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The Journal of Neuroscience, May 1, 1999, 19(9):3353-3366
Ca2+-Permeable P2X Receptor Channels in Cultured
Rat Retinal Ganglion Cells
H.
Taschenberger,
R.
Jüttner, and
R.
Grantyn
Developmental Physiology, Institute for Physiology, Humboldt
University Medical School (Charité), D-10117 Berlin, Germany
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ABSTRACT |
ATP has been identified as an excitatory neurotransmitter in both
the CNS and peripheral nervous system; however, little is known about
the functional properties of ATP-gated channels in central neurons.
Here we used a culture preparation of the postnatal rat retina to test
the responsiveness of identified retinal ganglion cells (RGCs) and
putative amacrines to exogenous ATP and other purinoceptor agonists.
Rapidly activating ATP-induced currents (IATP) were exclusively generated in
a subpopulation (~65%) of RGCs. The latter were identified by Thy1.1
immunostaining, repetitive firing patterns, and activation of
glutamatergic autaptic currents. None of the putative amacrine cells
was ATP-sensitive. IATP could be induced
with ATP, ADP, and , -mATP but not with adenosine. It was
antagonized by suramin. The current-voltage relationship of
IATP showed marked inward rectification.
Dose-response analysis yielded an EC50 of 14.5 µM, with a Hill coefficient of 0.9. Noise analysis of
IATP suggested a mean single channel
conductance of 2.3 pS. Retinal P2X purinoceptor channels exhibited a
high permeability for Ca2+.
PCa/PCs obtained from reversal
potentials of IATP under bi-ionic conditions
amounted to 2.2 ± 0.7. In the majority of cells, the decay of
IATP was biphasic. The degree of current
inactivation during the first 2 sec of agonist application was highly
variable. Heterogeneity was also found with respect to the sensitivity
to ADP and , -mATP and the blocking action of suramin, suggesting expression of multiple P2X receptor subtypes. Our results indicate that
activation of P2X receptor channels represents an important pathway for
Ca2+ influx in postnatal RGCs.
Key words:
adenosine triphosphate; purinoceptors; P2X; rat; retina; retinal ganglion cells; patch clamp; Ca2+
permeability; fura-2
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INTRODUCTION |
ATP has been regarded as
a fast neurotransmitter or co-transmitter with noradrenaline or
acetylcholine (Westfall et al., 1990 ; von Kügelgen and Starke,
1991 ; Edwards, 1994 ). In sensory structures of the spinal cord and
brain, the action of ATP was excitatory, and voltage-clamp experiments
demonstrated that exogenous ATP or its analogs induced cation
conductances (Jahr and Jessell, 1983 ; Ueno et al., 1992 ; Shen and
North, 1993 ). Purinergic excitatory synaptic currents have been
demonstrated in rat medial habenular neurons (Edwards et al., 1992 ) and
cultured neurons from rodent celiac ganglion (Evans et al., 1992 ).
Extracellular ATP is rapidly degraded by ecto-nucleotidases
(Zimmermann, 1996 ). The targets of ATP and its degradation product adenosine are P2 and P1 receptors, respectively. P2 receptors have been
classified according to their transduction mechanisms into ionotropic
(P2X) and G-protein-coupled metabotropic (P2Y) receptors. Molecular
cloning studies have identified seven different P2X subunits that
assemble to cation channels with distinct functional properties (North
and Barnard, 1997 ; Soto et al., 1997 ). In the vertebrate CNS, P2X
purinoceptors are abundant but display great variability in their
regional expression patterns (Collo et al., 1996 ; Séguéla
et al., 1996 ; Vulchanova et al., 1996 ).
In contrast to the wealth of data concerning nucleotide signaling in
the somatosensory and peripheral auditory system (Brake and Julius,
1996 ; Housley, 1998 ), very little is known about the role of
extracellular nucleotides in the visual system. A functional role for
ATP and its metabolites in visual signal processing has been suggested
by Blazynski and Perez (1991) , who showed that nucleotides were
released from the rabbit retina via Ca2+-dependent
and Ca2+-independent mechanisms. Using an eye-cup
preparation from rabbit, it was shown that P2 antagonists increased and
exogenous ATP decreased the light-induced release of acetylcholine
(Neal and Cunningham, 1994 ). These authors envisaged the possibility
that co-released ATP modulates light-evoked acetylcholine release from
amacrine cells via an inhibitory feedback loop. Stores of endogenous
adenosine were discovered in the inner retina of the rabbit (Blazynski
and Perez, 1991 ). In the rat retina, receptors for ATP were found in
photoreceptors and neurons of the inner nuclear and ganglion cell layer
(Greenwood et al., 1997 ). However, the cellular distribution of retinal
P2X receptors and their functional properties have remained unexplored.
We used a previously established culture model of the postnatal rat
retina (Taschenberger and Grantyn, 1995 ) to characterize the current
responses to exogenous ATP in defined neuronal populations. The first
aim of our study was to clarify which neurons in the inner retina
express P2X receptors. Furthermore, we addressed the possible
heterogeneity of retinal purinoceptor channels by comparing kinetic
properties and pharmacological profiles of ATP-activated currents
because it is known that the rodent retina contains several P2X
subunits (Brändle et al., 1998 ). Finally, we asked whether P2X
receptor channels can serve as a pathway for Ca2+
influx. Our data show that exogenous ATP induces depolarizing currents
with slow inactivation and high fractional Ca2+
influx selectively in ganglion cells.
A preliminary report of this work has appeared previously in abstract
form (Taschenberger and Grantyn, 1998b ).
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MATERIALS AND METHODS |
Cell culture. Experiments were performed on cultured
retinal neurons between 6 hr after plating up to 17 d in
vitro (DIV). Dissociated cell cultures were obtained from the
postnatal rat retina (postnatal day 3-7) and prepared as described
previously (Taschenberger and Grantyn, 1995 ), with one important
modification. The culture medium consisted of DMEM (Sigma, St. Louis,
MO) and was supplemented with a mixture of co-factors, vitamins, and
antioxidants essentially as described by Brewer and Cotman (1989) .
Additionally, 20 ng/ml recombinant BDNF and 5 µM
forskolin were added (Meyer Franke et al., 1995 ). Neuritogenesis and
survival of retinal ganglion cells (RGCs) were greatly enhanced under
these culture conditions. Retinal cultures were maintained at 35.5°C
in a 10% CO2, 90% moist air atmosphere. During the
first 3 DIV, the culture medium was supplemented with 2% horse serum
and 2% fetal calf serum. When non-neuronal cells reached 50-70%
confluence (usually at DIV 3), the culture medium was completely
exchanged, and cells were kept in serum-free medium for the rest of the
culture period.
Discrimination between retinal ganglion cells and putative
amacrine cells. A combination of morphological and functional
criteria allowed us to discriminate between GABAergic putative amacrine cells and glutamatergic RGCs at different stages of their in
vitro development. In the rat retina, ganglion cells constitute
the neuron population with the largest soma diameter (Huxlin and
Goodchild, 1997 ). Among short-term (DIV 0-3) cultured neurons of the
postnatal rat retina, all neurons with soma diameter >13 µm can be
retrogradely labeled (Grantyn and Korenbaum, 1992 ) and are
Thy1.1-positive (Guenther et al., 1994 ). Neurons that satisfied this
size criterion were therefore regarded as RGCs (see Fig.
3A,B). In long-term cultures ( 4 DIV), both cell types were
unambiguously distinguished by anti-Thy1.1 immunostaining (see Fig.
3C,D). Vital immunostaining of retinal cultures was
performed as described previously (Taschenberger and Grantyn, 1995 ).
Briefly, cultures were incubated with the monoclonal mouse anti-Thy1.1
antibody MRC OX-7 (1:40) (Serotec, Indianapolis, IN). Subsequently,
RGCs were identified by visualization of the Thy1.1 epitope under
fluorescent illumination after incubation with phycoerythrin-conjugated
goat anti-mouse antibody (1:100) (Jackson ImmunoResearch, West Grove,
PA). After staining, cultures were used for electrophysiological
experiments (see Fig. 3C,D). A small population of GABAergic
putative amacrine cells express Thy1.1 on a low level (Perry et al.,
1984 ; Taschenberger and Grantyn, 1995 ). These very weakly stained cells
were clearly discernible from Thy1.1-positive RGCs and, for the sake of
simplicity, will also be referred to as Thy1.1-negative.
In addition, cultured RGCs and putative amacrines differ in amplitudes
of voltage-activated Na+ currents and can be
separated according to the intrinsic pattern of the action potentials
that they generate on sustained current injection under current-clamp
conditions (Taschenberger and Grantyn, 1995 ). Glutamatergic RGCs are
regular spiking neurons with slow-frequency adaptation, whereas
GABAergic amacrines generate only few spikes that tend to inactivate
quickly (see Fig. 2A-C). Synaptic glutamate release
from RGCs was demonstrated by recording autaptic responses to
short depolarizing voltage steps (400 µsec, 5 mV).
Experimental solutions. During experiments cells were bathed
in control saline containing (in mM): NaCl 136, KCl 5.36, CaCl2 3, MgCl2 1, glucose 25, HEPES 15. To
investigate the Ca2+ permeability of retinal
ATP-activated channels, the recording chamber contained
Na+-free solution consisting of (in mM):
140 N-methyl-D-glucamine (NMDG), 20 CaCl2, 25 glucose, and 15 HEPES, pH 7.3. In the
majority of experiments, patch pipettes were filled with a solution of the following composition (in mM): CsCl 145, CaCl2 0.5, MgCl2 1, EGTA 5, HEPES 25, glucose
10, pH 7.3. In some experiments, pipettes contained 115 mM
Cs-gluconate, 30 mM CsCl or 115 mM K-gluconate, 30 mM KCl instead of 145 mM CsCl.
At the beginning of patch-clamp experiments, current output was set to
zero with the pipette being immersed in the bath. The time-dependent
drift of the offset potential was measured after the membrane patch was
destroyed. It was always 3 mV and therefore disregarded. Junction
potentials between pipette and bath solutions were measured as
described in Neher (1992) . For Na+-rich external
solution, reported reversal potentials were corrected by 4.5, 11,
and 10 mV for CsCl-, Cs-gluconate-, and K-gluconate-filled patch
pipettes, respectively. For NMDG+-containing bath
solution, Erev was corrected by 7.5 mV
(CsCl-filled electrodes). All experiments were performed at room
temperature (22-24°C).
Drug application. Drugs were applied via a gravity-driven
superfusion system with an outflow pipette of ~50 µm opening
diameter. An additional suction pipette (~70 µm opening diameter)
ensured the complete removal of test solutions from the bath. To switch between superfusion channels we used manually operated valves. In the
vicinity of the cell under investigation, the total exchange of test
solutions was accomplished in <1 sec. In some experiments rapid drug
application was performed by means of computer-operated electromagnetic
valves (Taschenberger and Grantyn, 1998a ).
6,7-Dinitroquinoxaline-2,3-dione (DNQX) was purchased from Tocris
Neuramin. Suramin and , -methylene ATP ( , -mATP) were
obtained from RBI (Natick, MA). All other chemicals were from Sigma.
Whole-cell patch-clamp recording. Whole-cell voltage-clamp
recordings were performed using an EPC-7 patch-clamp amplifier (List,
Darmstadt, Germany). Currents were measured through a 500 M feedback
resistor and low-pass-filtered at 3 kHz (three-pole Bessel filter).
Capacitive transients were reduced by analog circuitry. Patch pipettes
were pulled from thick-walled borosilicate tubing (WPI, Sarasota, FL)
on a Sutter P-87 micropipette puller (Sutter Instruments, Novato, CA).
The pipette to bath resistance of patch electrodes ranged from 4 to 7 M . Series resistance compensation was applied as much as possible
(50-90%). Holding potential (Vh) was
set to 70 mV if not otherwise stated. Autaptic currents were evoked
by short (400 µsec) depolarizing voltage steps from
Vh 70 to 5 mV. To measure the
current-voltage (I-V) relations of ligand-activated
currents, voltage ramps (from Vh 100 to +50 mV, 200 msec duration) were applied before, during, and after agonist
application. The net I-V relations for ligand-activated currents were obtained by digital subtraction of the ramp current in
the absence of agonist from that during agonist application. For these
experiments, voltage-activated currents were blocked by addition of 1 µM TTX, 200 µM 4-AP, 50 µM
NiCl2, and 50 µM CdCl2 to
the bath solution.
Fura-2 fluorescence measurements. To examine intracellular
Ca2+ concentration
([Ca2+]i), cells were loaded
with 5 µM fura-2 AM (Molecular Probes, Eugene, OR; stock
solution dissolved in DMSO) for 30 min in culture medium at 35.5°C.
After washing, cells were kept in normal bath solution for an
additional 15-20 min to ensure de-esterfication. Cultures were then
placed on the stage of an inverted microscope (Zeiss Axiovert) and
viewed with a 40× phase-contrast objective (Zeiss). A fluorescence
ratio-imaging system (Till Photonics, Martinsried, Germany) was used
for excitation and monitoring of fluorescence signals. Excitation
wavelength was switched between 340 nm
(F340) and 380 nm
(F380) by means of a monochromator (12 nm
bandwidth). Using a 12-bit CCD camera, fluorescence signals were
recorded after passing a dichroic beamsplitter (DCLP405) and a 510 WB40
emission filter (Omega Optical, Brattleboro, VT). Acquisition, storage,
and analysis were performed with Till Vision (vers. 3.02, Till
Photonics). Background fluorescence was measured from a region in the
immediate vicinity of the cell under investigation and subtracted.
Fluorescence ratio R
(F340/F380)
was used to describe relative changes in
[Ca2+]i without conversion to absolute
values of [Ca2+]i concentrations.
Data analysis. Whole-cell currents were digitized on-line
using a 12-bit labmaster DMA interfaced with a 586-base computer and
pClamp software (vers. 5.5; Axon Instruments, Foster City, CA) at a
sampling frequency of 8-25 kHz. Voltage-activated currents were
leak-corrected using the P/n protocol implemented in the pClamp
software. Off-line analysis was performed using the AutesP software
written by H. Zucker (NPI, Tamm, Germany) and Origin (vers. 4.1;
Microcal, Northampton, MA). Estimation of the zero current potential
(Erev) of ATP-activated currents
(IATP) was complicated because of the
strong inward rectification of IATP. Therefore,
fourth-order polynomial functions that accurately described the
inwardly rectifying I-V relationship of
IATP were fitted to individual I-V
curves. Erev was obtained by solving the roots of the polynomials. To quantify the degree of rectification present in
the I-V curves of kainic acid-activated currents
(IKA), a rectification index (RI) was
calculated as the ratio of the slope conductances at +40 and 60 mV
(Taschenberger and Grantyn, 1998a ). The slope conductance was estimated
by a linear fit to the I-V curves of IKA in the range of ±10 mV at the respective
membrane potential.
The permeability ratio PCa/PCs was
calculated from the experimentally determined
Erev in Na+-free solution
according to the constant field equation for bi-ionic conditions (Iino
et al., 1990 ): PCa/PCs = 0.25 × [Cs+]i/[Ca2+]o × exp(Erev/ ) × (1 + exp(Erev/ ) with = R × T/F = 25.42 mV (at room
temperature), where F, R, and T have
their usual thermodynamic meanings,
[Cs+]i is the Cs+
concentration in the patch pipette,
[Ca2+]o is the Ca2+
concentration in the external solution, and Erev
is the measured reversal potential in Na+-free
solution. PCa and PCs are
the permeability coefficients for Ca2+ and
Cs+, respectively.
The mean activity coefficient of CsCl and CaCl2 at 25°C
were estimated by interpolation of tabulated values and amounted to 0.724 and 0.664 for 145 mM CsCl and 20 mM
CaCl2, respectively. The calculated single ion
activities were 101.8 and 8.8 mM for Cs+
and Ca2+, respectively. Results are presented as
mean ± SEM. Statistical comparisons were made using nonparametric
tests (SPSS for Windows vers. 6.1; SPSS, Chicago, IL).
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RESULTS |
Exogenous ATP activates P2X receptor-mediated currents only
in a subpopulation of RGCs
Fast-flow application of micromolar concentrations of the P2
receptor agonist ATP elicited rapid conductance changes in a small
fraction of multipolar retinal neurons (Fig.
1). Cells were regarded as ATP-sensitive
if they generated IATP with peak amplitudes 15
pA in response to a saturating concentration of exogenous ATP (300 µM). Although much less effective, application of ADP induced inward currents as well. However, even at a concentration of 1 mM, peak amplitudes of ADP-induced currents were always
smaller than IATP elicited by 100 µM ATP (Fig. 1A).

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Figure 1.
ATP-induced ion currents in retinal neurons have a
P2 purinergic pharmacology. A-C, Whole-cell current
responses to fast-flow agonist application obtained from four different
neurons (Vh = 70 mV). In each experiment,
agonist application was followed by a washout period of at least 2 min.
Bars indicate application intervals. Agonist
concentrations are given above each bar. A, Sequential
application of the P2 receptor agonists ATP and ADP elicited rapid
conductance changes in retinal neurons. Note that despite higher
agonist concentration, ADP-induced currents were smaller than
IATP. B, Current responses to
ATP but not adenosine in another neuron. Agonist pulses of a fixed
concentration of ATP (100 µM) and two different
concentrations of adenosine (100 µM and 1 mM)
were sequentially applied at an interval of 120 sec.
IATP gradually declined on repeated
application of ATP. C, IATP
was partially antagonized by co-application of the P2 receptor
antagonist suramin (C1, 10 µM;
C2, 100 µM). The blocking action
of suramin was reversible at both concentrations as indicated by the
nearly complete recovery of IATP. Recordings
were obtained from acutely isolated RGCs. D, High-speed
agonist application (300 µM ATP) revealed rapid
activation time course of IATP followed by
slow inactivation. A rapidly inactivating current component was not
observed. E, Mean amplitudes of
IATP induced by application of saturating
concentrations (300 µM) plotted against DIV. Number of
tested ATP-sensitive cells at the given DIV is given in
parentheses. IATP increased
approximately fourfold from DIV 2 to 10.
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ATP is known to be rapidly degraded by ecto-ATPases to ADP and
eventually to adenosine (Zimmermann, 1996 ). Figure 1B
illustrates an experiment aimed at clarifying whether
IATP was activated by ATP or by its breakdown
product adenosine. In the depicted neuron, the peak amplitude of
IATP was 255.0 ± 16.8 pA, whereas
adenosine at both concentrations failed to evoke a sizable current.
Similar results were obtained in four other cells. The
nonsubtype-selective P2 receptor antagonist suramin that has been used
to distinguish P2X receptors from other ligand-gated ion channels
(Nakazawa et al., 1991 ) reversibly antagonized
IATP in a dose-dependent manner. The sensitivity
of IATP to suramin was investigated in 13 retinal neurons at DIV 0-3 (Fig. 1C). Application of 10 µM suramin reversibly reduced peak amplitudes of
IATP by 44.1 ± 1.8% (n = 5) (Fig. 1C1). Even 100 µM suramin
did not completely block IATP (68.8 ± 1.4% reduction, n = 8) (Fig.
1C2).
IATP activated rapidly and decayed quickly on
agonist removal. However, the activation and inactivation time course
of ligand-gated whole-cell currents is strongly influenced by the speed
of agonist application. We therefore measured
IATP in response to fast application of a
saturating ATP concentration (300 µM, n = 5). IATP fully activated within tens of
milliseconds, suggesting direct coupling between purinergic receptor
and ion channel (Fig. 1D). A rapidly inactivating
current component as described for IATP in a
subpopulation of sensory neurons (Cook et al., 1997 ) was not revealed.
Taken together, these results are consistent with a P2X
receptor-mediated action of exogenous ATP in a small population of
retinal neurons.
When tested between DIV 2 and 10, peak amplitudes of
IATP varied over a >100-fold range. Current
responses elicited by 300 µM ATP ranged from 27 to
3755 pA, with an average of 555 ± 46 pA (n = 171). As illustrated in Figure 1E,
IATP increased more than fourfold during the
culture period from 170 ± 31 pA to 748 ± 213 pA at DIV
2 to DIV 10, respectively.
Figure 2A-C presents
recordings from a culture that had been submitted to Thy1.1
immunostaining before whole-cell recording. IATP
was found only in a subpopulation of retinal ganglion cells (Fig.
2A, 3A-D),
whereas other RGCs (Fig. 2B) and all Thy1.1-negative amacrine cells were ATP insensitive (Fig. 2C). In five
Thy1.1-positive neurons the transmitter phenotype of ATP-sensitive
cells was tested by recording autaptic responses to short
depolarizations. With no exception, ATP-sensitive cells were identified
as glutamatergic (Fig. 2D).

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Figure 2.
Exogenous ATP exclusively excites a subpopulation
of Thy1.1-positive glutamatergic RGCs, whereas Thy1.1-negative putative
amacrine cells are ATP insensitive. Recordings from four different
cells were submitted to vital anti-Thy1.1 immunostaining before
patch-clamp recording. A, B, Recordings from two RGCs
with strong immunofluorescence, large amplitudes of
INa(V) (top row), and
repetitive discharge during depolarization under current-clamp
(middle row). Note that some RGCs generated
IATP (A, bottom row), whereas
others did not (B, bottom row). C,
Thy1.1-negative cells with small INa(V)
(top row) and spike inactivation during prolonged
depolarization (middle row) were always ATP insensitive
(C, bottom row). During agonist application, bursts of
glutamatergic EPSCs were frequently observed in both ATP-sensitive and
-insensitive cells (also see Fig. 7E). D,
ATP-sensitive cells were glutamatergic. IATP
(D1) and autaptic currents
(D2) were recorded from an RGC at DIV 17. Three
consecutive traces are shown in each panel in
D2. Autaptic currents were identified as
glutamatergic because of complete and reversible block by 20 µM DNQX. Capacitive artifacts were blanked, and
INa(V) was truncated for clarity. Bath
solution contained 3 mM Ca2+, 1 mM Mg2+ in all experiments. Addition of
50 µM bicuculline methiodide suppressed spontaneous
GABAergic synaptic currents.
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Figure 3.
ATP-activated P2X receptor channels are
exclusively expressed in RGCs. A-C, Phase-contrast
images illustrating three different ATP-sensitive RGCs after an
in vitro period of 6 hr (A, B) and 10 DIV
(C), respectively. D,
Corresponding fluorescence image of the cell shown in C.
In young cultures (DIV 0-3) RGCs were identified by a size criterion
(soma diameter >13 µm) (A, B), whereas in long-term
cultures ( DIV 4) vital anti-Thy1.1 immunostaining was applied.
E, Amplitudes of INa(V)
determined in a total of 97 multipolar cells that included 65 ATP-sensitive and 32 ATP-insensitive cells ( 7 DIV). Peak amplitudes
ranged from 0.39 nA to 24.83 nA with a mean value of 7.90 ± 0.54 nA. INa(V) was significantly larger in
ATP-sensitive compared with ATP-insensitive neurons
(p < 0.0001; Mann-Whitney test,
two-tailed). The number of tested cells is indicated. F,
If no preselection criterion was applied, the fraction of ATP-sensitive
cells was 4%. If recordings were restricted to RGCs identified after
anti-Thy1.1 immunostaining (second column) or by
size (third column), the fraction of ATP-sensitive was
65 and 67%, respectively. Above each column, the number
of ATP-sensitive cells and total number of tested neurons are in
parentheses.
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Furthermore, the peak amplitudes of INa(V) were
significantly higher in ATP-sensitive ( 10.41 ± 0.56 nA,
n = 65) compared with ATP-insensitive ( 2.82 ± 0.44 nA, n = 32) cells (p < 0.0001). This is in line with our previous observation that cultured
RGCs and amacrine cells differ largely in amplitudes of
INa(V) (Taschenberger and Grantyn, 1995 ) (Fig.
3E).
The conclusion that ATP excites RGCs but not amacrine cells was finally
also supported by comparing the fraction of ATP-sensitive neurons
within the entire population of multipolar neurons and within the RGCs
population and the population of Thy1.1-negative GABAergic amacrine
cells. As summarized in Figure 3F, only 4% of all
multipolar neurons (8 of 199) generated IATP. In
contrast, about two-thirds of the tested RGCs were ATP sensitive. The
fraction of ATP-sensitive RGCs remained unchanged during the culture
period despite the gradual decline in the total number of RGCs. All
Thy1.1-negative cells were ATP insensitive (n = 25).
Taken together, these results show that IATP is
an exclusive property of a subpopulation of RGCs.
Properties of ATP-activated ion currents in RGCs
Figure 4A
illustrates a family of ATP-induced currents at different
Vh values. IATP reversed
near 0 mV and showed a strong inward rectification. In fact, very
little outward current was measured even at Vh = 70 mV. Figure 4B presents recordings underlying the
dose-response relationship for IATP. When the
concentration of ATP was raised from 30 µM to 1 mM, current inactivation of IATP was
only slightly accelerated, although its peak amplitude nearly doubled
(Fig. 4B).

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Figure 4.
Voltage-dependence, dose-response relationship
and noise analysis of IATP in RGCs.
A, Family of ATP-induced current responses at different
Vh to illustrate strong inward rectification
of IATP. B,
IATP in response to half-effective
concentration (30 µM) and saturating concentration (1 mM) of ATP. Although the peak amplitude of
IATP nearly doubled, the time course of
inactivation was similar at both agonist concentrations.
C, Dose-response characteristics of
IATP. Pooled data from 36 cells. Current
responses were normalized to the peak amplitude evoked by 30 µM ATP. Fitting a Hill function (solid
line) to the data yielded an EC50 of ~14
µM with a Hill coefficient of ~1.
D1, Sensitivity of
IATP to changes of extracellular pH. At low
agonist concentrations, the amplitude of
IATP was strongly augmented by
acidification. This effect was fully reversible. Recordings from an
acutely isolated RGC. D2, In 13 tested RGCs,
lowering the extracellular pH by one log unit resulted in an increase
of IATP to 341 ± 62%.
E, Relation between mean current and variance of current
noise. Background noise was subtracted from test variance before
plotting. Data points were collected from 19 ATP-sensitive neurons.
Agonist concentration was 10 µM,
Vh = 70 mV. Straight line
and broken lines indicate least-square fit and 95%
confidence limits, respectively. Slope of the regression line was 0.16 pA, corresponding to a conductance of 2.3 pS. Electrodes contained
CsCl-based internal solution in A-D.
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It was difficult to obtain complete dose-response curves in individual
RGCs because in many cells IATP recovered
incompletely, particularly at higher ATP concentrations. Therefore,
only three to four different agonist concentrations were tested in most
cells. In each RGC, currents elicited by the various concentrations of ATP were normalized to the corresponding peak amplitudes of
IATP activated by 30 µM ATP. In
this way, a pooled concentration-response relationship was obtained
from a total of 36 RGCs (Fig. 4C). The data points were
fitted by a Hill function yielding an EC50 of 14.5 ± 3.1 µM with a Hill coefficient of h = 0.9 ± 0.1 (n = 36), which is consistent with a
1:1 binding of agonist to the receptor (Krishtal et al., 1983 ).
Recombinant P2X receptors show different sensitivity to changes in the
extracellular pH (Stoop et al., 1997 ). In RGCs,
IATP was strongly and reversibly augmented when
tested in acidic bath solution (Fig.
4D1). On average, current responses to 10 µM ATP amounted to 126 ± 21 pA at a pH of 7.3 and
to 335 ± 54 pA at a pH of 6.3 (n = 13) (Fig.
4D2), which corresponds to an increase of
IATP to 341 ± 62%.
Unitary conductances of recombinant P2X receptor channels differ
greatly (Evans, 1996 ). Unfortunately, we failed in our attempts to
record single-channel activity in membrane patches excised from somata
of ATP-sensitive RGCs (n = 6). Nevertheless, a rough estimate of the unitary conductance of retinal P2X receptor channels was obtained from analysis of whole-cell noise induced by application of low ( 10 µM) ATP concentrations (Fig.
4E). In the low concentration range and with the
assumption that the current noise is generated by activation of a
single-channel population with uniform conductance, the relation
between mean current (mI) and variance
(var(I)) can be described by the equation var(I) = i × mI, where
i represents the single-channel current (Anderson and
Stevens, 1973 ). The relation between mean IATP
and its variance was examined in 19 RGCs. As illustrated in Figure
4E, the current variance was almost linearly related
to the mean current with a slope of 0.16 ± 0.01 pA
(r = 0.88, p < 0.0001). Under the
assumption of Erev = 0 mV, the apparent
single-channel conductance was estimated to be 2.3 pS.
As first reported by Krishtal et al. (1983) , ATP-induced currents
desensitize quickly and recover slowly from inactivation. To determine
the time course of recovery from inactivation of IATP in RGCs, we applied test pulses of 300 µM ATP at variable intervals (ranging from 5 to 120 sec)
after control applications (Fig. 5)
(n = 8). For each RGC, the sequence of intervals
between control and test applications was randomized. Between
successive agonist applications, cells were allowed a recovery period
of 150 sec. Figure 5B summarizes pooled data from eight
different RGCs. The averaged time course of recovery from inactivation
could be approximated with a mono-exponential function yielding a time constant = 62.7 sec.

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Figure 5.
IATP recovers slowly
from desensitization. Control application of ATP (300 µM,
2 sec duration) was followed by test application after variable
intervals ranging from 10 to 120 sec. Each trial was followed by a
washout period of 2 min. A, Specimen recordings.
Application interval is indicated above each trace.
B, Pooled data from eight different cells. For each
application interval, IATP was normalized to
the respective control amplitude. Solid line indicates a
mono-exponential fit to the data yielding a time constant of
resensitization of ~60 sec.
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Heterogeneity in the inactivation kinetics and pharmacological
properties of IATP in different RGCs
During sustained agonist application, IATP
partially inactivated. There was a considerable variability in the
inactivation kinetics of IATP,
particularly in older RGCs cultured for >7 DIV. To study the
inactivation of IATP during prolonged agonist
pulses, 300 µM ATP was applied for 20 sec in a total of
27 RGCs. Figure 6A
compares current responses recorded from four different RGCs. For
comparison, scaled currents are shown superimposed in Figure 6B. In the majority of cells (n = 19)
the decay of IATP was biphasic. In these cells,
the decay of IATP was fitted with a
double-exponential function yielding a fast and a slow time constant of
fast = 1083 ± 52 msec and slow = 5498 ± 226 msec, respectively. The relative contribution of these
kinetically distinct components to IATP, however, was highly variable (Fig. 6A,B, compare
traces a, b, and c). In some RGCs the
fast inactivating component dominated (for example, Fig.
6A, trace a). In the remaining RGCs
(n = 8) only the slow component ( = 4492 ± 538 msec) was present (Fig. 6A, trace d). In
rare cases IATP did not inactivate at all (for example, Fig. 6D2).

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Figure 6.
Heterogeneous inactivation kinetics of
IATP in different ATP-sensitive RGCs.
A, Specimen recordings of
IATP from four different RGCs are depicted
to illustrate large differences in the decay kinetics of
IATP. Agonist concentration and application
interval are indicated by the bars. Calibration bar
applies to all four cells. In the majority of cells, the decay of
IATP exhibited a fast and a slow component
(traces a, b, c). However, in some cells the fast
component dominated the decay (trace a), whereas only
the slow component was present in other RGCs (trace d).
B, Superposition of the current responses illustrated in
A normalized to the same peak amplitude to facilitate
comparison. C, Fraction of
IATP remaining after 2 sec of agonist
application plotted against the peak amplitude of
IATP. Agonist concentration was 300 µM. In a majority of RGCs,
IATP inactivated within 2 sec to 25-60% of
its peak amplitude. However, in some RGCs with relatively small
IATP, the fraction of remaining
current was >70%. D, RGCs with slowly or
noninactivating current responses showed strong attenuation of
IATP by the P2 receptor antagonist suramin
(100 µM). Faster inactivation kinetics of
IATP correlated with weaker sensitivity to
suramin. In both cases, IATP recovered
almost completely after washout.
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The heterogeneous inactivation of ATP-induced currents in different
RGCs suggests a variable contribution of kinetically distinct P2X
receptor channels to IATP. For recombinant P2X
receptor channels, the inactivation time course has been described in
terms of the fraction of current remaining after prolonged ATP
application (Buell et al., 1996a ; Collo et al., 1996 ). Figure
6C illustrates the relationship between inactivation of
IATP and peak amplitudes in a total of 53 RGCs.
The degree of current inactivation was quantified as the fraction of
IATP remaining after 2 sec of agonist application (300 µM ATP). No significant correlation
between both parameters was found. In most RGCs, 40-80% of
IATP inactivated during the initial 2 sec of
agonist application; however, in some RGCs current inactivation was
<30%.
A high degree of variability was also observed in the efficacy of the
antagonist suramin to block IATP. Although fast
decaying current responses showed relatively little suramin sensitivity (Fig. 6D1), slowly or
noninactivating currents were strongly attenuated by
simultaneous application of suramin (Fig.
6D2). In nine RGCs with fast inactivating
currents, 100 µM suramin reduced
IATP to 35.2 ± 4.1% of the control
amplitude (n = 9). In contrast, in four other RGCs with
slowly inactivating currents suramin almost completely antagonized
ATP-induced currents (3.3 ± 3.3% of control).
To investigate the potency of the purinoceptor agonists ADP and
, -mATP, IATP elicited with 100 µM ATP was compared with the current amplitude induced by
100 µM ADP or 100 µM , -mATP, respectively (Fig. 7). Both agonists were
less potent than ATP. On average 38 and 70% of the ATP-induced current
response was elicited by application of ADP and , -mATP,
respectively (Fig. 7C,F). RGCs with fast decaying
IATP showed a higher sensitivity to the ATP
analogs (Fig. 7A,D) than cells with slowly inactivating currents (Fig. 7B,E). These differential actions of suramin
and ATP analogs suggest expression of multiple P2X receptor subtypes in
RGCs.

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Figure 7.
Differential action of the ATP analogs ADP and
, -mATP suggests expression of multiple subtypes of P2X receptors
in RGCs with fast inactivating and slowly or noninactivating
IATP. A, B, D, E, Specimen
recordings from four different RGCs with fast (A, D) and
slow (B, E) decay kinetics of
IATP, respectively
(Vh = 70 mV; CsCl-based pipette solution).
IATP (top panels) and current
responses to the respective analogs (bottom panels)
elicited at the same agonist concentration (100 µM) are
illustrated for comparison. C, F, Pooled data plotted as
the ratio of
IADP/IATP
and
I , -mATP/IATP
against peak amplitudes of IATP for 28 and
10 different RGCs, respectively. Note the large scattering of the data
points.
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P2X receptors couple to a nonspecific cation channel with high
Ca2+ permeability
To characterize the ion selectivity of ATP-gated P2X receptor
channels in RGCs, we recorded IATP during
voltage-ramp commands in the presence of blockers of voltage-gated
channels (Fig. 8). Reversal potentials of
IATP were obtained from the roots of polynomial functions (fourth degree order) fitted to the individual
I-V curves. Figure 8 shows the
I-V relation of IATP
determined with three different sets of ionic conditions. To
investigate the contribution of Cl to
IATP (Balachandran and Bennett, 1996 ), we varied
the chloride equilibrium potential (ECl)
by partially substituting gluconate for
Cl . Despite a shift of the calculated
ECl from near 0 mV to 39 mV, Erev
of IATP did not significantly change ( 0.1 ± 0.7 mV vs 2.3 ± 1.7 mV) (Figs. 8A,B,
10A,B), indicating that P2X receptor channels in RGCs
are impermeable for Cl .

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Figure 8.
P2X receptor channels in RGCs are impermeable to
Cl but show approximately equal permeability to
K+ and Cs+. A-C,
Ramp currents (Vh = 100-50 mV, 200 msec
duration) were recorded and digitally averaged to study the effect of
different internal solutions on the I-V
relationship of IATP. The composition of the
pipette solution, the calculated Erev
obtained from polynomials (fourth degree) fitted to individual
I-V curves, and the number of RGCs are
given on top of each diagram. Arrows
indicate the theoretical equilibrium potential for
Cl . A, With CsCl-based internal
solution, IATP reversed near 0 mV.
B, No significant shift of
Erev was observed after lowering
[Cl ]i from 145 to 30 mM
by substituting gluconate for Cl , indicating that
retinal P2X receptor channels are Cl impermeable
(compare A and B). Replacing internal
Cs+ with K+ did not affect
Erev of IATP
(compare B and C)
(p = 0.569, Friedmann test). Likewise, the
mean amplitudes of IATP were similar with
either Cs+ (D, second column)
or K+ (D, third column) as the main
internal cation (p = 0.48, Mann-Whitney
test, two-tailed), suggesting roughly equal permeability for both
cations. The degree of rectification was unaffected by the composition
of the pipette solution (compare I-V
curves in A-C).
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With K+ as the main internal cation,
voltage-activated outward currents were much larger, and consequently
estimation of Erev was more difficult. The
average value for Erev with potassium-based internal solution was 0.2 ± 2.1 mV (Fig. 8C) and
thus was similar to the values obtained with Cs-filled electrodes (Fig.
8B). This indicates that ATP activates a nonspecific
cation conductance with approximately equal permeability to
Na+, K+, and
Cs+. This conclusion is supported by the nearly
identical mean amplitudes for IATP recorded with
Cs+- or K+-filled electrodes. The
latter amounted to 547 ± 56 pA (n = 56) and
556 ± 78 pA (n = 78), respectively (Fig.
8D). The degree of rectification of the
I-V curve was unaffected by the composition of
the pipette solution (compare I-V curves in Fig.
8A-C; see also Fig. 10A,B).
To determine whether activation of P2X receptor channels is associated
with changes in the intracellular Ca2+ concentration
([Ca2+]i), we applied ATP (300 µM) to multipolar neurons loaded with fura-2 AM (Fig.
9). Again, ATP-induced
Ca2+ rises were found only in a subpopulation of
Thy1.1-positive cells (Fig. 9A-C), whereas all tested
multipolar neurons responded to elevated KCl (35 mM;
R = 0.70 ± 0.07, n = 21). We
therefore exclude impaired cell viability as an explanation for
ATP-response failures. In ATP-sensitive Thy1.1-positive RGCs, the
average Ca2+ rise elicited with 300 µM
ATP amounted to R = 0.60 ± 0.12 (n = 7).

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Figure 9.
P2X receptor channels in RGCs are highly permeable
to Ca2+. A, Ca2+
imaging experiments from two Thy1.1-positive RGCs (A, B)
and one Thy1.1-negative neuron (C) to test for
ATP-induced rise of [Ca2+]i. Cells
were loaded with the Ca2+ indicator fura-2 and
submitted to vital anti-Thy1.1 immunostaining before recording. In
imaging experiments, [Ca2+]o was 2 mM, and the external solution contained 1 µM
TTX to suppress action-potential generation. A short pulse of 300 µM ATP (15 sec duration) was followed by a washout period
of 150 sec. Thereafter, cells were depolarized by application of 35 mM KCl for a period of 15 sec. ATP-induced
Ca2+ elevations were found only in a subset of RGCs
(A, R = 0.60 ± 0.12, n = 7), whereas all tested neurons responded to
elevated KCl. For high KCl responses, R was
0.76 ± 0.19 (n = 6), 0.72 ± 0.13 (n = 7), and 0.64 ± 0.07 (n = 8) in Thy1.1-positive ATP-sensitive,
Thy1.1-positive ATP-insensitive, and Thy1.1-negative ATP-insensitive
neurons, respectively (p > 0.05, Mann-Whitney test, two-tailed). D1, ATP-induced
[Ca2+]i elevations persisted in
Na+-free solution. ATP and high KCl were applied in
control and Na+-free (Na+
substituted by NMDG+) external solution.
D2, Superposition of ATP-induced
[Ca2+]i rises in normal and
Na+-free solution recorded in another RGC. An offset
of 0.59 was subtracted from the response in Na+-free
solution. On average, R in
Na+-free solution was reduced to ~37% of the
ATP-induced [Ca2+]i rises in normal
external solution. E, IATP
recorded in Na+-free solution. External
Ca2+ was elevated tenfold compared with
A-D (Vh = 70 mV).
F, Average ramp current obtained from 10 different RGCs
to illustrate I-V relationship of
IATP in Na+-free
solution. External and pipette solution contained as the only permeant
ions 20 mM Ca2+ and 145 mM
Cs+, respectively. According to the constant field
equation, the mean value for Erev measured
under bi-ionic conditions ( 18.3 ± 5.6 mV) corresponds to a
permeability ratio
PCa/PCs of
2.2 ± 0.7.
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Although in all imaging experiments action potential generation was
blocked by TTX, it could not be excluded that ATP-induced depolarizations elicited Ca2+ influx though
voltage-activated Ca2+ channels. To eliminate a
potential contribution of ICa(V) to the
ATP-induced [Ca2+]i rise, 100 µM CdCl2 was included in the external
solution. Under these conditions, ATP-induced Ca2+
transients were reduced but still observable (50.6 ± 1.9% of the
control, n = 3; not illustrated). To record
ATP-activated Ca2+ signals in the absence of
Na+ entry-mediated depolarization, external
Na+ was replaced equimolarly by
NMDG+. External Ca2+
concentration in Na+-free bath solution was kept at
2 mM. As illustrated in Figure 9D, replacement
of extracellular Na+ by NMDG+
caused a transient increase of
[Ca2+]i, presumably because of
inhibition of the Na+/Ca2+
exchanger. Although much lower in amplitude, ATP still induced [Ca2+]i rises in
Na+-free bath solution (first and third peak in Fig.
9D1,D2). In Na+-free solution, R amounted
to 0.23 ± 0.04 (n = 5), suggesting that 39% of
the ATP-induced [Ca2+]i rise resulted
from external Ca2+ entering through P2X receptor
channels. This agrees well with the 40% reported by Mateo et al.
(1998) for cultured Purkinje neurons.
The lack of specific antagonists complicates the distinction between
metabotropic P2Y and ionotropic P2X receptor-mediated responses in
Ca2+ imaging experiments. Therefore, we sought to
directly measure Ca2+ entry through P2X channels by
recording IATP in the absence of external
Na+ (Na+ replaced by
NMDG+). In Na+- and
Ca2+-free solution, no ATP-induced inward currents
were recorded at membrane potentials down to 100 mV, indicating that
retinal P2X receptor channels are essentially impermeable to
NMDG+
(PNMDG/PCs < 0.02). To resolve IATP in
Na+-free solution, it was necessary to elevate the
external Ca2+ concentration
([Ca2+]o) to 20 mM.
Although IATP was largely reduced by
NMDG+ substitution, it was not eliminated completely
(Fig. 9E). An average I-V
relationship from 10 different RGCs tested in
Na+-free solution is illustrated in Figure
9F.
The permeability ratio
PCa/PCs was
estimated from the experimentally determined
Erev under bi-ionic conditions with
Cs+ and Ca2+ as the only permeant
ions at the intracellular and extracellular side, respectively. The
mean value of Erev ( 18.3 ± 5.6 mV) and the corresponding permeability ratio
(PCa/PCs = 2.2 ± 0.7) indicated a more than twofold higher permeability for
Ca2+ compared with Cs+ (Fig.
9F).
The expression level of Ca2+-permeable
P2X receptor channels is unrelated to the Ca2+
permeability of non-NMDA receptor channels
Non-NMDA receptor channels with a high permeability for
Ca2+ were found in a subset of postnatal rat retinal
ganglion cells (Rörig and Grantyn, 1993a ; Taschenberger and
Grantyn, 1998a ). We therefore sought to clarify whether the expression
of Ca2+-permeable P2X receptor channels in RGCs is
related to the Ca2+ permeability of their non-NMDA
receptor channels. Because Ca2+ permeability of
non-NMDA receptor channels correlated with inward rectification of
kainic acid-activated currents (IKA), we
could discriminate between RGCs expressing
Ca2+-permeable (RI <1, type II) and
Ca2+-impermeable (RI >1, type I) non-NMDA receptor
channels by investigating their I-V
characteristics (Taschenberger and Grantyn, 1998a ).
Recording of IATP and IKa
was performed in 31 ATP-sensitive RGCs using agonist concentrations of
100 µM for both ATP and kainic acid. Amplitudes of
IATP at Vh = 70 mV and
RIs of IKA were obtained from the corresponding
I-V curves. It was found that
IATP was elicited in type II (Fig.
10A) as well as in
type I RGCs (Fig. 10B). Amplitudes of
IATP and also the shapes of
I-V curves were similar in both types of RGCs.
Figure 10C shows the relationship between
IATP and RIs of IKA.
Although we noted a small tendency for type II RGCs to generate larger
IATP, a significant correlation was not
observed (p = 0.449). Thus, the level of P2X
receptor channel expression was unrelated to the
Ca2+ permeability of non-NMDA receptor channels.

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Figure 10.
In RGCs, P2X receptor channels do not
preferentially colocalize with Ca2+-permeable
(A, type II RGCs) or
Ca2+-impermeable (B, type
I RGCs) non-NMDA receptor channels. A, B, Ramp
currents during application of kainic acid (100 µM,
top panel) and ATP (100 µM,
bottom panel) from two different RGCs after 24 hr
in culture. RGCs expressing Ca2+-permeable non-NMDA
channels and RGCs with Ca2+-impermeable non-NMDA
channels were distinguished according to the rectification of
IKA. Note that
IATP was recorded in both type II and type I
RGCs. C, Pooled data from a total of 31 RGCs. Peak
amplitudes of IATP were plotted against RIs
of IKA. Solid and
broken lines indicate linear regression and 95%
confidence limits, respectively. No significant correlation was found
between RIs of IKA and amplitudes of
IATP.
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DISCUSSION |
This is the first description of an ATP-activated ion channel in
retinal neurons. We show that exogenous ATP excited the majority of
cultured retinal ganglion cells but none of the putative amacrine cells. In RGCs, activation of P2X purinoceptors induced inwardly rectifying whole-cell currents and intracellular
Ca2+ signals. IATP was also
induced by ADP and , -mATP but not by adenosine. The purinoceptor
antagonist suramin attenuated IATP in a
dose-dependent manner. Retinal P2X receptors coupled to nonspecific cation channels with a high permeability for Ca2+.
Our results point to an important role of ATP as an extracellular messenger that contributes to Ca2+ signaling in RGCs.
Identification of ATP-sensitive cells
Our conclusion that P2X receptors are selectively expressed in a
subpopulation of RGCs crucially relies on an unambiguous cell-type
identification in dissociated neuronal cultures. Our experiments were
restricted to large multipolar, neurite-bearing cells that generated
INa(V). This excluded the possibility that ATP-induced responses were recorded from photoreceptors, bipolar neurons, or non-neuronal cells. That ATP-sensitive neurons were, in
fact, RGCs was concluded on the basis of the following identification criteria. (1) Among short-term cultured neurons, ATP-sensitive cells
represented the largest cells, with a soma diameter always >13 µm.
(2) ATP-sensitive cells were without exception Thy1.1 positive. (3) In
addition, neurons with IATP also generated large voltage-activated Na+ currents and were able to
discharge repetitively on depolarization. (4) Finally, and most
compelling, ATP-sensitive neurons were glutamatergic, as demonstrated
by recording autaptic glutamatergic currents. In contrast, all
Thy1.1-negative cells proved to be ATP insensitive. Because the
Thy1.1-negative ATP-insensitive neurons had smaller INa(V) and lacked the capacity to generate
repetitive spike trains, we concluded that these cells were amacrine
cells. Thus, sensitivity to ATP may serve as another criterion
to distinguish RGCs from putative amacrine cells in dissociated cell culture.
P2X receptor subtypes in the retina
Previous studies suggested that retinal cells express the
purinoceptor subtypes P2X2-5 but not P2X1 or P2X6 (Brändle et
al., 1998 ). Comparison of our results with the properties of
IATP in other preparations gave first
indications of which receptor subtypes could mediate
IATP in RGCs.
ATP-gated channels of the P2X7 receptor subtype are responsible for
ATP-mediated lysis of antigen-presenting cells through the formation of
large membrane pores. These pores are readily permeable to organic
cations such as NMDG+ and may provide a mechanism of
transmitter-induced cell death (Surprenant et al., 1996 ). This
possibility could be considered as a mechanism contributing to the
regulated cell death of RGCs during ontogenesis (Beazley et al., 1987 ).
However, recombinant P2X7 receptors are relatively insensitive to the
antagonist suramin (Surprenant et al., 1996 ), and retinal ATP-activated
channels are essentially impermeable to NMDG+, which
makes a contribution of the P2X7 purinoceptor subtype to
IATP in RGCs unlikely.
Recombinant homomeric P2X4 and P2X6 receptors are not activated by
, -mATP and share the unique pharmacological characteristic of
being completely insensitive to suramin (up to 300 µM)
(Bo et al., 1995 ; Buell et al., 1996b ; Collo et al., 1996 ; Soto
et al., 1996 ). In most RGCs, however, , -mATP was a potent
agonist, and IATP was sensitive to suramin,
excluding the possibility that a major fraction of
IATP was mediated by homomeric P2X4 and P2X6 receptors. Heteromeric P2X4+6 receptors are suramin sensitive, but in
contrast to IATP in RGCs, acidification of the
extracellular solution resulted in a reduction of the ATP-induced
currents (Lê et al., 1998 ).
Homomeric P2X1 purinoceptors channels are activated by ADP, ATP, and
, -mATP (Valera et al., 1994 ). However, these channels are
characterized by a large unitary conductance (18-19 pS) and completely
blocked by low concentrations of suramin (Valera et al., 1994 ; Evans,
1996 ). In addition, homomeric P2X1 receptors expressed in
Xenopus oocytes were activated by submicromolar
concentrations of ATP (Valera et al., 1994 ). The estimated
EC50 was more than one order of magnitude lower than in
RGCs. Furthermore, complete desensitization of recombinant P2X1
purinoceptors occurs on a millisecond time scale (Lewis et al., 1995 ).
It is thus unlikely that the P2X receptors in RGCs belong to the P2X1 subtype.
In a minority of RGCs, the properties of IATP
corresponded to the characteristics described for homomeric P2X2 or
P2X5 receptor channels. These purinoceptor subtypes are antagonized by
suramin, are relatively insensitive to , -mATP and desensitize
only negligibly (Brake et al., 1994 ; Collo et al., 1996 ; Garcia-Guzman
et al., 1996 ).
Although the pharmacological properties of IATP
were compatible with an expression of the P2X3 purinoceptor in RGCs, it
is conceivable that retinal ATP-gated channels are P2X2+3 heteromers. Homomeric P2X3 receptors desensitize on a millisecond time scale (Chen
et al., 1995 ; Lewis et al., 1995 ). Heterologous expression of P2X2 and
P2X3 receptors gave rise to functional properties not found in the
respective homomeric receptors, e.g., slowly desensitizing currents
that were activated by , -mATP (Lewis et al., 1995 ). Among native
P2X receptor channels, rapidly desensitizing ATP-induced currents were
recorded in a subset of nociceptive neurons in the trigeminal ganglia
(Cook et al., 1997 ) but not in nodose (Lewis et al., 1995 ) or dorsal
root ganglion cells (Bean, 1990 ). The kinetic properties of
IATP in RGCs resembled those of dorsal root
ganglion cells (Krishtal et al., 1983 ; Bean, 1990 ), e.g., inactivation
and recovery from inactivation were in the range of seconds and
minutes, respectively. The values for the EC50 and the Hill
coefficient in RGCs were also similar to those of rat sensory neurons
(Krishtal et al., 1983 ). Hill slopes larger than unity were reported,
however, for bullfrog dorsal root ganglion cells (Bean, 1990 ).
Single-channel events of native P2X receptors in DRGs were brief and
flickery (Bean et al., 1990 ). Such brief openings could account for our
inability to resolve single-channel events in outside-out patches from
RGCs. Our estimate for the apparent single-channel conductance of P2X
receptor channels in RGCs was lower than the values reported previously
for dorsal root ganglion cells (Bean et al., 1990 ). However, in
that study a membrane potential of 100 mV was applied, and the
slope conductance of IATP in RGCs at
Vh = 100 mV was almost twice as large
compared with Vh = 70 mV.
The kinetic properties of IATP may be influenced
by manipulating the external Ca2+ and
Na+ concentrations. In bullfrog DRG neurons, the
deactivation of IATP was accelerated with higher
[Ca2+]o (Bean, 1990 ). In rat nucleus
solitarii neurons, high external Ca2+ accelerated
the inactivation of IATP (Ueno et al., 1992 ).
Desensitization through a calcium-dependent calcineurin-mediated
mechanism has recently been suggested for recombinant P2X3 receptor
channels (King et al., 1997 ). Because retinal P2X receptor channels are Ca2+ permeable, heterogeneous inactivation kinetics
of IATP during sustained agonist application
thus may be related to peculiarities in the regulation of
[Ca2+]i in individual RGCs rather than
to the expression of different P2X subtypes. Our estimate for the
relative Ca2+ permeability
PCa/PCs of retinal
P2X receptor channels is similar to previously reported values for
PCa/PNa of
recombinant heteromeric P2X2+3 channels (Virginio et al., 1998 ), taking
into account a PCs/PNa = 0.72 (Evans et al., 1996 ).
Possible role of P2X receptor channels in RGC
The physiological role of P2X receptor channels in RGCs is largely
unknown. Our results indicate that ATP can act as an excitatory neurotransmitter or neuromodulator on retinal ganglion cells and thereby influence visual information processing in the inner retina. In
the developing ferret retina, cholinergic transmission is required for
the propagation of spontaneous excitation waves in the ganglion cell
layer (Feller et al., 1996 ). An attractive, yet at present speculative,
hypothesis is that ATP is co-released with acetylcholine from starburst
amacrine cells and contributes to the generation of
Ca2+ waves in the inner retina by activation of P2X
receptors in RGCs. It is unlikely, however, that ATP alone serves as a
fast excitatory neurotransmitter in an amacrine-ganglion cell synapse,
because in retinal whole mounts from the postnatal rat, excitatory
synaptic activity in the ganglion cell layer was completely abolished
after addition of the glutamate receptor antagonist DNQX (Rörig
and Grantyn, 1993b ).
Together with previous studies (Aizenman et al., 1988 ; Rörig and
Grantyn, 1993a ; Taschenberger and Grantyn, 1998a ), our present results
demonstrate that postnatal rat RGCs express several types of
ligand-gated ion channels with a high permeability for
Ca2+. ATP-activated P2X receptor channels may
represent a particularly important pathway for external
Ca2+ entry in RGCs, not only because of their high
PCa/PCs but also because of their inwardly rectifying I-V
relationship. In contrast to NMDA receptor channels, P2X receptor
channels thus mediate the largest Ca2+ influx at
resting or hyperpolarized potentials when the driving force for
Ca2+ is high.
 |
FOOTNOTES |
Received Dec. 9, 1998; revised Feb. 16, 1999; accepted Feb. 17, 1999.
This work was supported by the Deutsche Forschungsgemeinschaft (SFB
515). We thank A. Draguhn and W. Müller for helpful discussion and critically reading an earlier version of this manuscript. The
technical assistance of Mrs. K. Przezdziecki is gratefully acknowledged.
Correspondence should be addressed to Dr. H. Taschenberger: Vollum
Institute, Oregon Health Sciences University L-474, 3181 S.W. Sam
Jackson Park Road, Portland, OR 97201.
 |
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