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Correspondence to Mikko Juusola: m.juusola{at}sheffield.ac.uk
 TOP ABSTRACT INTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONREFERENCES |
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INTRODUCTION |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONREFERENCES |
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; Sterling, 1983; Meinertzhagen, 1993; Juusola et al., 1996; Wässle, 2004). Ultrastructural studies and neurochemistry have shown a complex arrangement of feedforward and feedback synapses that use a diverse array of excitatory and inhibitory transmitters. However, the understanding of this sophistication has been limited at best, in part because monitoring activity in vivo and asserting functions for individual parts of the network is very difficult.
To further our understanding of feedback synapses in visual processing, we have turned to a Drosophila preparation, whose genetics and modular eye morphology (Meinertzhagen and Sorra, 2001) offer clear advantages (Fig. 1 A). The ultrastructure of the first visual synaptic layer in Drosophila (Fig. 1 B) has been fully described from electron-micrograph sections (Meinertzhagen and O'Neil, 1991). The first optic neuropile, the lamina, is an assembly of stereotyped cartridges, neuro-ommatidia, where axon terminals of photoreceptors (R1–R6, one from each of six neighboring ommatidia) each make 
50 output synapses known as tetrad synapses (Meinertzhagen and O'Neil, 1991), a total of 283 in one complete reconstruction (Meinertzhagen and Sorra, 2001). Each of these contacts (Fig. 1 B, a) releases histamine (Hardie, 1989a; Gengs et al., 2002) onto two large monopolar cells (LMCs) and onto a fingerlike process of an amacrine cell, AC, that runs between two photoreceptor axons (Fig. 1 B). AC processes are linked together and to adjacent cartridges with thin extending fibers (Campos-Ortega and Strausfeld, 1973; Fischbach and Dittrich, 1989), suggesting that each process could be a locally interacting element, which may see only limited activity from other such segments in the same or neighboring cartridges (Shaw, 1984). In return, photoreceptor axons receive feedback from the primary visual interneurons (Meinertzhagen and Sorra, 2001): a total of 48 synapses from the ACs (Fig. 1 B, b) and 25 from LMCs (Fig. 1 B, c) (Meinertzhagen and Sorra, 2001). Although these are the only direct feedback connections to photoreceptor terminals, photoreceptor output may also be influenced indirectly via LMCs that receive lateral (L4) and centrifugal feedback from other cartridges (Fig. 1 B, D) and from higher processing centers (Fig. 1 B, e), respectively.
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We use three specific mutants to work out the feedback dynamics: ortP306, ebony, and temperature-sensitive shibireTS1. According to in vitro experiments, LMCs of ortP306 have reduced sensitivity for histamine (Gengs et al., 2002), whereas ebony has impaired histamine recycling that reduces the available transmitter pool in photoreceptor axon terminals (Borycz et al., 2002). Both of these mutants should therefore reduce the probability for successful synaptic transmission from photoreceptors to the primary visual interneurons in vivo. Nonetheless, surprisingly our in vivo recordings show that voltage responses of ortP306 and ebony photoreceptors to light stimuli are larger and faster than those of WT flies, and that the rate of information transfer in ortP306 LMCs can reach that of WT LMCs at bright illumination. Hence the data from the synaptic mutants suggest that by boosting presynaptic responses visual signals can be made to cross the malfunctioning synapses. We then look for evidence for the mechanisms involved. In vitro patch-clamp data from dissociated photoreceptors, which lack axon terminals and thus any synaptic feedback, show that the response properties of ortP306 photoreceptors are identical to those of WT photoreceptors. Therefore, the differences in voltage responses of photoreceptors in vivo cannot be attributed to homeostatic mechanisms in the phototransduction or in the photoreceptor membrane properties. To resolve this matter we record in vivo from photoreceptors and LMCs of temperature-sensitive shibireTS1 mutants. We show that warming shibireTS1 above 28°C silences all vesicle-driven synaptic transmission between their photoreceptors and primary visual interneurons, and that the voltage responses of WT photoreceptors are being boosted continuously by excitatory feedback from the interneurons. When the signal transfer from photoreceptors to LMCs is low, as is the case in dim conditions, or compromised, as in mutants like ortP306 and ebony, the synaptic feedback gets stronger to boost photoreceptor output, increasing the probability for successful synaptic transmission to the primary visual interneurons.
We present our findings in two parts. First, recordings from ortP306, ebony, and temperature-sensitive shibireTS1 mutants provide strong evidence that synaptic feedback to photoreceptor terminals modulates the photoreceptor output. Second, using statistical methods, we provide evidence indicating that this modulation is predominantly from direct synaptic feedback and that it improves the signaling quality during naturalistic stimulation (NS). Based on the most dominant anatomical connections, we deduce the simplest negative feedback model that is sufficient to explain these findings. In this model, photoreceptor output to the interneurons is first sign-inverted and then fed back to photoreceptor terminals via excitatory synaptic conductances.
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MATERIALS AND METHODS |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONREFERENCES |
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; van der Bliek and Meyerowitz, 1991; Kawasaki et al., 2000; Kitamoto, 2001; Gengs et al., 2002), and ebony (Drosophila melanogaster) were raised on standard medium at 19°C in 12:12 light:dark cycle (Wolfram and Juusola, 2004). The flies were taken for in vivo experiments within 1–12 d and for in vitro patch-clamping a few hours after eclosion. We confirmed by sequencing that our ortP306 strain shared the same mutated base pairs as reported previously (Gengs et al., 2002).
In Vitro Electrophysiology
Whole-cell voltage-clamp recordings were made from WT and ortP306 photoreceptor somata to compare the phototransduction machinery and membrane properties of these cells. These recordings were used to test whether homeostatic mechanisms could enhance photoreceptor output when signal transmission to primary visual interneurons was compromised by faulty histamine (ort) receptors on post-synaptic LMCs. Dissociated ommatidia of recently eclosed flies were prepared and transferred to a recording chamber on an inverted Nikon Diaphot microscope (Hardie, 1991a). Experiments were performed within 2 h of eclosion, since photoreceptors do not readily dissociate at later times (Hardie, 1991b). The bath was composed of (in mM) 120 NaCl, 5 KCl, 10 TES, 4 MgCl2, 1.5 CaCl2, 25 proline, and 5 alanine. Recordings were done using Axopatch 1-D (Axon Instruments, Inc.) and electrodes of resistance 10–15 M
; series resistance <25 M and compensated to 80%. Light stimulation via a green LED was set to a maximum effective intensity of 2 x 105 photons/s per photoreceptor. Relative intensities were calibrated using a photomultiplier and converted to absolute intensities in terms of effectively absorbed photons by counting quantum bumps at low intensities (Hardie, 1991a).
In Vivo Experiments
We recorded voltage responses of photoreceptors and LMCs to identical light stimuli separately as the small cells make simultaneous recordings impractical. Intracellular recordings were made using sharp quartz microelectrodes (Juusola and Hardie, 2001a) (Sutter Instrument Co.) of resistance 120–200 M at 25.0 ± 0.5°C. The intraelectrode solution was 3 M KCl for photoreceptor experiments; but 3 M potassium acetate with 0.5 mM KCl for LMCs to prevent rundown of the chloride battery (Hardie, 1989a). Responses were amplified by SEC-10L (NPI Electronic) in current-clamp mode using switching frequencies of 15 kHz and low-pass filtered with light stimuli at 1.5 kHz (Kemo VBF8).
Similar to electrophysiological experiments in blowfly (Calliphora vicina) (Juusola et al., 1995), light responses from the cells of retina and lamina and their respective extracellular spaces show location-dependent, easily identifiable characteristics as the microelectrode advances in the tissue. The microelectrodes were guided through the small corneal openings with different entrance angles for photoreceptors and LMCs to facilitate the penetrations of the targeted cells (see Fig. 2).
When traveling in retina, microelectrodes penetrated alternatingly photoreceptors, glia, and intercellular space (Juusola et al., 1994; Juusola and Hardie, 2001a). Typically, the resting potentials of photoreceptors varied from –60 to –77 mV, while the intercellular space remained at zero, and glia potentials were below –85 mV. Bright light pulses evoked different responses from each of these cellular structures. Photoreceptors produced fast depolarizations of >40 mV, intercellular space showed slow hyperpolarizing field potentials to –8 mV, and maximum glia potentials were slow depolarizations <5 mV. All intracellular responses of photoreceptors of this study, apart from the photoreceptor axons shown in Fig. 9, were recorded in retina.
In the lamina, microelectrodes impaled photoreceptor axons, glia, intercellular space, and LMCs (and possibly ACs). The resting potential of photoreceptor axons varied from –65 to –80 mV, glia potentials were <–90 mV, laminal intercellular space was from –20 to –40 mV and LMCs were from –40 to –70 mV. All these values are given in respect to the intercellular space of retina (0 mV). Bright light pulses evoked different responses from laminal structures. Similar to data from Calliphora (Weckström et al., 1993; Juusola et al., 1995), voltage responses of photoreceptor axons showed a rapid prespike (Juusola and Hardie, 2001a) or an enhanced rise (Fig. 9) followed by 10–40 mV depolarization. As these responses deteriorated easily and were difficult to maintain for longer periods, their response statistics were not analyzed further. Glia cells produced very slow hyperpolarizations of few mV, whereas slow depolarizing field potentials could reach 15 mV. LMCs responded to light pulses with transient hyperpolarizations that could reach values of 45 mV. The large size, polarity, and rapid time course of these voltage responses closely resembled those of Calliphora LMCs, identified in previous electrophysiological and labeling studies (Juusola et al., 1995; Uusitalo et al., 1995). We made no attempt to characterize voltage responses of LMCs into subtypes.
Photoreceptors included in this study had resting potentials in darkness <–60 mV and maximum responses >40 mV (WT, ortP306, and ebony) or >30 mV (shibireTS1). WT, ortP306, and shibireTS1 LMCs had resting potentials <–40 mV and maximum responses >40 mV (WT), >15 mV (ortP306), and >20 mV (shibireTS1). The quality of recordings was high in these conditions.
Light Stimulation and Data Collection
Cells were stimulated at the center of their receptive fields by light from a high-intensity green LED (Marl Optosource, with peak emission at 525 nm) mounted on a cardan arm. The LED constituted a small field stimulus subtending 5° as seen by the fly. Such stimulus should be smaller than a typical receptive field of a Drosophila photoreceptor, whose half-width is estimated to be between 5° and 6° (Götz, 1964; Heisenberg and Buchner, 1977; Stavenga, 2003). The responsiveness of photoreceptors remained unchanged when stimulated with a small field light source that extended only 1°, as seen by the fly, indicating that during stimulation, lateral interactions were minimal (see Fig. S1 A, available at http://www.jgp.org/cgi/content/full/jgp.200509470/DC1). The LED output was taken as the light stimulus. It was measured by photodiodes both during 10-ms light pulses and during repetitions of a 1-s-long naturalistic light pattern (van Hateren, 1997; Juusola and de Polavieja, 2003). The naturalistic light pattern selected from the van Hateren natural stimulus collection, http://hlab.phys.rug.nl/archive.html (van Hateren, 1997), used fully the response ranges of the cells (30–60 mV, 2–200 Hz). The studied intensity range covered 4 log units (Juusola and Hardie, 2001a) from 600 photons/s to 6 x 106 photons/s (I0). Figures show results for dim (1,850 photons/s), medium (60,000 photons/s), and bright light (1.85 x 106 photons/s). Typically, cells were first studied at dim intensities before systematically proceeding to brighter stimulation. The stimulus and response were sampled at 10 kHz. Stimulus generation, data acquisition, and analysis were performed by Matlab interface BIOSYST (Juusola and Hardie, 2001a; Juusola and de Polavieja, 2003) with acquisition control via MATDAQ C-commands (H.P.C. Robinson, Cambridge Conductance).
Temperature Experiments
For temperature sensitivity tests, the voltage responses of 5– 15-min dark-adapted photoreceptors to light pulses were first recorded at 18–20°C before warming up the flies (28–32°C) using a feedback-controlled Peltier-element embedded in the setup (Juusola and Hardie, 2001b). Additionally, the head temperature of the flies was measured with a separate thermocouple and the recordings were calibrated using these values (Juusola and Hardie, 2001b). The warming caused muscle activity that made intracellular recordings very challenging. However, occasionally (in four shibireTS1 and five WT) we managed to record from the same photoreceptors without losing the penetration at different temperatures for several minutes (such as those shown in Fig. 6, C and D, and in Fig. S5, A and B). Other recordings, although requiring slight positional adjustments in the microelectrode to keep it intracellular, showed neither obvious differences in the findings nor in the quality of the data (Fig. S5, C and D). Furthermore, we frequently recorded electroretinograms (ERGs) of shibireTS1 mutants to a saturating light pulse at 20°C and at 30°C in order to confirm that warming removed the on- and off-transients, associated with synaptic transmission from photoreceptors to LMCs (Gengs et al., 2002) (Fig. S4).
Signal-to-Noise Ratio (SNR) Analysis
We analyzed the signaling performance of photoreceptor and LMC output by estimating their signal and noise components, and signal-to-noise ratios both in the time and frequency domain. The voltage responses were prepared for the analysis by removing the first 5–20 traces of response series to a repeated naturalistic stimulation to eliminate adaptational trends. The signal, s(t), was then the average of the remaining voltage responses (typically >50 traces), whereas the noise traces, n(t)i, were the difference between individual traces and the signal (Juusola et al., 1995).
Noise traces, n(t)i, of photoreceptors were analyzed further to see whether they were purely random or whether they contained time-dependent features. The noise variance of photoreceptors (Juusola and de Polavieja, 2003) as shown in Fig. 7 E was taken at each time (or sampling) point across all the noise traces (0.1 ms resolution).
SNR(t) in the time domain (Fig. 7 F) was calculated as the ratio between signal variance and noise variance, using 1-ms resolution. Fourier spectra of s(t) and n(t), i.e., S(f) and N(f), respectively, were calculated using 1 kHz sampling. Dividing S(f) by the corresponding N(f) gave the signal-to-noise ratio in the frequency domain (Shannon, 1948; Juusola and de Polavieja, 2003), SNR(f). In general, the SNR analysis gives an approximation of the signaling performance of the neurons, as their signal and noise are not purely additive, nor is their dynamics Gaussian (Shannon, 1948; Juusola and de Polavieja, 2003).
Calculating the Rate of Information Transfer
We used the triple extrapolation method (Juusola and de Polavieja, 2003) to calculate the rate of information transfer for photoreceptor and LMC voltage responses. The triple extrapolation method, unlike SNR analysis, requires no assumptions about the signal and noise distributions or their additivity (Juusola and de Polavieja, 2003). Some practical considerations for the analysis are as follows. Only cells that allowed stable recordings at eight or nine light intensity levels were selected for analysis. For both WT and ortP306 photoreceptors, we had seven complete recording series. For WT LMCs we used two complete series and one for an ortP306 LMC. Numerous recordings from WT and ortP306 photoreceptors and LMCs obtained at particular light levels behaved similarly to the corresponding ones in the complete series. After removing the first 5–20 trials that showed a strong adaptational trend, we typically used the next 50 traces. The voltage response was resampled from 10 kHz to 1 kHz to remove high frequency noise, and a response matrix of 1,000 points x 50 trials was obtained for the analysis. The order of the trials was also shuffled to minimize the effect of any remaining adaptational trends (Juusola and de Polavieja, 2003). The total entropy and noise entropy were then obtained from the response matrices using the extrapolation parameters given in Table S2.
Online Supplemental Material
Supplemental material for this paper consists of five figures and two tables (available at http://www.jgp.org/cgi/content/full/jgp.200509470/DC1). Fig. S1 shows that neither lateral synaptic connections in lamina nor ERG are the cause for the peak in noise variance of photoreceptors. Fig. S2 shows the phototactic behavior of ortP306 and WT flies. Fig. S3 shows mean membrane potential of LMCs during long experiments in vivo. Fig. S4 shows typical ERG responses of WT flies and shibireTS1 mutants. Fig. S5 shows voltage responses of shibireTS1 and WT flies and their statistics. Table S1 gives light current statistics of WT flies and ortP306 mutants. Table S2 gives extrapolation parameters used for calculating the rate of information transfer.
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RESULTS |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONREFERENCES |
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). Therefore, if the presumed feedback originates from the interneurons whose responses are altered by this mutation, ortP306 photoreceptors should receive very different feedback from them. To observe this difference in feedback activity without exciting neighboring neuro-ommatidia, the light stimulus was delivered within the receptive field of a single photoreceptor (Fig. 1 B, d and e; Fig. S1 A). Since it is possible that the reduced sensitivity of histamine receptors could render the ortP306 mutant blind (Gengs et al., 2002), this experiment (Fig. 2 A) should also reveal whether its LMCs, in fact, can convey any visual signals toward the brain.
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; Srinivasan et al., 1982; Laughlin et al., 1987; Srinivasan et al., 1990; van Hateren, 1992; Juusola et al., 1995; de Ruyter van Steveninck and Laughlin, 1996; van Hateren, 1997; van Hateren and Snippe, 2001), LMCs of WT Drosophila responded to photoreceptor depolarizations with a graded and phasic hyperpolarization (Fig. 2 E), mostly owing to histamine-gated chloride channels (Hardie, 1989a; Juusola et al., 1996; Gengs et al., 2002). As the speed and amplitude of presynaptic responses increased with the brightening stimulus (Fig. 2 D), the LMC output became increasingly transient, peaking before photoreceptor voltages (Fig. 2 H). In contrast, the responses of ortP306 photoreceptors and LMCs were different (Fig. 2, F and G). ortP306 photoreceptors generated faster (Fig. 2 H; red squares) and larger responses (Fig. 2 I) than WT photoreceptors (black squares) at all tested luminances apart from the brightest stimulation where the maximum amplitude of the responses saturated. While the responses of ortP306 and WT LMCs (Fig. 2 I, red circles) both increased with brighter stimulation, ortP306 responses remained smaller than the relatively constant-size WT responses (Fig. 2 I, black circles). Nevertheless, our data establishes that ortP306 LMCs generate a significant throughput for visual signals, responding better than might have been expected from their in vitro histamine sensitivity (Gengs et al., 2002), especially at bright luminances. To scrutinize the findings of intracellular recordings, we further recorded the eye's electrical responses to light pulses, so-called ERGs, by placing surface electrodes on WT flies and ortP306 mutants. Fig. 3 A shows that ERGs of WT flies have prominent on- and off-transients superimposed on a slower background signal, whereas Fig. 3 B shows that in ortP306 ERGs, these transients were much smaller but superimposed on a larger background. The size of the transients is believed to reflect the strength of signal transfer from photoreceptors to primary visual neurons, with the slower background signals being generally attributed to more graded responses of photoreceptors. However, owing to the lack of intracellular recordings, these assumptions have never been tested in Drosophila. Our data shows that at least for ortP306 this correspondence is clear. The differences between their ERG transients and those of WT flies (on-transients, Fig. 3 C; off-transients, Fig. 3 D) agree with the voltage responses of their LMCs, which are similarly smaller (compare Fig. 2, E and G, light gray traces). Furthermore, the respective waveforms of the background signals are systematically faster and larger in ortP306 (Fig. 3, A, B, and E), correlating well with the intracellularly measured photoreceptor outputs (compare Fig. 2 I).
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We summarize the findings from ortP306 mutants. Both intracellular and ERG recordings and behavioral experiments indicate that under bright illumination a significant amount of visual information can be transmitted across malfunctioning histaminergic receptors to the primary visual interneurones and further to the brain, and that this is associated with enhanced photoreceptor output. These findings are consistent with, but cannot yet substantiate, the hypothesis of photoreceptor output being modulated by synaptic feedback from the interneurons.
Evidence that Synaptic Feedback Modulates Photoreceptor Output
Besides feedback from the interneuron network, there are at least two other plausible mechanisms that could enhance the responsiveness of ortP306 photoreceptors. First, it could be caused by additional mutations; second, by homeostatic changes that affect the phototransduction machinery or voltage-gated membrane conductances. To test these hypotheses we examined light- and voltage-gated conductances of WT and ortP306 photoreceptors in vitro (Fig. 4) using whole-cell recordings from R1–R6 photoreceptors in dissociated ommatidia (Hardie, 1991b) (Fig. 4 A). This procedure, which for technical reasons must be done on young flies within a few hours of post-eclosion (see Materials and Methods) (Hardie, 1991b), severs the photoreceptor axons, thus eliminating all synaptic connections of the photoreceptors, including any synaptic feedback. Since whole-cell patch-clamp recordings of the dissociated ortP306 photoreceptors indicated that their transduction machineries (Hardie, 1991b) (Fig. 4, B and C) and membrane conductances (Hardie, 1991a) (Fig. 4 D) were indistinguishable from WT (Table S1), the enhanced output of ortP306 photoreceptors in vivo is unlikely to result from additional mutations or developmental homeostatic changes in photoreceptor somata.
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We also recorded from ebony mutant (Hotta and Benzer, 1969) flies, whose faulty histamine recycling is believed to significantly reduce transmission from photoreceptors to LMCs (Borycz et al., 2002). The aim of this experiment was similar to ortP306 experiments, namely to investigate whether the reduced input to the interneurons would boost photoreceptor output. Fig. 5 F shows that voltage responses of ebony photoreceptors were virtually identical to those of ortP306, and 40% faster than WT responses. Hence, the findings from ortP306 and ebony endorse the hypothesis that when the transmission from photoreceptors to interneurons is compromised, the signals that visual interneurones feed back to photoreceptor terminals boost the photoreceptor output (Fig. 5 G).
shibireTS1 Shows that Synaptic Feedback Comes via Excitatory Conductances
At this point we do not know whether the enhanced photoreceptor output of the mutants in vivo results from a reduction in inhibitory conductances or from an increase in excitatory conductances to photoreceptor terminals. To resolve this we asked what would happen to the photoreceptor output in vivo if the synaptic feedback ceased? If we expect constant feedback conductances even in darkness, and these are inhibitory, then lack of them would depolarize photoreceptors. Whereas, if the feedback uses excitatory conductances, their silence would hyperpolarize photoreceptors.
We tested this by using a temperature-sensitive synaptic mutant (Poodry et al., 1973; Kawasaki et al., 2000), shibireTS1. Warming these mutants to >27°C should silence all their vesicle-driven synaptic transmission. We first verified this for the photoreceptor-LMC synapses by recording intracellularly voltage responses of postsynaptic LMCs to light in shibireTS1 mutants; synaptic transmission from R1–R6 photoreceptors to LMCs appears normal at low room temperatures, but ceases by warming (Fig. 6, A and B, respectively; Fig. S4). Similarly, warming these mutants should also silence the feedback from the interneurons to photoreceptor terminals. Hence, intracellular recordings from WT and shibireTS1 photoreceptors, while warming and cooling the flies, should then reveal how the feedback modulates the photoreceptor output (Fig. 6 C, diagram).
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Key Elements of a Feedback Model
The results from the light-pulse experiments suggest a simple feedback model for signal transmission between photoreceptors and interneurones. It is known from the anatomy of single neuro-ommatidia that both LMCs and local AC processes receive input from six photoreceptors, and that these interneurons feed back to photoreceptors (Meinertzhagen and O'Neil, 1991). While LMCs also send information directly to higher visual centers, ACs signal upwards only indirectly (Meinertzhagen and O'Neil, 1991). The feedback model we propose builds on these anatomical connections to provide the simplest explanation for the data. It has three assumptions. (1) ACs and LMCs function similarly in the feedback network of a single cartridge, since they both detect histamine changes from the same photoreceptor output synapses (Fig. 1 B, a); more evidence for this assumption will be given by statistical analyses in the next section, while its merits and weaknesses will be argued in the discussion. (2) The feedback from the interneurons to photoreceptor terminals is fast, voltage dependent, and includes a maintained, tonic component, as suggested by the shibireTS1 experiment (Fig. 6 E), but also since these feedback synapses have characteristic ribbon structures (Meinertzhagen and O'Neil, 1991; Meinertzhagen and Sorra, 2001) typically associated with a high rate of vesicle release (Uusitalo et al., 1995; Juusola et al., 1996). (3) The feedback uses transmitter(s) that activate depolarizing conductances on photoreceptor terminals (Fig. 6, C–E); possibly glutamatergic, as both LMCs and ACs show glutamate-like immunoreactivity (Sinakevitch and Strausfeld, 2004), and/or cholinergic, as suggested by pharmacology (Hardie, 1989b) and immunohistochemistry (Yasuyama et al., 1996). In functional terms, an active feedback should add an extra depolarizing and accelerating component to the voltage response of a photoreceptor (compare Fig. 6 F; Fig. S5 J). When light depolarizes a photoreceptor, LMCs hyperpolarize, because of the sign inversion at the first (histaminergic) synapses. As the voltage drops in LMCs so does their synaptic transmission. This should reduce their feedback component to photoreceptor axon terminals, thereby shrinking and slowing down the photoreceptor output.
Function of the Feedback: (1) Rapid Gain Control
We tested the feedback model in vivo by comparing voltage responses of WT and ortP306 photoreceptors and LMCs to a 1-s-long bright NS pattern that was repeated 25–150 times (see Materials and Methods). The reason for using ortP306 for the functional analysis, instead of shibireTS1, is that the experiments can be done at a lower temperature (25°C) where long-lasting intracellular recordings are stable and much easier to do, as the flies are less active. To help visualize the function of the feedback, the data is presented with conceptual circuit diagrams, which show the major synaptic connections and the flow of information within a single WT and ortP306 neuro-ommatidium (Fig. 7, A and B, respectively). Light signals (orange arrows) are processed by photoreceptors (yellow) and transmitted via histaminergic synapses (H) to LMCs (blue) and ACs (light green). These feed back to photoreceptor terminals synaptically via ligand-gated conductances (G). Arrows indicate the magnitude and direction of information flow, while whiteness of circuitry marks increased depolarization.
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) they are, and the more transmitter they release onto photoreceptor terminals, causing an increase in excitatory conductance. Consequently, the feedback in ortP306 mutants should be stronger, as seen by the larger and faster responses of ortP306 photoreceptors in Fig. 7 C (whitened axons of ortP306 photoreceptors; cf. Fig. 7, A and B). In this way, the interneuron feedback provides gain control for the first visual synapses. When the probability of saturating LMCs is low (Fig. 7 D, red line), feedback to photoreceptor terminals is strong (Fig. 7 C, red line). When responses of LMCs become large (Fig. 7 D, black line), feedback reduces (Fig. 7 C, black line). The responses of ortP306 photoreceptors are faster for two reasons (Fig. 7 C and Fig. 2 H). The enhanced synaptic feedback increases their membrane conductances, thus giving them a smaller membrane time constant (Fig. 7 C; cf. responses to depolarizing current steps in Fig. 4, A and B). The second factor is that the feedback signals themselves are briefer (Fig. 7 D), attributable, at least partly, to the faster dynamics of histamine-gated ortP306 receptors on the LMC membrane (Fig. 2 G).
Function of the Feedback: (2) Regulation of the Signal Quality
The second prediction of the feedback model concerns network noise. The small size and high membrane impedance of Drosophila photoreceptors provide favorable electrophysiological conditions where the effects of synaptic feedback, although weakened by the distance, can still be detected when recording from their somata (Juusola and Hardie, 2001a). This should be seen as extra noise coming from the many synapses of the feedback network at particular points in time. The main origin of the noise is in the ligand-gated receptors, either histaminergic on the interneurons or probably glutamatergic and/or cholinergic on the photoreceptors (Hardie, 1989b; Yasuyama et al., 1996; Sinakevitch and Strausfeld, 2004). We expect lower noise when most of the receptor-bound ion channels on photoreceptors are open, i.e., when sufficiently high transmitter levels are being released from interneurons. Therefore, the noise variance (see Materials and Methods) in photoreceptor responses should peak when the interneurons are the most hyperpolarized. Fig. 7 E shows the mean noise variance of four WT photoreceptors, chosen from experiments where naturalistic stimulation was repeated >100 times. The dynamics of noise variance mirror the LMC potential with clear peaks appearing when LMCs hyperpolarize the most, as predicted by the feedback model. Since the noise variance peaks when noise from light- and voltage-gated channels in photoreceptors is minimum (Hardie, 1991a; Juusola and Hardie, 2001a) and it decays (Fig. 7 E, star) when the responses, and thus noise in the photon arrival, is the largest (Fig. 7 C, star), presynaptic explanations can be ruled out (see Fig. S1, A and B). In ortP306 mutants, the model predicts that, owing to the smaller amplitude and briefer transients in the responses of LMCs, the mean noise variance of their photoreceptors should show smaller and briefer peaks. This is also evident in Fig. 7 E.
What is the effect of the feedback on the information transfer? Because LMCs sum the input from six photoreceptors that receive visual input from the same visual field (Kirschfeld, 1967), their SNR is higher than that of a single photoreceptor (Srinivasan et al., 1982; Laughlin et al., 1987; van Hateren, 1992; Juusola et al., 1995; de Ruyter van Steveninck and Laughlin, 1996; van Hateren and Snippe, 2001). Likewise, we expect the same principle working for local ACs. By sharing each tetrad synapse with two LMCs, amacrine cells receive similar input from R1–R6 photoreceptors as the monopolar cells. Therefore, SNR of ACs should be similarly enhanced as that of LMCs. To study whether the feedback from LMCs and ACs improves presynaptic signaling we compared the dynamics of the SNR in WT and ortP306 photoreceptors. Given that hyperpolarization of LMCs and ACs reduces the feedback, most peaks on the WT photoreceptor SNR occur during their responses to transient light changes (Juusola and de Polavieja, 2003) (Fig. 7 F, black line). In ortP306 mutants, since their interneurons are more depolarized and their responses are richer in high frequencies (Fig. 7 D; red and black lines, respectively), the enhanced feedback typically makes the SNR of their photoreceptors reach higher values with faster rising and briefer peaks (Fig. 7 F, red line).
Additionally, we assess the effect of feedback on information transfer in WT and ortP306 photoreceptors and LMCs at different luminances (Fig. 8, A and B; see Materials and Methods). The extra high frequency feedback of high SNR from the interneurons should boost the SNR of ortP306 photoreceptors. This is indeed what we observe (Fig. 8 A, red and black lines, respectively) at all but the dim stimulation, where the photon shot noise dominates. The SNR of ortP306 LMCs is well below that of WT LMCs at dim stimulation and at low frequencies (Fig. 8 B, red and black lines, respectively). Yet, at bright stimulation, the SNR of ortP306 LMCs is above that of WT LMCs at medium and high frequencies. These results were further quantified by calculating the corresponding information transfer rates (R). Fig. 8 C shows that brightening, i.e., increasing the stimulus SNR, generates a concomitant increase in information transfer rates of photoreceptors and LMCs. Since the observed enhanced responsiveness in ortP306 photoreceptors originates from the enhanced feedback of high SNR, they can carry more information than the WT photoreceptors across the luminance levels. This allows the throughput of ortP306 LMCs to reach the values of WT LMCs at bright stimulation.
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DISCUSSION |
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TOPABSTRACTINTRODUCTIONMATERIALS AND METHODSRESULTSDISCUSSIONREFERENCES |
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Model of Synaptic Signal Transfer from Photoreceptors to the Primary Visual Interneurons
Results from ortP306, ebony, and shibireTS1 photoreceptors (Fig. 6) and noise analysis of WT photoreceptors (Fig. 7 E) strongly suggest that a simple negative feedback loop, combining sign-inverting graded potential synapses with a feedback circuitry of excitatory transmitters (Yasuyama et al., 1996; Sinakevitch and Strausfeld, 2004), regulates signal transfer from photoreceptors to LMCs. This overall framework can be further supported by directly comparing pre- and postsynaptic voltage responses on a stretched time scale, making it possible to roughly work out some time-dependent properties of this coding.
Fig. 9 illustrates typical correlations in high-quality (low noise) voltage responses of a WT photoreceptor axon (recorded in lamina; black thick line) and a WT LMC (gray thick line), and their rates of change (thin lines), to a 10-ms-long bright pulse (thin dark gray line). Phototransduction mechanisms have an absolute time delay (Juusola and Hardie, 2001a), so only 9 ms after the stimulus onset the photoreceptor axon begins to depolarize (a). As the photoreceptor depolarizes, its histamine release increases, and the LMC hyperpolarizes (b). This leads to a transient reduction in the excitatory feedback to the photoreceptor axon terminal (c), i.e., reduction of the transmitter release from the interneurons, slowing down the rate the photoreceptor is depolarizing (c). As soon as the rate of hyperpolarization in the LMC begins to decelerate, the boost from the feedback to photoreceptor terminals picks up again. It reaches its maximum, seen as the fastest rise in the photoreceptor depolarization (d), moments after the LMC begins to depolarize.
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; Meinertzhagen and Sorra, 2001) should make the feedback nearly instantaneous and thus able to prevent the postsynaptic histamine receptors from saturation. In this respect, the automatic balancing of synaptic drives resembles predictive coding, usually associated with neural inhibition (Srinivasan et al., 1982).
There are four reasons why we believe that our assumption of sign inverting amacrine cells, which hyperpolarize to light increments, is likely to be correct. First, since amacrine cells contribute the majority of the synapses (65%) to photoreceptor axon terminals (Meinertzhagen and Sorra, 2001), we expect that the waveforms (Fig. 6 F) feeding back to photoreceptors to be dominated by the dynamics of this circuit. Second, over the years there has been a considerable research effort for recording electrical responses from lamina of dipteran flies (Järvilehto and Zettler, 1971; Srinivasan et al., 1982; Laughlin et al., 1987; Hardie et al., 1988, 1989a,b; Srinivasan et al., 1990; James, 1992; van Hateren, 1992; Juusola et al., 1995; Uusitalo et al., 1995; de Ruyter van Steveninck and Laughlin, 1996; van Hateren, 1997; van Hateren and Snippe, 2001), yet these studies have provided no compelling evidence for graded depolarizing responses beyond those attributed to photoreceptor axons and slower laminal field potentials. Since the web of amacrine cells in lamina is dense, some of the hyperpolarizing responses should have come from amacrine cells (see also Shaw, 1984). Third, our data shows that the synaptic feedback enhances the information transfer rate of photoreceptors (Fig. 8 C), and that the noise characteristics of photoreceptors mirror the response dynamics of LMCs (Fig. 7 E). These findings strongly suggest that the separate feedback circuits from LMCs and ACs to photoreceptors are synchronized and in the same phase. Fourth, at temperatures >27°C all synaptic transmission in shibireTS1 mutants ceases (Figs. S4 and S5; Chen and Stark, 1993; ShibireTS has been very widely used and found to block synaptic transmission at all synapses investigated, both graded and spiking, e.g., van der Bliek and Meyerowitz, 1991; Kitamoto, 2001). Naturally, this should include both amacrine cell and LMC feedbacks. In such conditions, the total waveform of the signals fed back to photoreceptors can be approximated as the difference between the voltage responses of WT and shibireTS1 photoreceptors, given that the light stimulus is the same and the membrane impedances of the photoreceptors are similar. Since this total signal from the primary visual interneurones resembles the inverted voltage response of LMC (Fig. 6 F and Fig. S5 J), it is probable that its amacrine cell and LMC components are similar.
However, a recent publication by Douglass and Strausfeld (2005) apparently challenges this view. They report obtaining intracellular recordings from three amacrine cells in Phaenicia and show partially dye-filled processes of these neurons as evidence. The responses to light increments are small depolarizations (<5 mV), which according to their frequency responses are slower and more delayed than those of photoreceptors. Hence, judged by their waveforms, these responses could not be the main components of the fast synaptic feedback we have presented in this paper. However, if the recorded responses showed the total output of amacrine cells, then the synthesis would be that, regardless of their dominating prevalence, amacrine cell synapses are providing a weaker, tonic feedback to photoreceptor axon terminals, whereas the larger and faster responses from monopolar cells (L2 and possibly L4) would provide the dynamic modulation. To further investigate this we have started producing transgenic flies that ultimately should elucidate the role of different feedback synapses in lamina.
Comparison to Other Models
Other models have inconsistencies with the data. Here we compare our findings to three models, each based on different premises: inhibitory conductances, histaminergic autoreceptors, and homeostatic increase in histamine release.
We start by imagining a model whereupon a negative feedback from primary visual interneurones to photoreceptors uses inhibitory conductances. According to such a model, the responses of WT photoreceptors are smaller and slower because the feedback from the interneurons reduces their size and speed, while responses of ortP306 photoreceptors are larger and faster because this feedback is silent. However, this explanation is contradicted by the results from (1) shibireTS1 (Fig. 6), which establishes that the conductances involved are excitatory and have a tonic component. Further experimental evidence for this are: (2) WT and ortP306 photoreceptors have similar resting potentials (Fig. 5 C) and (3) membrane impedances (Fig. 5 D). In addition, (4) the signaling performances of ortP306 photoreceptors are better than those of WT photoreceptors (Fig. 8, A and C), requiring an increased, not reduced, flow of information from visual interneurons.
Could histaminergic autoreceptors explain the enhanced photoreceptor output? Autoreceptors, although never shown in Drosophila photoreceptors, have been speculated to form a negative feedback (Hardie et al., 1988) that regulates the level of histamine release from photoreceptor terminals. As such they should hyperpolarize, owing to chloride conductance, to light, otherwise the feedback would be positive, leading to a rapid increase in histamine concentration and saturation of the post-synaptic receptors. Several factors make it unlikely that histaminergic autoreceptors are responsible for the enhanced output of ortP306 photoreceptors. Comparison between in vitro (Gengs et al., 2002) and in vivo data from ortP306 LMCs (Fig. 2 F) suggests that histamine release from photoreceptors is increased. Hence, if autoreceptors were functional in ortP306 mutants, they would hyperpolarize photoreceptors more than those of WT flies. On the other hand, if they were sub- or nonfunctional, the ortP306 photoreceptors would depolarize more than WT photoreceptors. Our data contradicts these statements by showing that (1) the resting potentials of ortP306 and WT photoreceptors are similar, and that (2) shibireTS1 photoreceptors hyperpolarize when the synaptic transmission, and so also the histamine binding to possible autoreceptors, is silenced by warming (Fig. 6). Therefore, we rule out the hypothesis that hyperpolarizing conductances via histaminergic autoreceptors would be the cause for the enhanced output of ortP306 photoreceptors.
Finally, we consider why homeostatic mechanisms increasing histamine release from the photoreceptor terminals alone fail to explain our findings. Light-adaptational augmentation of the voltage responses in ortP306 LMCs could not only stem from the activity of enhanced synaptic feedbacks but also from a homeostatic increase in the histamine release from the photoreceptor terminals. However, our data do not support the latter mechanism alone, as this would increase the presynaptic noise, or at best keep it unchanged. The fact that the SNR of ortP306 photoreceptors is higher than that of the WT photoreceptors means that extra information must be channeled to ortP306 photoreceptors from a source that has a higher SNR than that of a single photoreceptor. As the phototransduction machineries and membrane properties, i.e., the capture and processing of light signals, are identical in WT and ortP306 photoreceptors, this extra information can only arrive from the feedback network, which, attributable to signal pooling (neural superposition), is the only local neural component (source) having a higher SNR than that of a single photoreceptor.
Dissecting the Feedback Model
We now examine how feedback shapes voltage responses of photoreceptors by schematically comparing the effects of different components of the feedback (Fig. 10). We start by dividing the voltage responses of a photoreceptor into two components: the phototransduction response and the excitatory feedback from interneurons. To keep the comparisons simple we consider a 45-mV phototransduction response to a light flash and a 10-mV feedback background (Fig. 6 C). Notice that while in reality the underlying conductances add and subtract, not the resulting voltages, this approximation can be safely used for stressing the major differences in the responses of wild-type and mutant photoreceptors, since the membrane impedances of these cells were similar (Fig. 5 D; Fig. S5). The resting potential of photoreceptors in darkness without the feedback is –85 mV (
. Inset a, tetrad synapse, a photoreceptor terminal connects to two LMCs and an AC. Insets b and c, feedback synapses from AC and L2 cell to a photoreceptor, respectively. Insets d and e, collaterals from other neuro-ommatidia.
