 |
Previous Article | Next Article 
The Journal of Neuroscience, August 15, 1998, 18(16):6501-6511
Expression of Different Types of Inward Rectifier Currents
Confers Specificity of Light and Dark Responses in Type A and B
Photoreceptors of Hermissenda
Ebenezer N.
Yamoah1, 2,
Louis
Matzel3, and
Terry
Crow2
1 Department of Cell Biology, Neurobiology, and
Anatomy, University of Cincinnati School of Medicine,
Cincinnati, Ohio 45267, and Marine Biological Laboratory, Woods Hole,
Massachusetts 02543, 2 Department of Neurobiology and
Anatomy, University of Texas Medical School, Houston, Texas 77030, and
3 Rutgers University, Department of Psychology, Busch
Campus, New Brunswick, New Jersey 08903
 |
ABSTRACT |
Each eye of the mollusc Hermissenda consists of five
photoreceptors, two type A and three type B cells. Type A cells are
quiescent, whereas B cells are spontaneously active in the dark.
Differences in the intrinsic membrane properties of type A and B
photoreceptors were studied using voltage- and current-clamp
techniques. The current density of a Ni2+-sensitive,
low-voltage activated Ca2+ current was similar in
the two cell types. However, type B cells express an inward rectifier
current (Ih) that has different permeation and pharmacological properties from the inward rectifier current in
type A cells. The current in the B cells was time-dependent and was
blocked by Cs+. Na+ and
K+ were the charge carriers for
Ih. The inward rectifier current in A
cells (IK1) was time-independent, was
selectively permeable to K+, and was blocked by
Ba2+. Ni2+ reduced the
spontaneous spike activities of type A and B cells, whereas
Cs+ produced membrane hyperpolarization and reduced
the spike activities of dark-adapted B cells. The application of both
Cs+ and Ni2+ completely blocked
dark-adapted spontaneous activities of B cells. Moreover,
Ba2+ increased the excitability of type A cells but
not B cells. Hence, differential expression of the two distinct inward
rectifiers found in type A and B cells contributes to differences in
their intrinsic membrane properties. Because changes in the
excitability of the two cell types are correlates of conditioning in
Hermissenda, modulation of these underlying currents may
play a major role during conditioning-induced plasticity.
Key words:
Hermissenda; photoreceptors; calcium currents; inward rectifiers; membrane oscillation; neuronal plasticity
 |
INTRODUCTION |
Alteration of membrane excitability
of neurons is an example of cellular plasticity associated with
learning in nervous systems of vertebrates and invertebrates
(Abrams, 1985 ; Jester et al., 1995 ). The mollusc
Hermissenda has a simple eye that serves not only as a site
for photo transduction but also as a locus for cellular plasticity
(Crow, 1988 ; Farley et al., 1990 ; Alkon et al., 1992 ; Matzel and
Rogers, 1993 ). The eye consists of five photoreceptors that are
classified as type A and B cells, based on anatomical and
electrophysiological differences (Alkon and Fuortes, 1972 ).
Classical conditioning of Hermissenda produces enhanced
excitability of the B photoreceptors that is expressed as an increase
in input resistance (Crow and Alkon, 1980 ; Crow, 1988 ; Matzel and
Rogers, 1993 ) and a reduction of both the transient K+ current (IA) and the
calcium-activated K+ current
(IK,Ca) (Alkon, 1979 ; Alkon et al.,
1985 ). In contrast, type A cells undergo a reduction in dark-adapted
input resistance (Farley and Alkon, 1982 ; Farley et al., 1990 ).
Differences between the two cell types are not only expressed in
conditioned animals but can be seen in naïve animals as
well.
Type A cells are quiescent in the dark, and type B cells undergo
rhythmic spike activities in darkness. Light elicits depolarizing generator potentials in both cell types. At the end of a light stimulus, the A cells remain electrically silent after a few seconds of
dark adaptation, but the B cells remain tonically active (Alkon and
Fuortes, 1972 ). The underlying mechanisms for the different electrical properties between the two cell types are unknown. Synaptic
inhibition between the photoreceptors has been used, in part, to
explain differences in the electrical properties of A and B cells
(Alkon and Fuortes, 1972 ). However, such an explanation may not suffice
to explain the properties of the two cell types. For instance, the A
cells are relatively hyperpolarized in the dark-adapted state, whereas
the B cells are more depolarized and remain spontaneously active; yet
the inhibitory inputs at the B cells are stronger than are those at the
A cells (Alkon and Fuortes, 1972 ).
Differential expression of different ionic currents in type A and B
cells may contribute to the apparent electrophysiological differences
between the two cell types. To examine this possibility, we studied
ionic currents and electrical properties of the photoreceptors using
the whole-cell voltage-clamp technique and conventional intracellular
recordings. The properties of three distinct inward currents are
presented. Type A and B cells express a transient Ca2+ current (ICat) at
similar densities. But the A cells predominantly express a
time-independent K+-permeable inward rectifier
current (IK1), which tends to
hyperpolarize the cells and prevent tonic activity in darkness. In
contrast, type B cells exhibit a time-dependent
Na+/K+-permeable inward rectifier
current (Ih).
Ih promotes membrane depolarization. The
combined effects of ICat and
Ih support spontaneous activities of type
B photoreceptors in the dark.
 |
MATERIALS AND METHODS |
Cell isolation. Specimens of Hermissenda
were obtained from Sea Life Supply (Sand City, CA) and housed in
artificial seawater (ASW) tanks at 14-16°C. Animals were fed
scallops daily and maintained on a 12 hr light/dark cycle. The
photoreceptors of Hermissenda were freshly isolated from the
nervous system, and the type A and B cells were identified according to
methods described previously (Yamoah and Crow, 1994 , 1996 ). The nervous
systems were dissected and incubated in ASW (composition in
mM is 420 NaCl, 10 KCl, 10 CaCl2, 22.9 MgCl2, 25.5 MgSO4, and 15 HEPES, buffered to pH 7.8 with 1N NaOH) at 4°C for 10 min and
then were exposed to an enzyme solution made of 7 mg/ml dispase grade
II (Boehringer Mannheim, Mannheim, Germany) and 1 mg/ml protease
(Sigma, St. Louis, MO) in ASW for 10 min at 4°C. The preparation was
transferred to room temperature (20°C) for another 7-10 min and then
was washed several times with ASW at 4°C. After incubation for 20 min
at 4°C, the eyes were isolated. Type A and B cells were identified on
the basis of their position relative to the lens and the optic nerve. Therefore, isolated eyes without a lens and the stump of the optic nerve were discarded. We did not further classify isolated
photoreceptors as either medial or lateral (Alkon and Fuortes,
1972 ). Using a fire-polished pipette, we isolated individual
photoreceptors, plated them into 35 mm sterile culture dishes (Falcon,
1008; Fisher Scientific, Houston, TX) containing 2 ml of
gentamycin-treated ASW (50 mg/ml), and stored the dishes at 4°C
(Yamoah et al., 1994 ). The solution was aspirated and replaced with
recording medium 5 min before voltage-clamp experiments were
performed.
Voltage clamp. Macroscopic whole-cell inward rectifier and
calcium currents were recorded at room temperature (20°C). All chemicals were obtained from Sigma unless otherwise noted. The compositions of the bath solutions for recording calcium and inward rectifier currents were as follows (in mM): for the
Ca2+ current, 400 tetraethylammonium (TEA)
acetate or 400 N-methyl-D-glucamine (NMG)
and 200/250 TEA-chloride, 10 CaCl2, 5 MgSO4, 5 4-aminopyridine, and 15 HEPES, pH
7.7, titrated with TEA-hydroxide (TEA-OH); and for the inward rectifier
currents, 200 NMG, 300 choline chloride, 2-50 KCl, 0-2
CaCl2, 50 MgSO4, and 15 HEPES, pH
7.7 (with KOH). Experimental agents were applied by bath superfusion at
a rate of 1-1.5 ml/min using gravity and an aquarium pump for suction (Penn-Pax Plastic, Garden City, NY) in a 1.2 ml experimental chamber. The pipette solution contained (in mM): for the
Ca2+ current, 300 NMG, 200 CsCl, 50 HEPES, 2-5
EGTA, 20 NaCl, 2 MgSO4, 20 TEA, 5 MgATP, 1 Na2GTP, and 10 reduced glutathione, pH 7.4 (with TEA-OH);
and for the inward rectifier currents, 0-20 NaCl, 0-2
MgSO4, 50 HEPES, 0.1-5 EGTA, 50-250 KCl, 250-350
NMG, 5 MgATP, 1 Na2GTP, and 10 reduced glutathione, pH 7.4 (with HCl).
Voltage clamp in the whole-cell configuration (Hamill et al., 1981 ) was
used to measure the inward rectifier and Ca2+
currents using the Axopatch 200A amplifier (Axon Instruments, Foster
City, CA). Recording pipettes were pulled and fire-polished with a
horizontal Flaming-Brown microelectrode puller (Sutter Instrument
Company, San Rafael, CA). To reduce the pipette capacitance, we coated
regions close to the tip of the pipette with Sylgard 184 (Dow
Coring, Midland, MI). Pipettes had a final resistance of 0.7-1.6 M .
Series resistance (1.2-4.5 M ) was compensated (nominally 50-60%).
Records were filtered at 5 kHz with a low-pass Bessel filter and were
digitized at 10 kHz with a Digidata interface controlled by the pClamp
software version 5.7.1 (Axon Instruments). Data were stored on a
personal computer (Gateway, Sioux City, SD). Leakage current was
canceled on-line with the p/ 5 protocol. Cell capacitance was
measured as described (Yamoah et al., 1994 ). After the capacitance of
the electrode had been canceled electronically, cells were held at 60
mV and stepped to 80 mV ( V = 20 mV). The time constant of
relaxation and the area above the transient that represents the charge
(Q) were measured. The capacitance (Cm) was calculated from the equation
Cm = Q/ V. Analyses of the data were performed using Clampfit (Axon Instruments), Sigma plot (Jandel Scientific, San Rafael, CA), and Microcal Origin (Microcal Software, Northampton, MA) programs. Values are expressed as mean ± SD.
Intracellular recording. Isolated nervous systems were
incubated in a protease solution (P-8038, 2 mg/ml in ASW; Sigma) at room temperature for 7 min to facilitate microelectrode penetration. Photoreceptors were impaled using 30-45 M microelectrodes filled with potassium acetate. Current-clamp experiments were accomplished via
an Axoclamp 2A (Axon Instruments). Data were fed into a tape recorder
and later digitized at 1 kHz or obtained as recordings from a
Gould Brush recorder.
 |
RESULTS |
We investigated the membrane properties of Hermissenda
photoreceptors to understand the underlying mechanisms for spontaneous activity and the response of type A and B photoreceptors to light and
darkness. The kinetic and pharmacological properties of a low-voltage
activated transient calcium current
(ICat) and two inward rectifier currents
were examined in both cell types. Type A and B cells expressed
ICat at similar densities. Two types of inward
rectifier currents are described from both type A and B cells,
time-dependent and time-independent currents. Both cell types expressed
the two currents, but the A cells predominantly expressed the
time-independent current (~90%), whereas the B cells exhibited the
time-dependent current (~77%).
Light response and dark adaptation of photoreceptors
Figure 1 illustrates the basic
differences in the electrical properties of type A and B
photoreceptors. Figure 1 (top) shows the light response of a
typical type A cell during a 5 sec light pulse. The A cells are
relatively hyperpolarized at rest compared with type B cells (Alkon and
Fuortes, 1972 ) and are quiescent after dark adaptation. In
contrast, as shown in Figure 1 (bottom), B cells are
tonically active even after dark adaptation. Inspection of the records
in Figure 1 suggests that type A and B photoreceptors differ both in
their tonic and phasic responses to light. We speculated that the
inward currents expressed by the two cell types may differ, rendering
the B cells spontaneously active while the A cells remain electrically
silent after dark adaptation. Three inward currents were found to be
crucial for the dark-response properties of the A and B cells.

View larger version (11K):
[in this window]
[in a new window]
|
Figure 1.
Differences in light- and dark-response properties
of Hermissenda photoreceptors.
Top, Voltage response obtained in a type A cell
with a 5 sec light pulse (solid bar) is shown. The
nervous system was bathed in artificial seawater, and the photoreceptor
was impaled with an electrode containing a 3 M potassium
acetate solution. After attenuation of the light stimuli, the membrane
potential of A cells typically drops to the resting potential and
remains silent in darkness. Inhibitory synaptic potentials induced from
adjacent photoreceptors can be recorded. Bottom, Type B
cells continue to be tonically active in darkness. A 5 sec light flash
induces the characteristic membrane depolarization shown here. In
contrast to A cells, B cells remain spontaneously active in the
dark-adapted state.
|
|
Transient calcium current
Transient low-voltage activated Ca2+
currents have been reported to contribute to the initial depolarization
phase of action potentials (Llinas and Yarom, 1981 ). The transient
Ca2+ current in the soma of the photoreceptors has
been studied previously (Yamoah and Crow, 1994 ), but the functions of
the current are unknown. Experiments were performed in solutions
expected to suppress all ionic currents except Ca2+
currents (see Materials and Methods). Shown in Figure
2A are representative
traces of the transient component of the
Ca2+ current recorded from a type B cell at a
holding potential of 90 mV. Data of the current density plot from
types A and B cells are represented in Figure 2B. In
both cell types, the current was activated at potentials close to 50
mV and peaked at approximately 10 to 0 mV. There were no significant
differences between the two cell types in the current densities at all
recorded step potentials. The examples shown represent cells that
predominantly express the transient component of the
Ca2+ current. Typically, we isolated the transient
current by suppressing the sustained Ca2+ current
with bath application of nitrendipine (5 µM) (Yamoah and
Crow, 1994 ). Steady-state activation and inactivation of
ICat revealed a window current close to the
resting potential of the photoreceptors ( 60 to 40 mV) (Fig.
2C). A previous report showed that both type A and B cells
express sustained and transient Ca2+ currents
(Yamoah and Crow, 1994 , 1996 ). In an A cell in which both
Ca2+ current subtypes were expressed,
Ni2+ blocked the transient component but left the
sustained current unblocked (Fig. 2D). Typical
traces of the effects of Ni2+ on
ICat in an A cell are shown in Figure
2E. The records show that the transient
Ca2+ current was reduced by Ni2+
in a concentration-dependent manner with a half-blocking concentration of 0.4 ± 0.21 mM (n = 6). The time
course and the concentration dependence of the blocking action of
Ni2+ on the transient current are demonstrated in
Figure 2F. The effect of Ni2+ was
reversed after ~50 sec of washout.

View larger version (28K):
[in this window]
[in a new window]
|
Figure 2.
Transient Ca2+ current.
A, Examples of transient Ca2+ current
traces generated by depolarizing voltage steps in a B
cell in ASW with 10 mM Ca2+ are shown.
Voltage steps were delivered from the holding potential of 90 mV to
potentials ranging from 80 to 60 mV in 10 mV increments. Some
traces have been removed for clarity. B,
The I-V relations of current densities plotted as a
function of voltage from type A ( ) and B ( ) cells are shown. Cell
capacitance was measured as described in Materials and Methods.
C, In a type B cell that predominantly expressed the
transient Ca2+ current, steady-state activation
( ) and inactivation ( ) curves were generated and fitted
to a Boltzmann function. The fits are plotted with
solid and dotted lines. Half-activation and
inactivation (assuming complete voltage-dependent inactivation) were
40 and 48 mV, respectively. The maximum slopes for the activation
and inactivation curves were 10 and 11 mV, respectively. Overlap of the
steady-state activation and inactivation curves at a voltage range of
60 to 40 mV suggests that the Ca2+ current is
active at the resting potentials of the photoreceptors ( 55 to 45
mV). D, Ni2+ at 0.5 to 2 mM selectively blocked the transient
Ca2+ current. The current
traces were elicited from a holding potential of 90 mV
and stepped to 20 mV from a type A cell. Only the sustained
Ca2+ current remained after application of 0.8 mM Ni2+. The difference current
(Ni2+-sensitive current; trace shown
with dotted line) is the transient component.
E, Changes in the transient Ca2+
current magnitude as [Ni2+] was gradually
increased from 0 to 0.8 mM are shown. F, The
effect of Ni2+ was reversible after washout.
The time course and the effect of different concentrations of
Ni2+ on the transient Ca2+
current are shown.
|
|
Time-dependent inward rectifier current
In Figure 3A are
representative traces of a time-dependent,
hyperpolarization-activated current recorded from a type B cell with a
holding potential of 45 mV. A previous report of inward rectification
in the photoreceptors identified the current as Iir (Acosta-Urquidi and Crow, 1993 ). In the
initial report, only one form of inward rectification in the B
photoreceptors was examined. As shown below, there are two distinct
types of inward rectification in type A and B cells. Because of the
similarities of the inward rectifier current in the B cells to the
time-dependent hyperpolarization-activated currents in photoreceptors
(Hestrin, 1987 ) and other systems (Angstadt and Calabrese, 1989 ;
Holt and Eatock, 1995 ), the current will be denoted
Ih. Tail current traces from
the same cell are shown (Fig. 3B). The current-voltage
relationship is shown in Figure 3C. The permeation property
of the channel was assessed by alteration of bath
[K+], [Na+], and
[Cl ]. Alteration of bath or pipette
[K+] shifted the reversal potential
(Erev) of the current (Fig.
3C). An increase in bath [Na+] shifted
the Erev to more positive voltages, whereas the
reverse was the case when [Na+] was reduced (Fig.
3D). In contrast, changes in [Cl ] did
not alter the Erev of the current. A small but
significant Cl current is present in the
photoreceptors (Yamoah and Kuzirian, 1994 ); however, this current is
predominantly outward rectifying. Therefore, Cl
current contributes very little to the total inward-rectifying current
in the photoreceptors.

View larger version (24K):
[in this window]
[in a new window]
|
Figure 3.
Time-dependent inward rectifier current
(Ih). A, A type B
photoreceptor was held at 45 mV and stepped to positive and negative
voltages relative to the holding potential ( V = 7 mV). A
time-dependent inward current that exhibited rectification at
potentials positive to the apparent reversal potential was elicited.
Traces shown were collected from an average of five
runs. B, Shown as well are tail current
traces from the same cell. C, The
corresponding I-V plot is shown. An apparent reversal
potential of 36 mV was calculated from the regression line generated
from instantaneous current traces ( ). Alteration of
external K+ concentration
([K+]o) shifted the apparent
reversal potential of Ih. Pipette
[K+]i was 250 mM, and the
altered [K+]o was 2.5, 10, or 30 mM, shown on the corresponding I-V plots as
, , or , respectively. D, Changes in
[Na+]o also altered the apparent
reversal potential (Erev) of
Ih. Alteration of
Erev by changing
[Na+]o suggested that the
Ih channel is permeable to
Na+ as well. Shown are representative plots of the
instantaneous I-V relationship generated
from tail current records with varying
[Na+]o. The
[Na+]o, the corresponding
Erev, and the conductances are 20 mM, 30.9 mV, 21.1 nS; 70 mM, 22.8 mV, 22.8 nS; and 100 mM, 15.6 mV, 27.0 nS, shown as , , and
, respectively. Using the Goldman-Hodgkin-Katz equation (Hille,
1992 ), the permeability ratio for K+ versus
Na+
(PK/PNa) = 0.7 for this channel.
|
|
Activation of the current was voltage- and time-dependent. A
normalized, steady-state activation curve for
Ih is presented in Figure
4A. The Boltzmann
distribution fit for the curve had a half-activation voltage
(V1/2) of 74 ± 5 mV and a maximum slope (Km) of 15.5 ± 2.3 mV
(n = 9). A single time constant provided a best fit for
the activation and deactivation profiles of the current. A plot of the
time constants of activation and deactivation versus membrane
potentials is shown in Figure 4B.

View larger version (19K):
[in this window]
[in a new window]
|
Figure 4.
Steady-state activation of
Ih and the time constant of activation.
A, The relative current plotted against the step
potentials. Error bars represent SD (n = 9 cells).
The continuous curve was generated from the Boltzmann function
(I/Imax = [1+exp(V1/2-V)/Km
] 1), where V1/2 is the half-activation
voltage and Km is the maximum slope;
V1/2 of 73.6 ± 5.1 mV and
Km of 15.5 ± 2.3 mV were
estimated. B, Time constants of activation and
deactivation fitted with a single exponential and plotted against the
corresponding voltages. Representative data from five cells are plotted
with scattered points. C, Block of
Ih by Cs+. The
time-dependent inward rectifier current was blocked in the presence of
0.5 mM Cs+. Cs+
induced a rapid decay of the current. D,
Current-voltage relationship of control ( ) and after application of
0.5 mM Cs+ ( ) (n = 6 type B cells). In the presence of 2 mM
Cs+, most of the inward-rectifying currents were
blocked; however, there remained a time-independent current (data not
shown). In five type B cells with a peak current of 1.95 ± 0.98 nA, the remaining time-independent peak current after application of 2 mM Cs+ was 0.20 ± 0.14 nA.
Therefore it is estimated that only 10% of inward rectification in the
type B cells is time-independent. E, Estimation of the
binding site for Cs+. The voltage dependence of
Cs+ blockade of the pore was determined assuming a
binding model as described previously (Woodhull, 1973 ). The model
assumes a single site for Cs+ binding whose
availability but not intrinsic affinity changes with voltage.
Cs+ is assumed to be an impermeant blocker that
enters and exits the pore from the same side. A linear transformation
of the voltage dependence of the ratio of the unblocked current (peak
current amplitude) and blocked current (steady-state current amplitude)
is as follows:
ln{(Ic/Ib) 1} = ln(KA) × [Cs+] (ZeV/RT),
where Ic is the unblocked and
Ib is the blocked macroscopic current
amplitudes, KA is the association
constant, is the fractional electrical distance from the outer face
of the membrane, and Z, e,
R, and T have their usual meanings. The
slope of the linear plot gives the . The data were fit by least
squares linear regression. The calculated membrane electric field
(z ) sensed by Cs+ from the linear plot was
0.8.
|
|
The sensitivity to block of Ih by
Cs+ was tested (Angstadt and Calabrese, 1989 ; Bond
et al., 1994 ). Cs+ blocked
Ih in a voltage- and
concentration-dependent manner. At large negative pulses, the current
turned on rapidly and then decayed with time. This decay became
pronounced in the presence of Cs+ (Fig.
4C). The current-voltage relationships for control
traces and after application of 0.5 mM
Cs+ were obtained from six B cells (Fig.
4D). The apparent fraction of the membrane electric
field (z ) sensed by Cs+ was calculated to be
0.8 ± 0.1 (n = 5) (Fig.
4E; Woodhull, 1973 ). Sensitivity of the current to
Cs+ is similar to the inwardly rectifying
conductances observed in vertebrate CNS neurons (Yamaguchi et
al., 1990 ), optic nerve, and cone photoreceptors (Eng et al., 1990 ;
Maricq and Korenbrot, 1990 ), as well as in invertebrate neurons
(Angstadt and Calabrese, 1989 ). However, the
hyperpolarization-activated current in Hermissenda photoreceptors is dissimilar to those reported from retinal glial cells
(Newman, 1993 ), cholinergic neurons in rat brain (Yamaguchi et al.,
1990 ), and Aplysia buccal muscles (Brezina et al., 1994 ) in
that the current showed no sensitivity to Ba2+. In
fact, in the presence of Ba2+ or
Ca2+, the magnitude of the current increased (data
not shown). This may reflect contamination of
Ih by a background Ca2+
current in the photoreceptors. To avoid the masking effects of a
possible hyperpolarizing-activated Ca2+ conductance
(Preston et al., 1992 ), we made recordings of
Ih at reduced [Ca2+]
(see Materials and Methods).
Time-independent inward rectifier current
Type A cells expressed a time-dependent and time-independent
inwardly rectifying current. However, the time-independent current was
predominant (~77%; n = 6; Fig.
5) in the A cells. We refer to the
time-independent inward rectifier current as
IK1, consistent with the terminology used
for a similar current in cardiac cells (Kurachi, 1985 ). Figure
5A shows current traces recorded in a type A cell
superfused with a Na+-free recording solution during
hyperpolarizing voltage steps from the 50 mV holding potential.
Hyperpolarization to potentials more negative than 70 mV induced an
inward current. The current activated rapidly and exhibited little or
no decay. As the bath [K+]o was
increased, the reversal potential of the current shifted to more
positive potentials, in a manner predicted by the Nernst potential for
a K+-selective conductance (Fig. 5C).
Raising [K+]o resulted in a steeper
slope conductance as well and produced a shift in the activation
voltage range of the current in the positive direction (data not
shown). In contrast to Ih,
IK1 was blocked by Ba2+ (Fig.
5A,B). Ba2+
produced a voltage-dependent block of
IK1, and the fractional electrical
distance between the external orifice of the channels and the
Ba2+ binding site was calculated to be 0.6 ± 0.1 (n = 4: see Fig. 5D,E). Application of
Na+-containing solution induced an apparent
inactivation of the current that is reminiscent of the extracellular
Na+ block of inward rectifier currents observed in
tunicate egg cells (Ohmori, 1978 ), skeletal muscles (Standen and
Stanfield, 1979 ), and endothelial cells (Silver and DeCoursey,
1990 ).

View larger version (23K):
[in this window]
[in a new window]
|
Figure 5.
The inward rectifier current in type A
photoreceptors was carried by K+. A,
Type A cells also exhibited inward rectification; however this current
was time-independent, and the apparent Erev
was more negative ( 70 to 80 mV) than were currents recorded from
type B cells ( 30 to 40 mV). B, This inward rectifier
current can be blocked by Ba2+. The remaining
current after application of Ba2+
(inset) exhibited a time dependence of activation and
can be blocked by Cs+. The effects of
Ba2+ were reversible (data not shown).
C, By varying the external concentration of
K+ and maintaining a constant pipette
K+ concentration of 250 mM, we obtained
the reversal potentials of the inward rectifier current; these were
plotted against the external K+ concentration. Data
were fit with a linear regression with a slope of 56 mV per log unit
(r = 0.989), consistent with a
K+-selective pore. D, The
current-voltage relations of the inward rectifier current at baseline
( ; n = 7) and after application of 0.25 mM ( ) and 2.5 mM ( )
Ba2+ are illustrated. This current was more
sensitive to block by Ba2+ than by
Cs+ (data not shown). Cumulative data from six type
A cells (control peak current, 1.59 ± 0.54 nA;
Ba2+-insensitive time-dependent current, 0.35 ± 0.21 nA) show that type A cells expressed ~77% of
IK1 and 23% of Ih.
E, The binding site of Ba2+ within
the pore is estimated. The slope yields a of 0.6 from the outer
face of the membrane (see Fig. 4E).
|
|
Effects of Cs+, Ba2+, and
Ni2+ on the excitability of A and B cells
Alkon (1979) reported that Ni2+ altered
spontaneous activity of B photoreceptors. Although the mechanisms for
the effects of Ni2+ were not investigated, it is
possible that Ni2+ block of the
ICat may be the underlying mechanism for
Ni2+-induced alteration of spontaneous activity of
the B cells. It has been suggested that inward rectification is
responsible for a voltage "sag" observed in the B cells after the
injection of hyperpolarizing currents (Acosta-Urquidi and Crow,
1995 ). The voltage sag is followed by a rebound spike
activity. A combination of the inward currents may partly explain the
differences in the properties of A and B photoreceptors. This idea was
examined further by blocking the transient Ca2+ and
inward rectifier currents with bath application of
Ni2+, Cs+, and
Ba2+.
To account for diffusional barriers in intact preparations, we applied
relatively high concentrations of the blockers. Figure 6 illustrates the effects of
Ni2+ and Cs+ on type B cells.
Block of the transient Ca2+ current by
Ni2+ induced a burst pattern that was
characteristically phasic, unlike the nonphasic, spontaneous activity
of the B cells in vivo. In Figure 6A, 1.5 mM Ni2+ reduced the frequency of
spontaneous activity. Spontaneous activity of the photoreceptors was
reduced further after the application of 2 mM
Cs+. Both Ni2+ and
Cs+ reduced the spontaneous firing of the type B
cells (Fig. 6B-D). Cs+ alone
induced membrane hyperpolarization and reduced the rate of firing of B
cells (Fig. 7). We further illustrate
that membrane depolarization by current injection was insufficient to
increase the firing rate, after block of
Ih by Cs+. The effects
of Cs+ were reversible after washout.

View larger version (36K):
[in this window]
[in a new window]
|
Figure 6.
Pharmacological manipulation of the electrical
activity of type B cells with Ni2+ and
Cs+. A, The characteristic tonic
activity of B cells in control solutions is transformed into
alternating burst activity after bath perfusion with 1.5 mM
Ni2+-containing artificial seawater. Addition of 2 mM Cs+ to the Ni2+
solution completely abolished spontaneous activity of the B cell in
dark-adapted conditions. B, Top,
Light-elicited generator potential and the corresponding spike rate in
the predark-adapted stage were reduced in the presence of
Ni2+ and Cs+.
Bottom, Replacement of Ni2+- and
Cs+-containing solution with normal artificial
seawater restored the excitability of the B cells. C, In
the cell shown in B, Ni2+ decreased
the spike rate from ~3 to 1 Hz; Cs+ reduced the
spike rate further to 0 Hz. D, Data from five cells on
the effects of Ni2+ and Cs+ on
spike rate and membrane potential are shown.
|
|

View larger version (28K):
[in this window]
[in a new window]
|
Figure 7.
Effects of Cs+ on the membrane
properties of type B photoreceptors. A, Spontaneous
activity of B photoreceptors in normal artificial seawater consists of
uninterrupted burst spikes in type B photoreceptors in the dark. After
application of 2 mM Cs+, the
steady-state potential dropped to a more hyperpolarized potential, and
the spike rate was reduced. Injection of positive current to depolarize
the steady-state potential close to control conditions was insufficient
to restore the spike rate. However, after 10 min of washout, the spike
rate returned to control levels. B, In the B cell shown
in A, Cs+ induced a spike rate of
~0.5 Hz compared with a rate in controls of 2.5 Hz. C,
Cumulative data from five type B cells are shown.
Cs+ reduced the spike rate from 2.7 ± 0.5 to
0.7 ± 0.3 Hz. However, the spike rate returned to 2.5 ± 0.4 Hz that was not significantly different from control after
washout.
|
|
Type A and B cells have similar spike rates in response to light (~40
Hz), but the two cell types are dissimilar in their dark-response
properties (Fig. 8). The B cells remain
tonically active with a spike rate of ~3 Hz in darkness, whereas the
A cells remain quiet after termination of light stimuli (Fig. 8).
Ba2+, a specific blocker of
IK1, significantly increased the
spontaneous activity of A cells in darkness [spike frequency in the
dark, 0.2 ± 0.2 Hz (mean ± SD); spike frequency in darkness
in the presence of Ba2+, 2.2 ± 1.1 Hz
(mean ± SD); n = 5; p < 0.005]
but failed to produce substantial changes in the light-elicited spike
activity in type A and B cells (see Fig. 8B). In
contrast to the activity in type A cells, the tonic activity of type B
cells in darkness was not significantly altered by
Ba2+ (spike frequency of B cells in the dark,
2.5 ± 0.6 Hz; spike frequency in darkness in the presence of
Ba2+, 2.6 ± 0.6 Hz; n = 5;
p = 0.8, not significant).

View larger version (24K):
[in this window]
[in a new window]
|
Figure 8.
Effects of Ba2+ on spike rates
of type A and B cells. A, Profile of electrical activity
of type A and B photoreceptors before and after stimulation with a 5 sec light stimulus. As seen in previous figures, the B cells retained
spontaneous activity after the light was turned off. B,
Histograms generated from five A and B photoreceptors.
Ba2+ (1 mM) increased the spike rate of
type A cells approximately 10-fold from 0.2 ± 0.2 to 2.2 ± 1.1 Hz. However, the light-elicited spike rate remained virtually the
same in the presence or absence of Ba2+. The
postlight electrical activity of the A cells was enhanced further in
Ba2+-containing artificial seawater than in normal
artificial seawater. In contrast, Ba2+ produced no
significant change in spike rates in type B cells both in the pre- and
postlight conditions. Prelight (pre) corresponds
to 20 min of dark adaptation, and postlight
(post) corresponds to 2 min after light
stimulation.
|
|
 |
DISCUSSION |
The properties of a transient Ca2+ and two
distinct inward rectifier currents in the photoreceptors of
Hermissenda were studied to understand the underlying
mechanisms for the electrophysiological differences between type A and
B photoreceptors. Here, we report the following. (1) A transient
Ca2+ current is expressed in both cells at similar
densities, and this current contributes to the generation of action
potentials in both cell types. (2) Both type A and B photoreceptors
express two inward rectifier currents, a time-dependent
(Ih) current and a time-independent
(IK1) current. However,
IK1 is predominantly expressed by the type A
cells. (3) In contrast, type B photoreceptors express mainly
Ih that has kinetic and pharmacological
properties that are distinct from IK1. (4)
IK1 contributes to membrane hyperpolarization and controls the resting membrane potential of cells during dark adaptation, whereas Ih enhances membrane
depolarization and promotes the spontaneous firing properties of the
cells in the dark. The additive properties of the
Ca2+ current and Ih
induce spontaneous activity in the B cells. However, the predominant
expression of IK1 in type A cells results in
membrane hyperpolarization and virtual quiescence in the dark.
Transient Ca2+ current
Previous reports attest that the photoreceptors express two
distinct Ca2+ currents, transient
(ICat) and sustained
(ICas) currents, and that no significant
differences were observed in the level of expression of the two
currents in the two cell types (Yamoah and Crow, 1996 ). The transient
current is classified as a T-like current (Nowycky et al., 1985 )
because it is activated at low voltages, has a rapid onset, is
inactivated at a relatively faster rate than is the sustained
Ca2+ current, and is selectively blocked by
Ni2+. ICat contributes to
rhythmic membrane spike activity in the type B photoreceptors, based on
the evidence that Ni2+ alters the frequency and
phasic properties of spontaneous activity of the cells. The voltage
dependence of both the activation and inactivation of
ICat revealed the existence of a window current at 50 to 30 mV, suggesting that at rest and during the
repolarization phase of a generator potential,
ICat may contribute to the total depolarization-induced currents.
Inward rectifiers
Evidence of the distinction between
Ih and IK1 is as
follows. (1) Ih was activated with time,
whereas activation of IK1 was time-independent.
(2) Ih was permeable to both
Na+ and K+, whereas
IK1 was relatively
K+-selective. (3) Ba2+
selectively blocked IK1 without having any
blocking action on Ih. (4) The kinetics of
block of the two currents by monovalent cations was different. From
these data, we conclude that two distinct inward-rectifying currents
exist in Hermissenda photoreceptors. The existence of
K+-selective and
Na+/K+-selective inward rectifier
currents in seemingly homogeneous cells has been reported in frog hair
cells (Holt and Eatock, 1995 ) and cardiac myocytes (Wu et al., 1991 ).
It is worth noting that in the right atrium of cats, ~90% of
myocytes that exhibit spontaneous pacemaker activity also express
Ih-like currents called
If, whereas approximately the same
population of quiescent cells was found to exhibit
IK1-like currents (Wu et al., 1991 ). Presumably,
the predominance of Ih-like current is one
of the requirements for spontaneous activity, whereas quiescence cells
may require IK1-like background current.
The properties of the inward-rectifying currents in the photoreceptors
account for some of the characteristic properties of the
photoreceptors. Specifically, Ih shares
features that are consistent with spontaneous pacemaker activity in the
B cells. (1) The activation threshold of
Ih ( 40 to 50 mV) is compatible with
the induction of afterdepolarization during the repolarization phase of
action and generator potentials. Also, the permeation properties of the
channels (Na+ and K+) and the
corresponding Erev of
Ih (approximately 40 mV) indicate that
at rest (approximately 50 mV) Ih
promotes membrane depolarization. (2) The time-dependent activation
kinetics of Ih is consistent with the
pacing of type B cells after dark adaptation (~3 Hz); however, as
depicted in Figure 6, it is clear that spontaneous activity of the B
cells results from the transient Ca2+ current as
well. (3) The fact that Ih blocked by
Cs+ reduces the frequency of spontaneous activity is
in agreement with the hypothesis that Ih
contributes to the initiation of spontaneous activity in the B cells.
The present hypothesis predicts that in vivo
Ih is activated by an ensemble of synaptic
inhibitory potentials from adjacent photoreceptors and vestibular
neurons (Rogers et al., 1994 ). Activation of
Ih is expected to follow membrane
repolarization of action and generator potentials. If inhibitory input
from the cells adjacent to type B cells is stronger than that from
those adjacent to type A cells, as suggested by Alkon and
Fuortes (1972) , then Ih in the B
cells will be poised to induce an enhanced membrane depolarization to
produce tonic activity. Because Ih
exhibits no inactivation at potentials close to the resting potential
of the B cells (approximately 50 mV), activation of
Ih can be cumulative, thus resulting in
phasic depolarization of the membrane potential. As seen in Figure
6A, after suppressing the transient
Ca2+ currents with Ni2+,
nonphasic spike activity in the B cells was transformed into a phasic
firing pattern that was abolished after application of Cs+. Thus, the properties of
Ih can account, at least in part, for the
reported properties of the B cells.
Ih recorded from the photoreceptors
exhibits many of the properties reported for the current in leech heart
interneurons (Angstadt and Calabrese, 1989 ), neonatal spinal
motor neurons (Takahashi, 1990 ), thalamic relay neurons (Huguenard and
McCormick, 1992 ), and vertebrate photoreceptors (Maricq and Korenbrot,
1990 ). In addition, there are remarkable similarities between the
properties of Ih and those of the currents
termed If in cardiac pacemaker cells
(Yanagihara and Irisawa, 1980 ; DiFrancesco, 1985 ) and
Iq in hippocampal neurons (Halliwell and
Adams, 1982 ; Maccaferri et al., 1993 ). Permeation of the channels by
Na+ and K+ and sensitivity to
Cs+ block are a few examples of the common features
shared by these hyperpolarization-activated currents. Furthermore,
cells that express these hyperpolarization-activated currents
invariably exhibit some form of membrane potential oscillations. Thus,
the present findings on the contribution of
Ih to type B photoreceptor spontaneous
activity are consistent with previous reports on the functions of
Ih. Although many of the characteristics
of Ih are similar to those reported for
hyperpolarizing-activated currents in other systems, the time course of
activation was significantly faster than that for
Ih and/or If
in other systems; e.g., at 60 mV, the time constant of activation of
Ih in Hermissenda
photoreceptors was ~300 msec, whereas values closer to 1 sec have
been reported in leech interneurons (Angstadt and Calabrese,
1989 ), and values from 1 to 3 sec have been documented in sinoatrial
node cells (Hagiwara and Irisawa, 1989 ; Zhou and Lipsius, 1992 ). The
time course of activation is expected to affect the beat frequency of
spontaneously active cells. However, a direct correlation between the
activation of Ih and the frequency of
membrane activity will be unlikely in the photoreceptors, where
multiple conductances dictate baseline activity. Interestingly, the
time course of activation of Ih in
photoreceptors is similar to that of Ih in
saccular hair cells (Holt and Eatock, 1995 ). Similar to the
photoreceptors, saccular hair cells express two inward-rectifying
currents, one Cs+- and the other
Ba2+-sensitive (Table
1).
Inward rectification promotes membrane depolarization if the
Erev of the current is positive relative to the
resting potential of the cell. The time-independent current
IK1 has permeation properties, which are
K+ selective, making the Erev
more negative ( 70 to 75 mV) than the recorded resting potential of
the photoreceptors (approximately 50 mV). In cells that predominantly
express IK1, the current acts as a
background current that tends to restore the resting potential of the
photoreceptors. Relatively high expression of IK1 in A cells is consistent with the relatively
hyperpolarized state of the A cells at rest and the lack of spontaneous
activity in the A cells during dark adaptation.
Combined techniques of molecular cloning and electrophysiological
studies of cloned channels in heterologous expression systems have
identified several types of inward rectifier channels (Bond et al.,
1994 ). These cloned channels exhibit distinct kinetics and
pharmacology. It is of interest to correlate the properties of these
expressed channels to the native currents recorded in a more
physiological system, keeping in mind the possible differences attributable to heteromultimerization and subunit coassembly in the
native systems. Emerging data on the inward rectifier currents in both
vertebrate and invertebrate systems clearly indicate expression of
these currents, namely Ih- and
IK1-like currents, in maintaining similar
functions in seemingly diverse systems, spanning from invertebrates to
vertebrates.
 |
FOOTNOTES |
Received March 16, 1998; revised May 21, 1998; accepted May 28, 1998.
This work was supported by a Grass Foundation fellowship to E.N.Y. and
by National Institutes of Health grants to T.C. (MH40860) and L.M. We
thank Dr. J. Byrne for the use of his osmometer during the initial
phase of the experiments. We also appreciate constructive comments
provided by Dr. N. Chiamvimonvat.
Correspondence should be addressed to Dr. Ebenezer N. Yamoah,
Department of Cell Biology, Neurobiology, and Anatomy, University of
Cincinnati School of Medicine, 231 Bethesda Avenue, Cincinnati, OH
45267.
 |
REFERENCES |
-
Abrams TW
(1985)
Activity-dependent presynaptic facilitation: an associative mechanism in Aplysia.
Cell Mol Neurobiol
5:123-145[ISI][Medline].
-
Acosta-Urquidi J,
Crow T
(1993)
Differential modulation of voltage-dependent currents in Hermissenda type B photoreceptors by serotonin.
J Neurophysiol
70:541-548[Abstract/Free Full Text].
-
Acosta-Urquidi J,
Crow T
(1995)
Characterization of voltage-activated currents in Hermissenda type B photoreceptors.
J Neurosci
15:319-332[Abstract].
-
Alkon DL
(1979)
Voltage-dependent calcium and potassium ion conductances: a contingency mechanism for an associative learning model.
Science
205:810-816[Abstract/Free Full Text].
-
Alkon DL,
Fuortes MGF
(1972)
Responses of photoreceptors in Hermissenda.
J Gen Physiol
60:639-649.
-
Alkon DL,
Sakakibara M,
Forman R,
Harrigan J,
Lederhendler I,
Farley J
(1985)
Reduction of two voltage-dependent K+ currents mediates retention of a learned association.
Behav Neural Biol
44:278-300[ISI][Medline].
-
Alkon DL,
Sanchez-Andres JV,
Ito E,
Oka K,
Yoshioka T,
Collin C
(1992)
Long-term transformation of an inhibitory into excitatory GABAergic synaptic response.
Proc Natl Acad Sci USA
89:11862-11866[Abstract/Free Full Text].
-
Angstadt JD,
Calabrese RL
(1989)
A hyperpolarization-activated inward current in heart interneurons of the medicinal leech.
J Neurosci
9:2846-2857[Abstract].
-
Bond CT,
Pessia M,
Xia MX,
Lagrutta A,
Kavanaugh MP,
Adelman JP
(1994)
Cloning and expression of a family of inward rectifier potassium channels.
Receptors Channels
2:183-191[ISI][Medline].
-
Brezina C,
Evans G,
Weiss KR
(1994)
Characterization of the membrane ion currents of a model molluscan muscle, the accessory radula closer muscle of Aplysia californica. Hyperpolarization-activated currents.
J Neurophysiol
72:2093-2112.
-
Crow T
(1988)
Cellular and molecular analysis of associative learning and memory in Hermissenda.
Trends Neurosci
11:136-142[ISI][Medline].
-
Crow T,
Alkon DL
(1980)
Associative behavioral modification in Hermissenda; cellular correlates.
Science
209:412-414[Abstract/Free Full Text].
-
DiFrancesco D
(1985)
The cardiac hyperpolarizing-activated current If; origins and developments.
Prog Biophys Mol Biol
46:163-183[ISI][Medline].
-
Eng DL,
Gordon TR,
Kocsis JD,
Waxman SG
(1990)
Current-clamp analysis of a time-dependent rectification in rat optic nerve.
J Physiol (Lond)
421:185-202[Abstract/Free Full Text].
-
Farley J,
Alkon DL
(1982)
Associative neural and behavioral change in Hermissenda; consequences of nervous system orientation for light- and pairing-specificity.
J Neurophysiol
48:785-807[Free Full Text].
-
Farley J,
Richards WG,
Grover LM
(1990)
Associative learning changes intrinsic to Hermissenda type A photoreceptors.
Behav Neurosci
104:135-152[ISI][Medline].
-
Hagiwara N,
Irisawa H
(1989)
Modulation by intracellular Ca2+ of the hyperpolarization-activated inward current in rabbit single sino-atrial node cells.
J Physiol (Lond)
409:121-141[Abstract/Free Full Text].
-
Halliwell JV,
Adams PR
(1982)
Voltage-clamp analysis of muscarinic excitation in hippocampal neurons.
Brain Res
250:71-92[ISI][Medline].
-
Hamill OP,
Marty A,
Neher E,
Sakmann B,
Sigworth JF
(1981)
Improved patch-clamp techniques for high resolution current recording from cells and cell-free membrane patches.
Pflügers Arch
391:85-100[ISI][Medline].
-
Hestrin S
(1987)
The properties and function of inward rectification in rod photoreceptors of the tiger salamander.
J Physiol (Lond)
390:319-333[Abstract/Free Full Text].
-
Hille B
(1992)
In: Ionic channels of excitable membranes, 2nd edition, pp 341-347. Sunderland, MA: Sinauer.
-
Holt JR,
Eatock RA
(1995)
Inwardly rectifying currents of saccular hair cells from the leopard frog.
J Neurophysiol
73:1484-1502[Abstract/Free Full Text].
-
Huguenard JR,
McCormick DR
(1992)
Simulation of the currents involved in rhythmic oscillations in thalamic relay neurons.
J Neurophysiol
62:1373-1399.
-
Jester JM,
Campbell WL,
Sejnowski TJ
(1995)
Associative EPSP-spike potentiation induced by pairing orthodromic and antidromic stimulation in rat hippocampal slices.
J Physiol (Lond)
484:689-705[ISI][Medline].
-
Kurachi Y
(1985)
Voltage-dependent activation of the inward-rectifier potassium channel in the ventricular cell membrane of guinea-pig heart.
J Physiol (Lond)
366:365-385[Abstract/Free Full Text].
-
Llinas R,
Yarom Y
(1981)
Electrophysiology of mammalian inferior olivary neurons in vitro: different types of voltage-dependent ionic conductances.
J Physiol (Lond)
315:549-567[Abstract/Free Full Text].
-
Maccaferri G,
Mangoni M,
Lazzari A,
DiFrancesco D
(1993)
Properties of hyperpolarization-activated current in rat hippocampal CA1 pyramidal cells.
J Neurophysiol
69:2129-2136[Abstract/Free Full Text].
-
Maricq AV,
Korenbrot JI
(1990)
Inward rectification in the inner segment of single retinal cone photoreceptors.
J Neurophysiol
64:1917-1928[Abstract/Free Full Text].
-
Matzel LD,
Rogers RF
(1993)
Postsynaptic calcium, but not cumulative depolarization, is necessary for the induction of associative plasticity in Hermissenda.
J Neurosci
13:5029-5043[Abstract].
-
Newman EA
(1993)
Inward-rectifying potassium channels in retinal glial (Muller) cells.
J Neurosci
13:3333-3345[Abstract].
-
Nowycky AC,
Fox AP,
Tsien RW
(1985)
Three types of neuronal calcium channels with different calcium agonist sensitivity.
Nature
316:440-443[Medline].
-
Ohmori H
(1978)
Inactivation kinetics and steady-state current noise in the anomalous rectifier of tunicate egg cell membranes.
J Physiol (Lond)
281:77-99[Abstract/Free Full Text].
-
Preston RR,
Saimi Y,
Kung C
(1992)
Calcium current activated upon hyperpolarization of Paramecium tetraurelia.
J Gen Physiol
100:233-251[Abstract/Free Full Text].
-
Rogers RF,
Fass DM,
Matzel LD
(1994)
Current, voltage and pharmacological substrates of a novel GABA receptor in the visual-vestibular system of Hermissenda.
Brain Res
650:93-106[ISI][Medline].
-
Silver MR,
DeCoursey TE
(1990)
Intrinsic gating of inward rectifier in bovine pulmonary artery endothelial cells in the presence or absence of internal Mg2+.
J Gen Physiol
96:109-133[Abstract/Free Full Text].
-
Standen NB,
Stanfield PR
(1979)
Potassium depletion and sodium block of potassium currents under hyperpolarization in frog sartorius muscle.
J Physiol (Lond)
294:497-520[Abstract/Free Full Text].
-
Takahashi T
(1990)
Inward rectification in neonatal rat spinal motoneurons.
J Physiol (Lond)
423:47-62[Abstract/Free Full Text].
-
Woodhull AM
(1973)
Ionic blockage of sodium channels in nerve.
J Gen Physiol
61:687-708[Abstract/Free Full Text].
-
Wu J,
Vereecke J,
Carmeliet E,
Lipsius SL
(1991)
Ionic currents activated during hyperpolarization of single right atrial myocytes from cat heart.
Circ Res
68:1059-1069[Abstract/Free Full Text].
-
Yamaguchi K,
Nakajima Y,
Nakajima S,
Stanfield PR
(1990)
Modulation of inward rectifying channels by substance P in cholinergic neurons from rat brain in culture.
J Physiol (Lond)
426:499-520[Abstract/Free Full Text].
-
Yamoah EN,
Crow T
(1994)
Two components of calcium currents in the soma of photoreceptors of Hermissenda.
J Neurophysiol
72:1327-1336[Abstract/Free Full Text].
-
Yamoah EN,
Crow T
(1996)
Protein kinase and G-protein regulation of Ca2+ currents in Hermissenda photoreceptors by 5-HT and GABA.
J Neurosci
16:4799-4809[Abstract/Free Full Text].
-
Yamoah EN,
Kuzirian A
(1994)
Effects of GABA on outward currents in Hermissenda photoreceptors.
Biol Bull
187:265-266[ISI][Medline].
-
Yamoah EN,
Kuzirian AM,
Sanchez-Andres JV
(1994)
Calcium current and inactivation in identified neurons in Hermissenda crassicornis.
J Neurophysiol
72:2196-2208[Abstract/Free Full Text].
-
Yanagihara K,
Irisawa H
(1980)
Inward current activated during hyperpolarization in the rabbit sinoatrial node cell.
Pflügers Arch
185:11-19.
-
Zhou Z,
Lipsius S
(1992)
Properties of the pacemaker current (If) in latent pacemaker cells isolated from cat right atrium.
J Physiol (Lond)
453:503-523[Abstract/Free Full Text].
Copyright © 1998 Society for Neuroscience 0270-6474/98/18166501-11$05.00/0
This article has been cited by other articles:

|
 |

|
 |
 
R. Narayanan and D. Johnston
The h Channel Mediates Location Dependence and Plasticity of Intrinsic Phase Response in Rat Hippocampal Neurons
J. Neurosci.,
May 28, 2008;
28(22):
5846 - 5860.
[Abstract]
[Full Text]
[PDF]
|
 |
|

|
 |

|
 |
 
K. T. Blackwell
Ionic Currents Underlying Difference in Light Response Between Type A and Type B Photoreceptors
J Neurophysiol,
May 1, 2006;
95(5):
3060 - 3072.
[Abstract]
[Full Text]
[PDF]
|
 |
|
|