993 ), possibly related to GABA release by
horizontal cells (Verweij et al., 1996 ), dopamine (Stella and Thoreson,
1998 ), and Ca release from intracellular stores (Krizaj et al.,
1999 ).
SRIF will contribute to the overall modulation by downregulating
glutamate release from rods via two mechanisms. The steady outward
K+ current will hyperpolarize the rod.
Even a small (1-2 mV) hyperpolarization might be important, because of
the change of slope of the Ca2+ current
activation function that occurs near the 40 mV resting potential of
the rod in darkness (Rieke and Schwartz, 1996 ; Witkovsky et al., 1997 ).
Second, by further reducing ICa
directly, glutamate release by rods will be attenuated.
The situation for cones is complex in that the shift toward negative
voltages of the Ca2+ current-voltage
function by SRIF will tend to be counterbalanced by any
hyperpolarization resulting from a SRIF-induced increase in
IK. Thus a good test of the net action
of SRIF on photoreceptor signaling will be to examine rod and cone
inputs to the second-order retinal neurons and horizontal and bipolar
cells. In amphibian retinas these second-order neurons receive a mixed
input from rods and cones (Hare et al., 1986 ). On the basis of the
findings of the present study, one would expect SRIF to reduce rod
input and increase cone input, just as has been reported for the action of dopamine on amphibian horizontal cells (Witkovsky et al., 1988 ).
 |
FOOTNOTES |
Received Oct. 7, 1999; revised Nov. 12, 1999; accepted Nov. 15, 1999.
This work was supported by National Institutes of Health Grants EY
03570 to P.W., EY 07026 to J.J, and EY 04067 to N.B. and by a Veterans
Administration Career Scientist award to N.B. Additional support
came from the Hoffritz Foundation and an unrestricted grant from
Research to Prevent Blindness to the Department Ophthalmology, New York
University School of Medicine.
Correspondence should be addressed to Dr. Abram Akopian, New York
University School of Medicine, 550 First Avenue, New York, NY 10016. E-mail: aa3{at}is4.nyu.edu.
 |
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1410 - 1415.
[Abstract]
[Full Text]
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A. Vasilaki, T. Papadaki, G. Notas, G. Kolios, N. Mastrodimou, D. Hoyer, M. Tsilimbaris, E. Kouroumalis, I. Pallikaris, and K. Thermos
Effect of Somatostatin on Nitric Oxide Production in Human Retinal Pigment Epithelium Cell Cultures
Invest. Ophthalmol. Vis. Sci.,
May 1, 2004;
45(5):
1499 - 1506.
[Abstract]
[Full Text]
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J. E. McRory, J. Hamid, C. J. Doering, E. Garcia, R. Parker, K. Hamming, L. Chen, M. Hildebrand, A. M. Beedle, L. Feldcamp, et al.
The CACNA1F Gene Encodes an L-Type Calcium Channel with Unique Biophysical Properties and Tissue Distribution
J. Neurosci.,
February 18, 2004;
24(7):
1707 - 1718.
[Abstract]
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S. L. Stella Jr., E. J. Bryson, L. Cadetti, and W. B. Thoreson
Endogenous Adenosine Reduces Glutamatergic Output From Rods Through Activation of A2-Like Adenosine Receptors
J Neurophysiol,
July 1, 2003;
90(1):
165 - 174.
[Abstract]
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A. Straiker and J. M. Sullivan
Cannabinoid Receptor Activation Differentially Modulates Ion Channels in Photoreceptors of the Tiger Salamander
J Neurophysiol,
May 1, 2003;
89(5):
2647 - 2654.
[Abstract]
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R. Simo, A. Lecube, L. Sararols, J. Garcia-Arumi, R. M. Segura, R. Casamitjana, and C. Hernandez
Deficit of Somatostatin-Like Immunoreactivity in the Vitreous Fluid of Diabetic Patients: Possible role in the development of proliferative diabetic retinopathy
Diabetes Care,
December 1, 2002;
25(12):
2282 - 2286.
[Abstract]
[Full Text]
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E. A. Schwartz
Transport-Mediated Synapses in the Retina
Physiol Rev,
October 1, 2002;
82(4):
875 - 891.
[Abstract]
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N. Zhang and E. Townes-Anderson
Regulation of Structural Plasticity by Different Channel Types in Rod and Cone Photoreceptors
J. Neurosci.,
August 15, 2002;
22(16):
7065 - 7079.
[Abstract]
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Q.-Q. Sun, J. R. Huguenard, and D. A. Prince
Somatostatin Inhibits Thalamic Network Oscillations In Vitro: Actions on the GABAergic Neurons of the Reticular Nucleus
J. Neurosci.,
July 1, 2002;
22(13):
5374 - 5386.
[Abstract]
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X.-B. Gao and A. N van den Pol
Melanin-concentrating hormone depresses L-, N-, and P/Q-type voltage-dependent calcium channels in rat lateral hypothalamic neurons
J. Physiol.,
July 1, 2002;
542(1):
273 - 286.
[Abstract]
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S. L. Stella Jr., E. J. Bryson, and W. B. Thoreson
A2 Adenosine Receptors Inhibit Calcium Influx Through L-Type Calcium Channels in Rod Photoreceptors of the Salamander Retina
J Neurophysiol,
January 1, 2002;
87(1):
351 - 360.
[Abstract]
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H. Hirasawa, R. Shiells, and M. Yamada
A Metabotropic Glutamate Receptor Regulates Transmitter Release from Cone Presynaptic Terminals in Carp Retinal Slices
J. Gen. Physiol.,
January 1, 2002;
119(1):
55 - 68.
[Abstract]
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A. Vasilaki, R. Gardette, J. Epelbaum, and K. Thermos
NADPH-Diaphorase Colocalization with Somatostatin Receptor Subtypes sst2A and sst2B in the Retina
Invest. Ophthalmol. Vis. Sci.,
June 1, 2001;
42(7):
1600 - 1609.
[Abstract]
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R. Cristiani, G. Fontanesi, G. Casini, C. Petrucci, C. Viollet, and P. Bagnoli
Expression of Somatostatin Subtype 1 Receptor in the Rabbit Retina
Invest. Ophthalmol. Vis. Sci.,
September 1, 2000;
41(10):
3191 - 3199.
[Abstract]
[Full Text]
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T. Ivanina, Y. Blumenstein, E. Shistik, R. Barzilai, and N. Dascal
Modulation of L-type Ca2+ Channels by Gbeta gamma and Calmodulin via Interactions with N and C Termini of alpha 1C
J. Biol. Chem.,
December 15, 2000;
275(51):
39846 - 39854.
[Abstract]
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