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* Department of Biomedical Engineering, Neuroscience Graduate Program, and Center For Visual Science and Technology, University of Southern California, Los Angeles, California; and
Department of Anatomy and Neurobiology, Boston University School of Medicine, Boston, Massachusetts
Correspondence: Address reprint requests to Norberto M. Grzywacz, Tel.: 213-821-1150; E-mail: nmg{at}bmsr.usc.edu.
| ABSTRACT |
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| INTRODUCTION |
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-aminobutyric acid (GABA), releasing them upon light stimulation (5
In this article, we use a biophysical model to test the feasibility of the GABAB-autoreceptor hypothesis for Starburst cells. To know whether this hypothesis will work is not so easy. One difficulty is to know how GABAB agonists reduce the muscarinic input to the glycinergic cell at the same time that they increase the overall release of ACh. Perhaps the answer lies in the recent surprising finding that only
25% of Starburst-cell varicosities contain GABAB receptors (22
). If the input to glycinergic cells came only from these varicosities, then GABAB agonists might affect these cells without reducing ACh release from other varicosities. However, the model must solve another problem with GABAergic action on Starburst cells. The release of ACh from Starburst cells may be also inhibited by GABA through GABAA receptors (8
,16
,39
,40
). How is it that the GABA that putatively feeds back to the GABAB autoreceptor does not inhibit the ACh release through the GABAA heteroreceptor? The model provides answers to these questions and fits the Neal and Cunningham data well. An abstract version of the model appeared elsewhere (41
).
The next section of this article will provide the model assumptions and their justifications, along with a physical description of the model. That section will include no equations to facilitate the comprehension of the ideas. The model equations and the parameters used in the simulations will appear in Appendices A and B, respectively.
| MODEL |
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25% of Starburst-cell varicosities (22
Because GABAB receptors are proximal in the model, the synapse to the glycinergic cell must also be proximal. From the data of Neal and Cunningham (5
) and Zucker et al. (22
), we assume that this synapse is muscarinic. (One could also use nicotinic and GABAA synapses, but this would make the model unnecessarily complex.) Furthermore, it is postulated that GABA is released in a Ca2+-independent manner (48
50
) by the proximal dendritic compartment and feeds back onto it. This assumption is not completely realistic, because some GABA release from Starburst cells is Ca2+ dependent (51
). However, in varicosities with GABAB receptors, their action suppresses Ca2+-dependent release of GABA. Consequently, such a release would only occur early in the response, that is, before GABAB action begins. Because the stimulus' period (333 ms; see Appendix B) is much slower than most synapses, any Ca2+-dependent release would occur during a negligible portion of the response in the proximal compartment of the model. Nevertheless, such a release could happen in the distal compartment, making the model still compatible with the data of Zheng et al. (51
). Thus, for simplicity, we only included Ca2+-independent release of GABA in the proximal compartment.
The activation of the GABAB autoreceptor would reduce the gain of the muscarinic synapse by lowering the influx of Ca2+ into the presynaptic site (28
30
). Hence, the glycinergic cell and its synapse would be less active and thus inhibit less the Starburst cell (Fig. 1). (Alternatively, the glycinergic cell could inhibit the bipolar-cell input onto the Starburst amacrine cell (37
).) This disinhibition would increase the release of ACh. How is it possible for the ACh release to increase at the same time that the muscarinic synapse is becoming weaker? Again, since GABAB receptors exist only proximally in the model, one can answer this question if one postulates that there is distal cholinergic release. What one needs is for the distal release to dominate the overall release. Therefore, even though the ACh release that activates muscarinic receptors falls, the total release may increase. Fortunately, there is evidence that Starburst dendrites normally release ACh onto ganglion-cells' nicotinic receptors (7
,52
56
).
Bipolar cells making glutamatergic synapses are the beginning of the model's excitatory pathway. These cells receive the visual input (not shown in Fig. 1), and synapse onto the Starburst and the GABAergic amacrine cells. In turn, the GABAergic cells feed the bipolar inputs and the distal dendrites of the Starburst cells. There is evidence for a GABAergic feedback onto the bipolar cells feeding the Starburst cell (57
). The GABAergic synapse onto the bipolar cells could be through GABAA (58
61
) or GABAC (59
,62
64
) receptors. In this article, we will assume for simplicity that the GABAergic synapses onto bipolar and distal Starburst dendrites are identical.
| METHODS |
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All the solutions of the equations used the same parameters, which appear in Appendix B. With one exception (explained below), we did not attempt to optimize parameters finely, but only to capture the data qualitatively. Several parameters were around values estimated from the literature. We used parameters as close as possible to the cells of interest, but sometimes, the only ones we could find were not even for the retina. We used them anyway, as they at least constrained our simulations to realistic values.
Parameters estimated from the literature were as follows: We used a specific membrane-capacitance value of 1 µF/cm2. This was close to the value measured for bipolar, amacrine, and ganglion cells of mudpuppy and tiger-salamander retinas (66
). In turn, for membrane time constants, we used characteristic vertebrate-neuron values of 1020 ms (but see (66
)). These values came, for example, from the Guinea-pig's hippocampal neurons (67
), and from the cat's spinal motoneurons (68
) and sensory-motor-cortex cells (69
). Values for resting potentials were 50 mV, as recorded in the turtle's amacrine cells (70
). Amacrine-cell soma diameters were between 5 and 10 µm, as in the cat's AII amacrine cells (71
), the primate's Starburst amacrine cells (72
), and the pigeon's amacrine cells (73
). GABAA and glycinergic reversal potentials were typical for the retina by being between 60 and 50 mV. For instance, studies on GABAA and glycinergic synapses were performed respectively with the turtle's cone photoreceptors (74
) and the tiger salamander's amacrine cells (75
). In turn, muscarinic receptors reversed at
0 mV in most vertebrate tissues. The information on these receptors came, for example, from the bullfrog's sympathetic ganglia (76
), the Guinea-pig's smooth muscles (77
), and the bovine ciliary muscle cells (78
). Finally, we set glutamatergic receptors to reverse at 20 mV, as for the Guinea-pig's laterodorsal tegmental neurons (79
).
Different from these parameters, we had no good experimental basis to select other synaptic parameters. For instance, maximal synaptic conductances for our simulations would depend on light-stimulus properties, such as intensity. Such conductances had not been measured in conditions similar to those that we were trying to simulate. Hence, we selected these conductances based on the resting conductances of the membrane. The maximal glutamatergic conductance was the same as the resting conductance of the cellular compartments. Our rationale was that much smaller glutamatergic conductances would depolarize the cell too little, whereas much larger ones would saturate it. Similar considerations were used for the muscarinic conductance. In contrast, the glycinergic conductance was four times stronger than the resting conductance to produce shunting inhibition (with a similar rationale applying to the GABAA synapse). We tested the robustness of our results with these conductance choices by varying each of them individually by 25% up or down. Our fits remained inside the range of the experimental values (Figs. 6 and 8) despite these variations.
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| RESULTS |
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Control
The first things to consider, in understanding the model's behavior, are the potentials in control conditions in the various compartments. The most-central compartments for this understanding are those of the Starburst amacrine cell. In Fig. 2, we show the potentials in this cell's soma and distal dendritic compartment (Fig. 1) in response to a full-field square-wave modulation. Appropriately, the response is periodic. As seen in Fig. 2 A, the response reaches equilibrium essentially during the first cycle. Fig. 2 B shows the voltage's details in one of the cycles. Not surprisingly, there is much voltage attenuation from the distal dendrite to the soma. In addition, the voltage waveforms are complex, showing two peaks during the cycle. The reason for these peaks will be understood when we consider the glycinergic input to the Starburst cell.
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Bicuculline
Neal and Cunningham also used bicuculline, a GABAA antagonist, in addition to baclofen and strychnine. Fig. 7 shows how the model reacts to bicuculline and to its combination with baclofen. Bicuculline causes a relatively small increase in the Starburst potential without eliminating its two peaks (Fig. 7 A). This increase follows an increase in the bipolar input to the Starburst cell. Furthermore, the increase in Starburst potential follows a reduction of the inhibition in this cell's distal dendritic compartment (Fig. 1). As a result of this increase in potential, the cholinergic release also undergoes a small augmentation (Fig. 7 B). The increase in potential is much more dramatic when one adds baclofen to the bicuculline (Fig. 7 A). Comparison of Figs. 4 and 7 reveals that the combination of bicuculline and baclofen causes a larger increase in potential than with each drug in isolation. This dramatically increased potential leads to a boosted release of ACh (though the boost seems to be in the duration of the release and not in its total amplitude).
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| DISCUSSION |
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Limitations of the model
The main limitations of the model are due to the simplicity of its components. Perhaps its main simplifying feature is its segregation of GABAergic receptors, and of ACh release that activates nicotinic and muscarinic receptors into different dendritic compartments of the Starburst cell. We already discussed the rationale and limitations of this segregation assumption in Model. In Experimental Predictions, we will address some of the consequences of segregation.
To make the model more realistic, one would have to include better morphological structure for all cells (Fig. 1). In addition, one would have to use synaptic mechanisms and inputs to bipolar cells that are more realistic (Appendix A). A benefit of using realistic morphology for the Starburst cell would have been an assessment of the spatial-separation requirements for this cell's synaptic inputs and outputs. The details of this cell's response dynamics would also change, but we do not believe that the main conclusions would be modified (Model). The synapses are modeled without dynamicsthat is, assuming that they are sufficiently fast to be in quasi steady state. This is probably true, since the stimulus' period (333 ms; see Appendix B) is much slower than most synapses. However, this may not apply to the GABAB synapse, since it may depend on a G-Protein second-messenger pathway (30
32
). If we were to slow down this synapse in the model, the dynamics of the responses would change and the autoreceptor control may lose its effectiveness at high temporal frequencies. The stimulus' slowness is also our justification for disregarding the dynamics of the input to the bipolar cell (Appendix A). However, it would have been better not to neglect these dynamics if we wanted to predict the results of faster experiments. Moreover, the model input to the bipolar cell neglected surround-inhibition from horizontal cells. This hampers the ability to make predictions on the effect of spatial frequency. If spatial frequency were of interest, then one would have to include a richer spatial representation of the inputs. Because the stimuli are full-field square-waves (Methods), there is no need to worry about spatial frequency. For these stimuli, surround-inhibition only reduces the bipolar-cell gain.
Functional roles
The roles of several components of the model have been discussed elsewhere. For instance, the role of the GABAergic input to the bipolar cells may be to give the retina a degree of transience (81
83
). In turn, one role of the GABAergic input to the distal dendrites of the Starburst cell may be to contribute to directional selectivity ((16
,84
); but see (85
)). What could be the role of the GABAB-controlled glycinergic feedback loop to the Starburst cell? We propose that this loop could work to make the sensitivity of ACh release in response to motion larger than those in response to other stimuli. Acetylcholine has been proposed to be involved in the enhancement of retinal motion sensitivity (10
12
) and in preferred-direction facilitation in directionally selective cells (10
,86
,87
). Here is how we think of the GABAB-receptor involvement in these motion functions. If one suddenly delivers a no-motion stimulus to the Starburst cell, then the GABAB action on the muscarinic synapse may not have time to react. This is because a slow G-protein second-messenger system may mediate this action (30
32
). Without this action, muscarinic activation of the glycinergic cell can occur and thus, there is inhibitory feedback onto the Starburst cell (Fig. 1). If instead of sudden stimuli, a sufficiently slow motion sweeps through the Starburst cell, then a different set of events take place. Consider a motion sweeping from left to right in Fig. 1. The left bipolar cells will be the first to be made active, depolarizing the Starburst cell. This depolarization would start the GABAB loops (synapses labeled 6 in Fig. 1) even before the motion reaches the right bipolar cells. In this case, when the motion finally reaches them, the ACh release that activates muscarinic receptors to the glycinergic cell is truncated, eliminating the glycinergic feedback onto the Starburst cell.
To illustrate these predictions of the model, we added an artificial constant delay to the GABAB synapse (Eq. A4 in Appendix A). Furthermore, we activated the bipolar cells sequentially to simulate motion. These cells were still activated by a 3-Hz square-wave (Eq. A1). However, the cycle of any given bipolar cell started after that of the neighbor to its left by a preset delay. For example, in Fig. 9 A, this delay was 100 ms, implying an edge motion sweeping the Starburst cell in 400 ms from left to right. The figure shows the response as recorded on the right distal dendritic compartment. As predicted, the response to the motion was larger than the response to the full-field stimulation (Fig. 9 A). With this delay and this motion, the facilitation of the amplitude of response above resting potential was 84.1%. Without the GABAB delay, facilitation disappeared (only 7.6% for this motion and negative for other motions). However, although the GABAB delay had effects on the details of the responses, it did not affect the qualitative effects of the various pharmacological drugs described earlier in the article. Even with this delay, baclofen and strychnine still increased the response (compare Fig. 9 B with the solid line of Fig. 9 A). Bicuculline alone did not have a major effect on the response (compare Fig. 9, A and B). But bicuculline augmented the effect of baclofen (Fig. 9 B). These results with baclofen, strychnine, and bicuculline were similar to those in Figs. 48![]()
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Experimental predictions
One novel aspect of the model is the proposal that GABAB receptors work as autoreceptors in the Starburst cell. There are many experiments in the literature trying to prove that particular receptors work as autoreceptors (23
25
). For the most part, these experiments try to investigate whether a cell containing a particular transmitter responds to that transmitter. It is known that Starburst cells respond to GABA, but no current or voltage responses to baclofen have been observed (39
). However, we propose that baclofen has an effect on the muscarinic synapse without affecting particular conductances. An ideal experiment would measure baclofen's effect on ACh's release from Starburst cells synaptically isolated from the rest of the retina. One could attempt to isolate the Starburst cells synaptically by using low-Ca2+ media. Unfortunately, this condition would also shut down these cells' synapses, eliminating ACh release. Alternatively, one could use a cell culture to try to isolate the cholinergic Starburst cell. An experiment that is more feasible is to study whether the effect of baclofen on cholinergic and glycinergic releases is interrupted by drugs that interfere with G-protein pathways. This would not prove the existence of autoreceptors, but would provide circumstantial evidence for them as they tend to work through such proteins (30
32
).
Another novel aspect of the model is that different types of GABAergic receptors may have different distributions across the Starburst cell's dendritic tree. Indirect evidence is now available for such different distributions of receptors (see Model for detailed arguments). The same differences should apply for cholinergic synapses. A test for such different distributions would be to use antibodies against these receptors and synapses in an identified Starburst cell. One could then check microscopically whether there are different distributions of immunoreactivity with the different antibodies. If such differences exist, then they would raise the possibility that the Starburst dendrite has more functionality than previously thought. Some studies propose that this cell's dendritic branches may function as independent electrotonic subunits (16
,84
,85
,88
). If different receptors and synapses have different distributions in the dendritic tree, then this may allow different portions of a dendritic branch to have different roles in information processing.
| APPENDIX A: EQUATIONS |
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Light stimuli
With the exception of the motion described in the Discussion, the light stimuli used in the simulations paralleled those used by Neal and Cunningham (5
). Here, we will discuss the model only in the context of their stimuli. We used full-field square-wave stimulation,
![]() | (1) |
Biophysical notation
Because the stimulus is full field, all the bipolar compartments in Fig. 1 respond alike. The same holds for the GABAergic compartments, glycinergic compartments, the two proximal dendritic compartments of the Starburst cell, and its two distal compartments. In this Appendix, we will denote a compartment by the subindex c. This subindex can attain the values of b,
, g, s, p, and d for the bipolar, GABAergic, and glycinergic cells, soma of the Starburst cell, and its proximal and distal compartments, respectively. (Although the simulations do not include the ganglion cell, its subindex will be gc for simplifying the notation below.) Besides cells and compartments, release of neurotransmitters is identical for several different synapses containing the same transmitter. We will denote a neurotransmitter by the subindex n. This subindex can attain the values of gu for glutamate,
a for GABA released from GABAergic cells toward GABAA receptors, gy for glycine,
b for GABA released onto GABAB autoreceptors, and mu and ni for ACh released onto muscarinic and nicotinic receptors, respectively.
This article models the cellular compartments through standard cable-theory assumptions (89
). The most important variable in this model is the compartment's potential (voltage), Vc(t). A compartment's potential causes transmitter release, which is denoted by
with c1 and c2 being the pre- and postsynaptic compartments, respectively. For instance, Rp, mu, g is the ACh release that activates muscarinic receptors from the proximal dendritic compartment of the Starburst cell onto the glycinergic cell. In turn, neurotransmitter release causes the activation of a membranous postsynaptic conductance, whose symbol is
Besides synaptic conductances, between any two neighbor compartments of the Starburst cell, there is an axial conductance
And all the model's compartments also have resting conductances, which we denote gc, r, c.
We denote by Ix,y,c the current flowing through the conductance gx,y,c into compartment c. To calculate this current, one needs the compartment's voltage (Vc(t)) and the conductance's reversal potential, Ey,c. The axial-conductance current flowing from compartment c1 to compartment c is
From the axial and membranous currents, one can calculate the temporal evolution of the voltage at the compartment if one has its capacitance Cc. This capacitance and resting conductance were computed from the multiplication of the compartment's membranous area (Ac) by their specific values, denoted
and
respectively.
Synapses
All synapses in the model, except for the GABAB synapse, respond conventionally to presynaptic voltage. We model conventional synapses as if they are not the temporal bottlenecks of the system. The sigmoidal pre-synaptic-to-transmitter relationship in the model conventional synapses follows the steady-state input-output curves found experimentally (90
,91
). This relationship is
![]() | (2) |
is the synapse's gain,
n > 0 is the slope of the synapse's input-output relationship, and
n is the synaptic threshold. Without loss of generality, one can set the post-synaptic conductance equals to release, since
could be made to have units of conductance:
![]() | (3) |
In Appendix B we express
with such units.
The GABAB synapse responds differently to presynaptic voltage than conventional synapses, since this synapse does not induce, directly, a conductance change (see Model). Instead, this synapse reduces the presynaptic Ca2+ conductance in the muscarinic synapse to the glycinergic cell. As a result, this synapse's gain falls. We model this fall by letting ßmu, g depend on the locally released GABA,
![]() | (4) |
is the gain of the muscarinic synapse when the GABAB receptors are not activated. (This equation assumes that the Starburst-cell release of GABA has the same dependence on presynaptic voltage as other releases (i.e., Eq. 2). This assumption cannot be, strictly speaking, correct. This is because we assume that this release is Ca2+ independent and thus not affected by the activation of the autoreceptors. The use of Eq. A2 is only justified for the sake of model simplicity, since there are no good models of Ca2+-independent release.) Such a model must be taken as a simple abstraction of the complicated G-protein-dependent mechanism by which the GABAB autoreceptors work (30
Currents and potentials
This section describes how we calculate the voltages across the membranes of the different cellular compartments. This calculation is identical in all compartments except for the bipolar cells. The currents flowing through synaptic or resting conductances depend on the voltage at nonbipolar compartments and on the conductances' reversal potentials. These currents are
![]() | (5) |
The current flowing into compartment c from a compartment c1 through an axial conductance is
![]() | (6) |
From these currents, the potential in the nonbipolar compartment follows
![]() | (7) |
The bipolar cells are special cases among all compartments, because one of its inputs does not come from synapses but directly from light. We model this input as a current being injected onto the bipolar compartment. In addition, this compartment receives a GABAergic current and has a resting-conductance current (Fig. 1), making Nb = 3 in Eq. A7. For simplicity, the stimulus current is exactly S(t) (Eq. A1). This means that the simulations neglect the temporal properties of the photoreceptors feeding the bipolar cells, that is, they consider the input's dynamic sufficiently slow. For the same reason, the simulations assume that the bipolar compartment has zero capacitance, that is, Cb = 0. With these assumptions, one can set the left-hand side of Eq. A7 to 0 and use Eq. A5 to get
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a, b(t) obeys Eq. 3. This voltage is then fed to the bipolar synapse, whose glutamatergic release is governed by Eq. 2. | APPENDIX B: PARAMETERS |
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Stimulus parameters
The three parameters of the stimulus (Eq. 1) were a = 8 pA, f = 3 Hz, and d = 0.25.
Synaptic parameters
We present the synaptic parameters (Eqs. 25) in six subsets: glutamatergic, GABAA, glycinergic, GABAB, muscarinic, and nicotinic synapses.
Glutamatergic synapses
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GABAA synapses
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Glycinergic synapses
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GABAB synapses
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Muscarinic synapses
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Nicotinic synapses
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The only exception is that
pS for the central glycinergic cell, so its total muscarinic input is equal to the other glycinergic cells in the full-field experiments.
Cellular parameters
Three cellular parameters (Eqs. 57) were identical for all compartments: the specific membrane capacitance (
=1 µF/cm2), the resting potential (Er, c = 50 mV), and the axial conductance (
pS). The rest of parameters are organized in two sets: compartmental membranous areas and specific resting conductances.
Compartmental membranous areas
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Specific resting conductances
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Pharmacology parameters
The simulations of the pharmacology were performed by setting the appropriate parameters to zero when a particular drug was used. We present the pharmacology parameters in three subsets: baclofen, strychnine, and bicuculline.
Baclofen
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Strychnine
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Bicuculline
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| ACKNOWLEDGEMENTS |
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This work was supported by National Eye Institute grants No. EY08921 and No. EY11170 to N.M.G., and by National Eye Institute grant No. EY07552 to C.L.Z.
Submitted on August 8, 2005; accepted for publication April 10, 2006.
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