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(The FASEB Journal. 1999;13:S271-S276.)
© 1999 FASEB

Fast multisite optical measurement of membrane potential: three examples

SRDJAN ANTIC1, LAWRENCE B. COHEN, YING-WAN LAM, MATT WACHOWIAK, DEJAN ZECEVIC and MICHAL ZOCHOWSKI

Department of Cellular and Molecular Physiology, Yale University School of Medicine, New Haven, Connecticut 06520, USA

1Correspondence: Physiology, 333 Cedar Street, New Haven, CT 06520, USA. E-mail: antic{at}fred.med


   INTRODUCTION
TOP
INTRODUCTION
RESULTS
FUTURE DIRECTIONS
REFERENCES
 
THIS PAPER DESCRIBES threekinds of measurements from nervous systems using a microscope camera with unusual characteristics. This camera has poor spatial resolution (24x24 pixels), but its temporal resolution (1 ms) and dynamic range (100 dB) are close to ideal. For each kind of measurement we present arguments suggesting that the limited spatial resolution of the camera is not actually limiting.

In all of these experiments, the source of the optical signals are voltage-sensitive dyes. These are dye molecules that bind to membranes and change their spectral properties (absorption and/or fluorescence) in response the changes in membrane potential (for reviews see refs 1 2 3 4 5 ). The dyes that we have used are both linear and fast (6 , 7) ; they respond to changes in membrane potential with a time constant of <10 µs.

The first kind of measurement uses the optical signal of membrane potential to determine the spread of potential in the processes of an individual neuron. The second kind of measurement uses the dyes to monitor the spike activity in many individual cell bodies in an invertebrate ganglion while that ganglion is generating a behavior. The third kind of measurement records the population signals representing the average change in membrane potential from many cells and processes in a vertebrate central nervous system (CNS). All three kinds of recordings have provided information about the function of the nervous system that was previously unobtainable.

The measurements were made with a 464 element silicon photodiode array system (24x24 grid with corner detectors omitted) with parallel readout (NeuroPlex; RedShirt Imaging, LLC, Fairfield, Conn.) placed in the image plane formed by a microscope objective. With this many detectors it is easy to sample a complete frame every millisecond. The parallel readout allows the measurement of a large number of photons (up to 1010/ms), which yields a dynamic range of up to 100 dB. (For additional details about the apparatus and measurements see refs 8 , 9 ).


   RESULTS
TOP
INTRODUCTION
RESULTS
FUTURE DIRECTIONS
REFERENCES
 
Signals from the processes of an individual neuron
Understanding the biophysical properties of single neurons and how they process information is fundamental to understanding how the brain works. With the development of new measuring techniques, it became widely recognized that dendritic membranes of many vertebrate CNS neurons contain active conductances (e.g., refs 10 11 12 ). An important consequence of active dendrites is that the electrical properties of these processes will be extraordinarily complex, dynamic, and, in the general case, impossible to predict in the absence of detailed measurements.

To obtain such a measurement, one would, ideally, like to be able to monitor, at multiple sites, subthreshold events as they travel from the sites of origin on neuronal processes and summate at particular locations to influence action potential initiation. This goal has not been achieved in any neuron, vertebrate, or invertebrate, because of the technical limitations of experimental measurements that use electrodes. To achieve better spatial resolution, it is necessary to turn from direct electrical recording to indirect, optical measurements using voltage-sensitive dyes. Recently, the sensitivity of intracellular voltage-sensitive dye techniques for monitoring neuronal processes in situ has been improved (by a factor of ~150), allowing direct recording of subthreshold and action potential signals from the neurites of invertebrate neurons (13 , 14) . The improvement in signal-to-noise ratio is based on previous experience from other laboratories (15 , 16) and on 1) finding an intracellular dye that gives a relatively large fractional change in fluorescence and 2) improvements in the apparatus to increase the incident light intensity, lower the noise, and filter more efficiently. Encouraging results have also been obtained in preliminary studies on vertebrate CNS neurons in brain slices (17, 17a).

A typical result of multi-site optical recording from an individual invertebrate nerve cell in situ is shown in Fig. 1A . To understand the functional organization of this neuron, experiments were carried out to determine the position of the action potential trigger zones in different processes. The image of the cell, stained by intracellular injection of the fluorescent voltage-sensitive dye JPW1114, was projected by an objective onto the array of photodiodes as indicated in the Fig. 1Aa . This panel represents the multi-site recording of action potential signals, evoked by a transmembrane current step, from axonal branches Br2, Br3, and Br4. Optical signals associated with action potentials, expressed as fractional changes in fluorescent light intensity ({Delta}F/F), were ~1% in recordings from the processes. With these measurements, it is straightforward to determine the direction and velocity of action potential propagation in the processes. The direction of propagation is clear from the color-coded representation of the data (Fig. 1Ab ). This panel shows the potential changes in the branching structure at nine different times separated by 1.6 ms. The red color corresponds to the peak of the action potential. The panels shows that the action potential trigger zone is located at position 2 and ortho- and antidromic spread of the nerve impulse occurs from this site. The earliest spike was evoked ~1 mm away from the soma. The spike initiation segment in the axon is ~300 µM in length. Under normal conditions, slow depolarizing voltage pulses applied to the soma are electronically spread into the processes with little attenuation because of the very long axonal space constant for slow voltage changes. These depolarizing pulses initiate action potentials at remote sites in the processes that are characterized by higher excitability than that of neighboring segments.



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Figure 1. Aa) Voltage-sensitive dye recording of action potential signals from elements of the photodiode array positioned over the image of axonal arborization of a Helix metacerebral cell in the left cerebral ganglion. Axonal branches are marked Br 1–4. Spikes were evoked by transmembrane current steps delivered through the recording microelectrode in the soma. Each optical trace represents 70 ms of recording centered around the peak of the spike. Each diode received light from 50 x 50 µM area in the object plane. Ab) Color-coded representation of the data shown in panel Aa indicating the size and location of the primary spike trigger zone and the pattern of spike propagation. Consecutive frames represent time points 1.6 ms apart. The color scale is relative with the peak of the action potential for each detector shown in red (modified from ref 14 ). B) Raster diagram of the action potential activity recorded optically from an Aplysia abdominal ganglion during a gill-withdrawal reflex. The command pulse to the mechanical toucher began at the time of the line labeled Stim. In this recording, activity in 110 neurons was measured. The bottom trace shows the gill movement (contraction upward) recorded on videotape. We think this recording is incomplete and that the actual number of active neurons was 200–250. Most neurons are activated by the touch but one, #4334 (~1/3 down from the top), was inhibited. This inhibition was seen in repeated trials in this preparation. (Modified from ref 21 ). C) The outputs of five individual detectors in a population signal measurement from a turtle olfactory bulb. Four different signals in response to an odor stimulus (cineole; 10% saturation) are illustrated. The time course of the DC signal has been attenuated by the 5 Hz high-pass filter that was used for all of the traces. Three different oscillations are distinguishable. The length of the vertical calibration on the right represents the stated value of the change in fluorescence divided by the resting fluorescence ({Delta}F/F). A dynamic range of >80 dB is required to measure these signals. Modified from ref 26a , 32 ).

Both the finite space constant for membrane potential changes in the processes (hundreds of microns for potential changes around the resting potential) and the blurring as a result of light scattering in the Helix ganglion limit the maximum useful spatial resolution in this kind of measurement. The 24 x 24 pixel resolution of NeuroPlex appears to be adequate in some circumstances.

Action potentials recorded from many individual neurons in an Aplysia ganglion
Nervous systems are made up of large numbers of neurons, and many of these are simultaneously active during the generation of behaviors. The original motivation for developing optical methods was the hope that they could be used to record all of the action potential activity of all the neurons in simpler invertebrate ganglia (15) . Techniques that use microelectrodes to monitor activity are limited in that they can observe single cell activity in only as many cells as one can simultaneously place electrodes (typically two or three neurons). Obtaining information about the activity of many cells is important for understanding the roles of the individual neurons in generating behavior and for understanding how nervous systems are organized.

In the first attempt to use voltage-sensitive dyes in ganglia (18) , we were fortunate to be able to monitor activity in a single neuron because the photodynamic damage was severe and the signal-to-noise ratio small. Now, however, with better dyes and apparatus, the spike activity of hundreds of individual neurons can be recorded simultaneously (19 , 20) . In the experiment described below, we measured the spike activity of ~50% of the ~1,000 cells in the Aplysia abdominal ganglion. Opisthobranch molluscs have been a preparation of choice for this kind of measurement because their CNSs have relatively few, relatively large neurons, and almost all of the cell bodies are fully invaded by the action potential.

Because the image of a ganglion is formed on a rectilinear diode array, there is no simple correspondence between images of cells and photodetectors. Thus, a sorting step is required to determine the activity in neurons from the spike signals on individual photodiodes. Although this sorting step is tedious, difficult, and almost certainly results in errors, different individuals from the same laboratory and from different laboratories have obtained similar results. The result from one data set is shown in the raster diagram of Fig. 1B . The start of the 0.5 s mechanical stimulus occurred at the time indicated by the ‘Stim’ at the bottom. The bottom trace shows the gill movement. There were 110 neurons whose activity was detected optically. Similar results have been obtained by Nakashima et al. (20) . Because the signal-to-noise ratio in the measurements was not large, it seemed likely that this recording was not complete. Wu et al. (21) estimated that ~50% of the active neurons were detected. Thus, the actual number of activated neurons during the gill-withdrawal reflex was ~250.

We were surprised at the large number of neurons that were activated by the light touch. Furthermore, a substantial number of the remaining neurons are likely to be either inhibited by the stimulus or receive a large subthreshold excitatory input. It is almost as if the Aplysia nervous system is designed such that every cell in the ganglion cares about this (and perhaps every) sensory stimulus. In addition, >1000 neurons in other ganglia are activated by this touch (22) . Clearly, information about this very mild and localized stimulus is propagated widely in the Aplysia nervous system. These results force a more pessimistic view of the present understanding of the neuronal basis of apparently simple behaviors in relatively simple nervous systems. Elsewhere we present arguments suggesting that the abdominal ganglion may function as a distributed system (21 , 22) .

The fact that we can monitor the activity of a large fraction of the neurons during the behavior means that we can attempt to relate the activity of individual (groups) of neurons to the behavior.

In this kind of measurement the optimal signal-to-noise ratio will be obtained when the size of the image of an individual neuron and the size of a photodetector are identical. A smaller signal-to-noise ratio will result either if the light from a single cell body falls on many detectors or if the light from many neurons falls on a single detector. Thus, the 464 element array was approximately ideal for the Aplysia preparation containing ~1,000 neurons.

Population signals from the turtle olfactory bulb
In a measurement from a vertebrate brain stained by superfusing a solution of the dye over the surface, each photodetector will receive light from a large number of neurons and neuronal processes. Because of the blurring resulting from light scattering and from signals from layers that are out-of-focus, the X-Y spatial resolution from a measurement of an intact brain structure using ordinary microscopy cannot be better than 100–200 µM (23) . This limitation means that a 24 x 24 array is adequate for brain areas up to ~4 x 4 mm (which would include the entire olfactory bulb in the turtle). In the measurements described below, each detector received light from a 150 µM square area (a volume of ~0.1 mm3) of bulb, which contains thousands of neurons and processes. The voltage-sensitive dye signal will be a population average of the change in membrane potential in all of these membranes. The signals will represent the coherent (synchronous) activity of the neurons in the areas imaged onto the individual photo-diodes.

E. D. Adrian first recorded spontaneous oscillations in field potential recordings from the olfactory bulbs of the cat, rabbit, and hedgehog and showed that odors would increase their magnitude and frequency (23a) . The induced oscillations were the same for different odors (23a , 24 ).

The spatial distribution of the field potential oscillations was studied in the rabbit by Freeman (24) and Freeman and Di Prisco (25) using an array of 64 implanted electrodes. They found that "the same time series held for almost all channels on almost every burst." The largest phase difference between distant sites on the bulb was a small fraction (5–8%) of the cycle period, implying that the signals would mainly appear over the entire bulb as standing waves of depolarization.

We made voltage-sensitive dye recordings of the response to odors in the olfactory bulb of the turtle. Preliminary evidence (26a) suggests that these optical measurements have a spatial resolution ~25 times better than local field potential measurements. Our results in the turtle are quite different from those found by Freeman and Di Prisco (25) . We found that odor application to the nose elicited three different oscillations in the turtle bulb. These oscillations differed in location, frequency, latency, and concentration dependence. Figure 1C illustrates the outputs of five photodiodes (1–5) positioned in a rostral to caudal order. There is a short latency DC signal (arrow) seen on all five detectors. The next signal is an oscillation (~14 Hz) labeled medial, which is seen best isolated at position 3. This is followed by the rostral signal, which is seen best isolated at position 1. The rostral has the highest frequency (16 Hz). The caudal signal has the longest latency and lowest frequency (a frequency that is very close to one half of the rostral frequency). This signal is best isolated at position 5. Detectors 2 and 4 come from regions where signals overlap (rostral and medial for detector 2 and medial and caudal for detector 4). The medial signal occurred at the lowest odorant concentration; both the rostral and the caudal signals could often not be detected at concentrations where the medial signal was relatively large. The rostral and caudal signals appeared to propagate. The rostral signal began in the most rostral part of the bulb and propagated caudally. The caudal signals had less regular propagation patterns, but they too were not simple standing waves.

The difference between our results in the turtle and the earlier results of Freeman (24) in the rabbit may result from a species difference. However, another possible explanation for the difference is that our voltage-sensitive dye measurements have a spatial resolution that would facilitate the detection of spatially separate patterns. Additional experiments will be required to distinguish these two possibilities.

The fact that these odor induced oscillations involve coherent activity of a large number of neurons suggests that they might be functionally important. However, their functional meaning and/or importance are not known. Future experiments will be directed at determining whether these signals are different for different odors and thereby have some role in odor recognition. Another possibility is that the coherent activity is related to the animal’s arousal state.


   FUTURE DIRECTIONS
TOP
INTRODUCTION
RESULTS
FUTURE DIRECTIONS
REFERENCES
 
An exciting novel direction is the development of methods that would stain specific types of neurons in vertebrate preparations. Three quite different approaches are being explored; all three require additional developmental efforts before they can be used routinely. First, the use of retrograde staining procedures has recently been investigated in the embryonic chick and lamprey spinal cords (27 , 28) . An identified cell class (motoneurons) was selectively stained. Spike signals from individual neurons were measured in lamprey experiments (29) . Second, is the use of cell-type specific staining developed for fluorescein (30) . It might be possible to use a similar strategy to selectively stain cells with voltage-sensitive or ion-sensitive dyes. Third, Siegel and Isacoff (31) constructed a genetically encoded combination of a potassium channel and green fluorescent protein. When introduced into a frog-oocyte, this molecule had a (relatively slow) voltage dependent signal with a fractional fluorescence change of 5%.

Optical recording already provides unique insights into brain activity and organization. Improvements in sensitivity or selectivity would make these methods even more powerful.


   ACKNOWLEDGMENTS
 
The experiments carried out in our laboratories were supported by NIH grant NS08437 and NSF grant IBN 9604356.


   REFERENCES
TOP
INTRODUCTION
RESULTS
FUTURE DIRECTIONS
REFERENCES
 

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