Measurements on fast light-induced light-scattering and -absorption changes in outer segments of vertebrate light sensitive rod cells

Rhodopsin, light-sensor of vision

The light sensor of vertebrate scotopic (low-light) vision, rhodopsin, is a G-protein-coupled receptor comprising a polypeptide chain with bound chromophore, 11-cis-retinal, that exhibits remarkable physicochemical properties. This photopigment is extremely stable in the dark, yet its chromophore isomerises upon photon absorption with 70% efficiency, enabling the activation of its G-protein, transducin, with high efficiency. Rhodopsin's photochemical and biochemical activities occur over very different time-scales: the energy of retinaldehyde's excited state is stored in <1 ps in retinal-protein interactions, but it takes milliseconds for the catalytically active state to form, and many tens of minutes for the resting state to be restored. In this review, we describe the properties of rhodopsin and its role in rod phototransduction. We first introduce rhodopsin's gross structural features, its evolution, and the basic mechanisms of its activation. We then discuss light absorption and spectral sensitivity, photoreceptor electrical responses that result from the activity of individual rhodopsin molecules, and recovery of rhodopsin and the visual system from intense bleaching exposures. We then provide a detailed examination of rhodopsin's molecular structure and function, first in its dark state, and then in the active Meta states that govern its interactions with transducin, rhodopsin kinase and arrestin. While it is clear that rhodopsin's molecular properties are exquisitely honed for phototransduction, from starlight to dawn/dusk intensity levels, our understanding of how its molecular interactions determine the properties of scotopic vision remains incomplete. We describe potential future directions of research, and outline several major problems that remain to be solved.

Toward a clinical optoretinogram: a review of noninvasive, optical tests of retinal neural function

The past few years have witnessed rapid development of the optoretinogram-a noninvasive, optical measurement of neural function in the retina, and especially the photoreceptors (Ph). While its recent development has been rapid, it represents the culmination of hundreds of experiments spanning decades. Early work showed measurable and reproducible changes in the optical properties of retinal explants and suspensions of Ph, and uncovered some of the biophysical and biochemical mechanisms underlying them. That work thus provided critical motivation for more recent work based on clinical imaging platforms, whose eventual goal is the improvement of ophthalmic care and streamlining the discovery of novel therapeutics. The first part of this review consists of a selective summary of the early work, and identifies four kinds of stimulus-evoked optical signals that have emerged from it: changes in light scattered from the membranous discs of the Ph's outer segment (OS), changes in light scattered by the front and back boundaries of the OS, rearrangement of scattering material in and near the OS, and changes in the OS length. In the past decade, all four of these signals have continued to be investigated using imaging systems already used in the clinic or intended for clinical and translational use. The second part of this review discusses these imaging modalities, their potential to detect and quantify the signals of interest, and other factors influencing their translational promise. Particular attention is paid to phase-sensitive optical coherence tomography (OCT) with adaptive optics (AO), a method in which both the amplitude and the phase of light reflected from individual Ph is monitored as visible stimuli are delivered to them. The record of the light's phase is decoded to reveal a reproducible pattern of deformation in the OS, while the amplitude reveals changes in scattering and structural rearrangements. The method has been demonstrated in a few labs and has been used to measure responses from both rods and cones. With the ability to detect responses to stimuli isomerizing less than 0.01% of photopigment, this technique may prove to be a quick, noninvasive, and objective way to measure subtle disease-related dysfunction at the cellular level, and thus to provide an entirely new and complementary biomarker for retinal disease and recovery.

Imaging Retinal Activity in the Living Eye

Retinal function has long been studied with psychophysical methods in humans, whereas detailed functional studies of vision have been conducted mostly in animals owing to the invasive nature of physiological approaches. There are exceptions to this generalization, for example, the electroretinogram. This review examines exciting recent advances using in vivo retinal imaging to understand the function of retinal neurons. In some cases, the methods have existed for years and are still being optimized. In others, new methods such as optophysiology are revealing novel patterns of retinal function in animal models that have the potential to change our understanding of the functional capacity of the retina. Together, the advances in retinal imaging mark an important milestone that shifts attention away from anatomy alone and begins to probe the function of healthy and diseased eyes.

Light-Induced Length Shrinkage of Rod Photoreceptor Outer Segments

Purpose

This study was designed to verify light-induced outer segment (OS) length shrinkage of rod photoreceptors and to characterize its anatomic source at disc-level resolution.

Methods

Frog (Rana pipiens) retinas were used for this study. Time-lapse light microscopy of freshly isolated OSs was employed to test transient rod OS changes at 10 ms temporal resolution. Histological light microscopy of dark- and light-adapted retinas was used to confirm light-induced rod OS length changes; and transmission electron microscopy (TEM) was used to quantify light-driven structural perturbation of rod OSs at disc level resolution.

Results

Time-lapse light microscopy images verified transient length shrinking responses in freshly isolated rod OSs. Histological light microscopy images confirmed reduced rod OS lengths in light-adapted retinas, compared to that of dark-adapted retinas. TEM images disclosed shortened inter-disc distances in light-adapted retinas compared to dark-adapted retinas.

Conclusions

Light-induced rod OS length shrinkage was confirmed using time-lapse light microscopy of isolated rod OSs and histological light microscopy of dark- and light-adapted retinas. TEM revealed that the rod OS length shrinkage was correlated to the light-driven decrease of the space between individual discs, not the disc thickness itself.

Translational Relevance

Light-induced transient rod response promises a noninvasive biomarker for early diagnosis of age-related macular degeneration and retinitis pigmentosa, in which the rod photoreceptors are known to be more vulnerable than cone photoreceptors.

Non-invasive assessment of human cone photoreceptor function

Vision begins when light isomerizes the photopigments within photoreceptors. Noninvasive cellular-scale observation of the structure of the human photoreceptor mosaic is made possible through the use of adaptive optics (AO) enhanced ophthalmoscopes, but establishing noninvasive objective measures of photoreceptor function on a similar scale has been more difficult. AO ophthalmoscope images acquired with near-infrared light show that individual cone photoreceptor reflectance can change in response to a visible stimulus. Here we show that the intrinsic response depends on stimulus wavelength and intensity, and that its action spectrum is well-matched to the spectral sensitivity of cone-mediated vision. Our results demonstrate that the cone reflectance response is mediated by photoisomerization, thus making it a direct measure of photoreceptor function.

Comparative investigation of stimulus-evoked rod outer segment movement and retinal electrophysiological activity

Transient retinal phototropism (TRP) has been observed in rod photoreceptors activated by oblique visible light flashes. Time-lapse confocal microscopy and optical coherence tomography (OCT) revealed rod outer segment (ROS) movements as the physical source of TRP. However, the physiological source of TRP is still not well understood. In this study, concurrent TRP and electroretinogram (ERG) measurements disclosed a remarkably earlier onset time of the ROS movements (≤10 ms) than that (∼38 ms) of the ERG a-wave. Furthermore, low sodium treatment reversibly blocked the photoreceptor ERG a-wave, which is known to reflect hyperpolarization of retinal photoreceptors, but preserved the TRP associated rod OS movements well. Our experimental results and theoretical analysis suggested that the physiological source of TRP might be attributed to early stages of phototransduction, before the hyperpolarization of retinal photoreceptors.

Stimulus-evoked outer segment changes occur before the hyperpolarization of retinal photoreceptors

Transient retinal phototropism (TRP) has been predominantly observed in rod photoreceptors activated by oblique visible light stimulation. Dynamic confocal microscopy and optical coherence tomography (OCT) have revealed rod outer segment (ROS) movement as the physical source of TRP. However, the physiological source of ROS movement is still not well understood. In this study, concurrent near-infrared imaging of TRP and electroretinogram (ERG) measurement of retinal electrophysiology revealed that ROS movement occurs before the onset of the ERG a-wave, which is known to reflect the hyperpolarization of retinal photoreceptors. Moreover, substitution of normal superfusing medium with low-sodium medium reversibly blocked the photoreceptor ERG a-wave, but largely preserved the stimulus-evoked ROS movements. Our experimental results and theoretical analysis indicate that early, disc-based stages of the phototransduction cascade, which occur before the hyperpolarization of retinal photoreceptors, contribute to the TRP associated ROS movement.

Stimulus-evoked outer segment changes in rod photoreceptors

Rod-dominated transient retinal phototropism (TRP) has been recently observed in freshly isolated mouse and frog retinas. Comparative confocal microscopy and optical coherence tomography revealed that the TRP was predominantly elicited from the rod outer segment (OS). However, the biophysical mechanism of rod OS dynamics is still unknown. Mouse and frog retinal slices, which displayed a cross-section of retinal photoreceptors and other functional layers, were used to test the effect of light stimulation on rod OSs. Time-lapse microscopy revealed stimulus-evoked conformational changes of rod OSs. In the center of the stimulated region, the length of the rod OS shrunk, while in the peripheral region, the rod OS swung toward the center region. Our experimental observation and theoretical analysis suggest that the TRP may reflect unbalanced rod disc-shape changes due to localized visible light stimulation.

Intrinsic optical signal imaging of retinal physiology: a review

Intrinsic optical signal (IOS) imaging promises to be a noninvasive method for high-resolution examination of retinal physiology, which can advance the study and diagnosis of eye diseases. While specialized optical instruments are desirable for functional IOS imaging of retinal physiology, in depth understanding of multiple IOS sources in the complex retinal neural network is essential for optimizing instrument designs. We provide a brief overview of IOS studies and relationships in rod outer segment suspensions, isolated retinas, and intact eyes. Recent developments of line-scan confocal and functional optical coherence tomography (OCT) instruments have allowed in vivo IOS mapping of photoreceptor physiology. Further improvements of the line-scan confocal and functional OCT systems may provide a feasible solution to pursue functional IOS mapping of human photoreceptors. Some interesting IOSs have already been detected in inner retinal layers, but better development of the IOS instruments and software algorithms is required to achieve optimal physiological assessment of inner retinal neurons.

Functional optical coherence tomography enables in vivo physiological assessment of retinal rod and cone photoreceptors

Transient intrinsic optical signal (IOS) changes have been observed in retinal photoreceptors, suggesting a unique biomarker for eye disease detection. However, clinical deployment of IOS imaging is challenging due to unclear IOS sources and limited signal-to-noise ratios (SNRs). Here, by developing high spatiotemporal resolution optical coherence tomography (OCT) and applying an adaptive algorithm for IOS processing, we were able to record robust IOSs from single-pass measurements. Transient IOSs, which might reflect an early stage of light phototransduction, are consistently observed in the photoreceptor outer segment almost immediately (<4 ms) after retinal stimulation. Comparative studies of dark- and light-adapted retinas have demonstrated the feasibility of functional OCT mapping of rod and cone photoreceptors, promising a new method for early disease detection and improved treatment of diseases such as age-related macular degeneration (AMD) and other eye diseases that can cause photoreceptor damage.

A polarization-sensitive light field imager for multi-channel angular spectroscopy of light scattering in biological tissues

BACKGROUND

Angular spectroscopy of light scattering can be used for quantitative analysis of cellular and subcellular properties, and thus promises a noninvasive methodology for in vivo assessment cellular integrity to complement in vitro histological examination. Spatial information is essential for accurate identification of localized abnormalities. However, conventional angular spectroscopy systems only provide single-channel measurement, which suffers from poor spatial resolution or requires time-consuming scanning over extended area. The purpose of this study was to develop a multi-channel angular spectroscopy for light field imaging in biological tissues.

MATERIALS AND METHODS

A microlens array (MLA) (8×8) based light field imager for 64-channel angular spectroscopy was developed. A pair of crossed polarizers was employed for polarization-sensitive recording to enable quantitative measurement at high signal specificity and sensitivity. The polarization-sensitive light field imager enables rapid measurement of multiple sampling volumes simultaneously at 18 μm spatial-resolution and 3° angular-resolution. Comparative light field imaging and electrophysiological examination of freshly isolated and physiologically deteriorated lobster leg nerves have been conducted.

RESULTS

Two-dimensional (2D) polarization-sensitive scattering patterns of the fresh nerves were highly elliptical, while they gradually lost the ellipticity and became rotationally symmetric (i.e., circular) as the nerves physiologically deteriorated due to repeated electrical stimulations. Characterized parameters, i.e., the ellipticity and the scattering intensity, rendered spatially various characteristics such as different values and deteriorating rates.

CONCLUSIONS

The polarization-sensitive light field imager is able to provide multi-channel angular spectroscopy of light scattering with both spatial and angular resolutions. The light scattering properties of nerves are highly dependent on the orientation of nerves and their physiological status. Further development of polarization-sensitive multi-channel angular spectroscopy may promise a methodology for rapid and reliable identification of localized abnormalities in biological tissues.

Functional optical coherence tomography reveals transient phototropic change of photoreceptor outer segments

Dynamic near infrared microscopy has revealed transient retinal phototropism (TRP) correlated with oblique light stimulation. Here, by developing a hybrid confocal microscopy and optical coherence tomography (OCT), we tested sub-cellular source of the TRP in living frog retina. Dynamic confocal microscopy and OCT consistently revealed photoreceptor outer segments as the anatomic source of the TRP. Further investigation of the TRP can provide insights in better understanding of Stiles-Crawford effect (SCE) on rod and cone systems, and may also promise an intrinsic biomarker for early detection of eye diseases that can produce photoreceptor dysfunction.

Optical imaging of human cone photoreceptors directly following the capture of light

Capture of light in the photoreceptor outer segment initiates a cascade of chemical events that inhibit neurotransmitter release, ultimately resulting in vision. The massed response of the photoreceptor population can be measured non-invasively by electrical recordings, but responses from individual cells cannot be measured without dissecting the retina. Here we used optical imaging to observe individual human cones in the living eye as they underwent bleaching of photopigment and associated phototransduction. The retina was simultaneously stimulated and observed with high intensity visible light at 1 kHz, using adaptive optics. There was marked variability between individual cones in both photosensitivity and pigment optical density, challenging the conventional assumption that photoreceptors act as identical subunits (coefficient of variation in rate of photoisomerization = 23%). There was also a pronounced inverse correlation between these two parameters (p<10(-7)); the temporal evolution of image statistics revealed this to be a dynamic relationship, with cone waveguiding efficiency beginning a dramatic increase within 3 ms of light onset. Beginning as early as 2 ms after light onset and including half of cells by ∼7 ms, cone intensity showed reversals characteristic of interference phenomena, with greater delays in reversal corresponding to cones with more photopigment (p<10(-3)). The timing of these changes is argued to best correspond with either the cessation of dark current, or to related events such as changes in intracellular cGMP. Cone intensity also showed fluctuations of high frequency (332±25 Hz) and low amplitude (3.0±0.85%). Other groups have shown similar fluctuations that were directly evoked by light; if this corresponds to the same phenomenon, we propose that the amplitude of fluctuation may be increased by the use of a bright flash followed by a brief pause, to allow recovery of cone circulating current.

En face optical coherence tomography of transient light response at photoreceptor outer segments in living frog eyecup

This study was designed to test the feasibility of en face mapping of the transient intrinsic optical signal (IOS) response at photoreceptor outer segments and to assess the effect of spatial resolution on functional IOS imaging of retinal photoreceptors. A line-scan optical coherence tomography (LS-OCT) was constructed to achieve depth-resolved functional IOS imaging of living frog eyecups. Rapid en face OCT revealed transient IOS almost immediately (<3 ms) after the onset of visible light flashes at photoreceptor outer segments. Quantitative analysis indicated that the IOS kinetics may reflect dynamics of G-protein binding and releasing in early phases of visual transduction, and high resolution is essential to differentiate positive and negative IOS changes in adjacent locations.

Dynamic near-infrared imaging reveals transient phototropic change in retinal rod photoreceptors

Stiles-Crawford effect (SCE) is exclusively observed in cone photoreceptors, but why the SCE is absent in rod photoreceptors is still a mystery. In this study, we employed dynamic near infrared light imaging to monitor photoreceptor kinetics in freshly isolated frog and mouse retinas stimulated by oblique visible light flashes. It was observed that retinal rods could rapidly (onset: ∼10 ms for frog and 5 ms for mouse; time-to-peak: ∼200 ms for frog and 30 ms for mouse) shift toward the direction of the visible light, which might quickly compensate for the loss of luminous efficiency due to oblique illumination. In contrast, such directional movement was negligible in retinal cones. Moreover, transient rod phototropism could contribute to characteristic intrinsic optical signal (IOS). We anticipate that further study of the transient rod phototropism may not only provide insight into better understanding of the nature of vision but also promise an IOS biomarker for functional mapping of rod physiology at high resolution.

In vivo confocal intrinsic optical signal identification of localized retinal dysfunction

PURPOSE

The purposes of this study were to investigate the physiological mechanism of stimulus-evoked fast intrinsic optical signals (IOSs) recorded in dynamic confocal imaging of the retina, and to demonstrate the feasibility of in vivo confocal IOS mapping of localized retinal dysfunctions.

METHODS

A rapid line-scan confocal ophthalmoscope was constructed to achieve in vivo confocal IOS imaging of frog (Rana pipiens) retinas at cellular resolution. In order to investigate the physiological mechanism of confocal IOS, comparative IOS and electroretinography (ERG) measurements were made using normal frog eyes activated by variable-intensity stimuli. A dynamic spatiotemporal filtering algorithm was developed to reject the contamination of hemodynamic changes on fast IOS recording. Laser-injured frog eyes were employed to test the potential of confocal IOS mapping of localized retinal dysfunctions.

RESULTS

Comparative IOS and ERG experiments revealed a close correlation between the confocal IOS and retinal ERG, particularly the ERG a-wave, which has been widely used to evaluate photoreceptor function. IOS imaging of laser-injured frog eyes indicated that the confocal IOS could unambiguously detect localized (30 μm) functional lesions in the retina before a morphological abnormality is detectable.

CONCLUSIONS

The confocal IOS predominantly results from retinal photoreceptors, and can be used to map localized photoreceptor lesion in laser-injured frog eyes. We anticipate that confocal IOS imaging can provide applications in early detection of age-related macular degeneration, retinitis pigmentosa, and other retinal diseases that can cause pathological changes in the photoreceptors.

Comparative intrinsic optical signal imaging of wild-type and mutant mouse retinas

Functional measurement is important for retinal study and disease diagnosis. Transient intrinsic optical signal (IOS) response, tightly correlated with functional stimulation, has been previously detected in normal retinas. In this paper, comparative IOS imaging of wild-type (WT) and rod-degenerated mutant mouse retinas is reported. Both 2-month and 1-year-old mice were measured. In 2-month-old mutant mice, time course and peak value of the stimulus-evoked IOS were significantly delayed (relative to stimulus onset) and reduced, respectively, compared to age matched WT mice. In 1-year-old mutant mice, stimulus-evoked IOS was totally absent. However, enhanced spontaneous IOS responses, which might reflect inner neural remodeling in diseased retina, were observed in both 2-month and 1-year-old mutant retinas. Our experiments demonstrate the potential of using IOS imaging for noninvasive and high resolution identification of disease-associated retinal dysfunctions. Moreover, high spatiotemporal resolution IOS imaging may also lead to advanced understanding of disease-associated neural remodeling in the retina.

Alkylated hydroxylamine derivatives eliminate peripheral retinylidene Schiff bases but cannot enter the retinal binding pocket of light-activated rhodopsin

Besides Lys-296 in the binding pocket of opsin, all-trans-retinal forms adducts with peripheral lysine residues and phospholipids, thereby mimicking the spectral and chemical properties of metarhodopsin species. These pseudophotoproducts composed of nonspecific retinylidene Schiff bases have long plagued the investigation of rhodopsin deactivation and identification of decay products. We discovered that, while hydroxylamine can enter the retinal binding pocket of light-activated rhodopsin, the modified hydroxylamine compounds o-methylhydroxylamine (mHA), o-ethylhydroxylamine (eHA), o-tert-butylhydroxylamine (t-bHA), and o-(carboxymethyl)hydroxylamine (cmHA) are excluded. However, the alkylated hydroxylamines react quickly and efficiently with exposed retinylidene Schiff bases to form their respective retinal oximes. We further investigated how t-bHA affects light-activated rhodopsin and its interaction with binding partners. We found that both metarhodopsin II (Meta II) and Meta III are resistant to t-bHA, and neither arrestin nor transducin binding is affected by t-bHA. This discovery suggests that the hypothetical solvent channel that opens in light-activated rhodopsin is extremely stringent with regard to size and/or polarity. We believe that alkylated hydroxylamines will prove to be extremely useful reagents for the investigation of rhodopsin activation and decay mechanisms. Furthermore, the use of alkylated hydroxylamines should not be limited to in vitro studies and could help elucidate visual signal transduction mechanisms in the living cells of the retina.

Microlens array recording of localized retinal responses

We designed a rapid functional imager for the parallel recording of localized intrinsic optical signals (IOSs). This imager used a microlens array (MLA)-based illuminator to deliver visible stimulus light and near-infrared (NIR) recording light simultaneously. The parfocal configuration of the stimulus and recording light illumination enabled confocal recording of the stimulus-evoked IOSs. Because the MLA stimulation/recording spots were widely separated on the retina, and only the photoreceptors within the MLA stimulation/recording spots were stimulated, the potential IOS cross talk effect among neighboring retinal areas was minimized. Our experiments revealed robust IOS activities tightly correlated with localized retinal responses.

Sensitive light scattering probe of enzymatic processes in retinal rod photoreceptor membranes

Light excitation of as little as 0.05% of the rhodopsin in a retinal rod membrane suspension reduces the near-IR optical transmission by 25%. This transmission decrease requires the presence of guanosine triphosphate, is opposite in sign and 25 times larger in amplitude than a GTP-dependent light-scattering signal previously reported in rod outer segment suspensions [Kuhn, H., Bennett, N., Michel-Vallez, M. & Chabre, M. (1981) Proc. Natl. Acad. Sci. USA, 78, 6873-6877], and is kinetically complex. The initial phase of the optical transmission decrease begins after about a 50-ms lag (at 0.05% bleach) and has a first-order time constant of 300-500 ms. The scattering signal returns to the preactinic baseline in a time dependent on the amount of GTP added. A nonhydrolyzable GTP analogue, guanylyl imidodiphosphate, produces a scattering signal that does not return to the preactinic baseline. Adenosine triphosphate strongly inhibits the return of the GTP-dependent transmission decrease to the preactinic baseline. This effect of ATP on the GTP signal apparently requires ATP hydrolysis because it is inhibited by the simultaneous presence of adenylyl imidodiphosphate, a nonhydrolyzable analogue of ATP. The light-scattering signal and the velocity of the activation of a rod outer segment phosphodiesterase saturate when >0.05% of the rhodopsin is bleached and both show nearly identical dependence on light stimulus. It is suggested that these nucleotide-dependent light-scattering signals arise from changes in the state of membrane aggregation that are controlled by enzymatic processes. This hypothesis is supported by the large amplitude of the signals, sedimentation experiments, and a strong membrane concentration dependence. The ATP effects can be rationalized within the above hypothesis as being due to ATP-dependent rhodopsin phosphorylation that adds negative charges to the membrane surface and tends to keep the membranes disaggregated. An additional signal, which increases light transmission, is produced by a second, much more intense flash. The latter signal is interpreted as the result of proton binding by bleached rhodopsin molecules that decreases the negative charge repulsion between the membranes and allows increased aggregation.

High spatiotemporal resolution imaging of fast intrinsic optical signals activated by retinal flicker stimulation

High resolution monitoring of stimulus-evoked retinal neural activities is important for understanding retinal neural mechanisms, and can be a powerful tool for retinal disease diagnosis and treatment outcome evaluation. Fast intrinsic optical signals (IOSs), which have the time courses comparable to that of electrophysiological activities in the retina, hold the promise for high resolution imaging of retinal neural activities. However, application of fast IOS imaging has been hindered by the contamination of slow, high magnitude optical responses associated with transient hemodynamic and metabolic changes. In this paper we demonstrate the feasibility of separating fast retinal IOSs from slow optical responses by combining flicker stimulation and dynamic (temporal) differential image processing. A near infrared flood-illumination microscope equipped with a high-speed (1000 Hz) digital camera was used to conduct concurrent optical imaging and ERG measurement of isolated frog retinas. High spatiotemporal resolution imaging revealed that fast IOSs could follow flicker frequency up to at least 6 Hz. Comparable time courses of fast IOSs and ERG kinetics provide evidence that fast IOSs are originated from stimulus activated retinal neurons.

Intrinsic optical signal imaging of retinal activation

Fast intrinsic optical signals (IOSs) correlated with stimulus-activated retinal responses are reviewed. Fast IOSs have a time course comparable to the stimulus-evoked electrophysiological kinetics of the retina, and thus promise a new methodology for high-resolution evaluation of the physiological health of the retina. However, practical application of fast IOSs for retinal study and diagnosis is challenging because of their low sensitivity and limited specificity. Using isolated amphibian retinas, a series of experiments to optimize and characterize fast IOSs has been conducted. Fast, high-resolution nearinfrared light imaging disclosed both positive (increasing) and negative (decreasing) optical responses in adjacent retinal areas, which satisfied spatial resolution essential to the differentiation of IOSs from opposite polarities. At the subcellular (approximately microm) level, fast IOSs often exceeded 5% DeltaI/I, where I is the dynamic optical change, and I is the background light intensity. Experiments with isolated frog retinas suggest that negative IOSs stem primarily from the photoreceptor layer, while positive IOSs come from inner retinal layers.

Optical dissection of stimulus-evoked retinal activation

Better understanding of stimulus-evoked intrinsic optical signals (IOSs) in the retina promises new methodology for study and diagnosis of retinal function. Using a flood-illumination near infrared (NIR) light microscope equipped with high-speed CCD (80 Hz) and CMOS (1000 Hz) cameras, we validated depth-resolved enface imaging of fast IOSs in isolated retina of leopard frog. Both positive (increasing) and negative (decreasing) IOSs were observed at the photoreceptor and inner layers of the retina. The distribution of IOSs with opposite polarities showed a center-surround pattern. At the photoreceptor layer, negative IOSs dominated the center area illuminated by the stimulus light spot, while positive signals dominated the surrounding area. In contrast, at inner retinal layers, positive IOSs dominated the center area covered by the stimulus light spot, and negative IOSs were mainly observed in the surrounding area. Fast CMOS imaging disclosed rapid IOSs within 5 ms after the stimulus onset, and both ON and OFF optical responses were observed associated with a step light stimulus.

FDTD simulation of electromagnetic wave scattering from retina cells

Finite Difference Time Domain (FDTD) method was developed to model changes in the light scattering properties of retinal photoreceptors resulting from the functional response of living retina to external light stimulation. Physiological processes such as membrane hyper-polarization and conformation changes of rhodopsin in the photoreceptors outer segment (OS) were simulated by varying the optical properties of the cell organelles. The FDTD code was validated by comparing the results from a 2D simulation of light scattering from an infinite cylinder to the Mie analytical solution for the same geometry. Results from the FDTD simulations show that hyper-polarization of the outer cell membrane is the least likely cause for the observed increase in light scattering in photoreceptors. Other computational data suggests that the experimentally observed changes in reflectivity are most likely related to cell dynamics and to cell volume changes.

In vivo functional imaging of human cone photoreceptors

We evaluate a novel non-invasive optical technique for observing fast physiological processes, in particular phototransduction, in single photoreceptor cells in the living human eye. The method takes advantage of the interference of multiple reflections within the outer segments (OS) of cones. This self-interference phenomenon is highly sensitive to phase changes such as those caused by variations in refractive index and scatter within the photoreceptor cell. A high-speed (192 Hz) flood-illumination retina camera equipped with adaptive optics (AO) is used to observe individual photoreceptors, and to monitor changes in their reflectance in response to visible stimuli ("scintillation"). AO and high frame rates are necessary for resolving individual cones and their fast temporal dynamics, respectively. Scintillation initiates within 5 to 10 ms after the onset of the stimulus flash, lasts 300 to 400 ms, is observed at visible and near-infrared (NIR) wavelengths, and is highly sensitive to the coherence length of the imaging light source. To our knowledge this is the first demonstration of in vivo optical imaging of the fast physiological processes that accompany phototransduction in individual photoreceptors.

Optophysiology: depth-resolved probing of retinal physiology with functional ultrahigh-resolution optical coherence tomography

Noncontact, depth-resolved, optical probing of retinal response to visual stimulation with a <10-microm spatial resolution, achieved by using functional ultrahigh-resolution optical coherence tomography (fUHROCT), is demonstrated in isolated rabbit retinas. The method takes advantage of the fact that physiological changes in dark-adapted retinas caused by light stimulation can result in local variation of the tissue reflectivity. fUHROCT scans were acquired from isolated retinas synchronously with electrical recordings before, during, and after light stimulation. Pronounced stimulus-related changes in the retinal reflectivity profile were observed in the inner/outer segments of the photoreceptor layer and the plexiform layers. Control experiments (e.g., dark adaptation vs. light stimulation), pharmacological inhibition of photoreceptor function, and synaptic transmission to the inner retina confirmed that the origin of the observed optical changes is the altered physiological state of the retina evoked by the light stimulus. We have demonstrated that fUHROCT allows for simultaneous, noninvasive probing of both retinal morphology and function, which could significantly improve the early diagnosis of various ophthalmic pathologies and could lead to better understanding of pathogenesis.

Electrostatic properties of membrane lipids coupled to metarhodopsin II formation in visual transduction

Changes in lipid composition have recently been shown to exert appreciable influences on the activities of membrane-bound proteins and peptides. We tested the hypothesis that the conformational states of rhodopsin linked to visual signal transduction are related to biophysical properties of the membrane lipid bilayer. For bovine rhodopsin, the meta I-meta II conformational transition was studied in egg phosphatidylcholine (PC) recombinants versus the native rod outer segment (ROS) membranes by means of flash photolysis. Formation of metarhodopsin II was observed by the change in absorbance at 478 nm after a single actinic flash was delivered to the sample. The meta I/meta II ratio was investigated as a function of both temperature and pH. The data clearly demonstrated thermodynamic reversibility of the transition for both the egg PC recombinants and the native ROS membranes. A significant shift of the apparent pK(a) for the acid-base equilibrium to lower values was evident in the egg PC recombinant, with little meta II produced under physiological conditions. Calculations of the membrane surface pH using a Poisson-Boltzmann model suggested the free energies of the meta I and meta II states were significantly affected by electrostatic properties of the bilayer lipids. In the ROS membranes, phosphatidylserine (PS) is needed for full formation of meta II, in combination with phosphatidylethanolamine (PE) and polyunsaturated docosahexaenoic acid (DHA; 22:6omega3) chains. We propose that the PS surface potential leads to an accumulation of hydronium ions, H(3)O(+), in the electrical double layer, which drive the reaction together with the large negative spontaneous curvature (H(0)) conferred by PE plus DHA chains. The elastic stress/strain of the bilayer arises from an interplay of the approximately zero H(0) from PS and the negative H(0) due to the PE headgroups and polyunsaturated chains. The lipid influences are further explained in terms of matching of the bilayer spontaneous curvature to the curvature at the lipid/rhodopsin interface, as formulated by the Helfrich bending energy. These new findings guide current ideas as to how bilayer properties govern the conformational energetics of integral membrane proteins. Moreover, they yield knowledge of how membrane lipid-protein interactions involving acidic phospholipids such as PS and neutral polyunsaturated DHA chains are implicated in key biological functions such as vision.

G proteins and phototransduction

Phototransduction is the process by which a photon of light captured by a molecule of visual pigment generates an electrical response in a photoreceptor cell. Vertebrate rod phototransduction is one of the best-studied G protein signaling pathways. In this pathway the photoreceptor-specific G protein, transducin, mediates between the visual pigment, rhodopsin, and the effector enzyme, cGMP phosphodiesterase. This review focuses on two quantitative features of G protein signaling in phototransduction: signal amplification and response timing. We examine how the interplay between the mechanisms that contribute to amplification and those that govern termination of G protein activity determine the speed and the sensitivity of the cellular response to light.

A novel photointermediate of octopus rhodopsin activates its G-protein

The photointermediate of octopus rhodopsin responsible for G-protein activation was examined by a GTPgammaS-binding assay in a reconstituted system with purified rhodopsin and photoreceptor G-protein. When octopus rhodopsin alone was incubated in the dark after illumination, its ability to stimulate GTPgammaS-binding by the G-protein decreased in a time-dependent manner. We associate this decay with the decay of a novel photointermediate, transient acid metarhodopsin, which lies between mesorhodopsin and acid metarhodopsin. Spectroscopic evidence for its existence was suggested by its effects on the turbidity of the vesicles. These results suggest that the transient acid metarhodopsin, not the stable final photoproduct, acid metarhodopsin, activates a G-protein in octopus photoreceptors.

Characterization of rhodopsin mutants that bind transducin but fail to induce GTP nucleotide uptake. Classification of mutant pigments by fluorescence, nucleotide release, and flash-induced light-scattering assays

The photoreceptor rhodopsin is a seven-transmembrane helix receptor that activates the G protein transducin in response to light. Several site-directed rhodopsin mutants have been reported to be defective in transducin activation. Two of these mutants bound transducin in response to light, but failed to release the bound transducin in the presence of GTP (Franke, R. R., König, B., Sakmar, T. P., Khorana, H. G., and Hofmann, K. P. (1990) Science 250, 123-125). The present study was carried out to determine the nucleotide-binding state of transducin as it interacts with rhodopsin mutants. Five mutant bovine opsin genes were prepared by site-specific mutagenesis. Three mutant genes had deletions from one cytoplasmic loop each: AB delta 70-71; CD delta 143-150; and EF delta 237-249. Two additional loop CD mutant genes were prepared: E134R/R135E had a reversal of a conserved charge pair, and CD r140-152 had a 13-amino acid sequence replaced by a sequence derived from the amino-terminal tail. Three types of assays were carried out: 1) a fluorescence assay of photoactivated rhodopsin (R*)-dependent guanosine 5'-O-(3-thiotriphosphate) uptake by transducin, 2) an assay of R*-dependent release of labeled GDP from the alpha-subunit of transducin holoenzyme (Gt alpha).GDP, and 3) a light-scattering assay of R*.Gt complex formation and dissociation. We show that the mutant pigments, which are able to bind transducin in a light-dependent manner but lack the ability to activate transducin, most likely form R*.Gt alpha beta gamma.GDP complexes that are impaired in GDP release.

cGMP phosphodiesterase dependent light-induced scattering changes in suspensions of retinal disc membranes

Light-induced GTP-dependent scattering changes are studied in suspensions of retinal disc membranes to which one or both of the purified proteins involved in the phototransduction mechanism (G-protein and cGMP phosphodiesterase) are reassociated; a scattering change which depends on the presence of both G-protein (G) and inhibited cGMP phosphodiesterase (PDE) and on an ATPase-dependent process, previously described in Bennett [(1986) Eur. J. Biochem. 157, 487-495] is compared to the signal observed in the absence of PDE or of ATP and to PDE activity. The same signal can also be induced either in the dark or in the light by addition of preactivated G in the presence of inhibited PDE. This PDE-dependent scattering change is composed of two components (fast and slow); the variation of the amplitude and kinetics of both components with PDE or G concentration is similar to the variation of the active PDE state with two activator GGTP molecules (G with GTP bound), calculated with dissociation constants previously reported for the interaction between GGTP and PDE [Bennett, N., & Clerc, A. (1989) Biochemistry 28, 7418-7424]. The two components are therefore proposed to be associated with processes which depend on the formation of the active PDE state with two activators.

Reaction rate and collisional efficiency of the rhodopsin-transducin system in intact retinal rods

A model of transducin activation is constructed from its partial reactions (formation of metarhodopsin II, association, and dissociation of the rhodopsin-transducin complex). The kinetic equations of the model are solved both numerically and, for small photoactivation, analytically. From data on the partial reactions in vitro, rate and activation energy profile of amplified transducin turnover are modeled and compared with measured light-scattering signals of transducin activation in intact retinal rods. The data leave one free parameter, the rate of association between transducin and rhodopsin. Best fit is achieved for an activation energy of 35 kJ/mol, indicating lateral membrane diffusion of the proteins as its main determinant. The absolute value of the association rate is discussed in terms of the success of collisions to form the catalytic complex. It is greater than 30% for the intact retina and 10 times lower after permeabilization with staphylococcus aureus alpha-toxin. Dissociation rates for micromolar guanosinetriphosphale (GTP) (Kohl, B., and K. P. Hofmann, 1987. Biophys. J. 52:271-277) must be extrapolated linearly up to the millimolar range to explain the rapid transducin turnover in situ. This is interpreted by an unstable rhodopsin-transducin-GTP transient state. At the time of maximal turnover after a flash, the rate of activation is determined as 30, 120, 800, 2,500, and 4,000 activated transducins per photoactivated rhodopsin and second at 5, 10, 20, 30, 37 degrees C, respectively.

Optical probes of intradiskal processes in rod photoreceptors. II: Light-scattering study of ATP-dependent light reactions

Rod outer segment (ROS) disks, either stacked or freely floating, respond to flash illumination to yield a specific, ATP-dependent, light-scattering signal AL. In broken ROS AL signals occur only when AD signals have preceded them. The degree to which the preceding AD signal has been completed determines the amplitude of the following AL signal. However, in freshly detached ROS from dark-adapted frogs Al signals with maximal size can be obtained without pre-incubation with exogenous ATP. The energized state, which is restored in broken ROS with the help of ATP, appears to prevail in the living retina and must therefore be considered to be "physiological". AL signals require structurally intact disks. Neither peripheral ROS proteins nor connecting filaments between adjacent disks are necessary. Their structural origin is the same as that of the preceding AD signal, i.e. osmotic disk swelling. AL signals consist of a single slow kinetic component (half-life 10 s at room temperature) and multiphase fast kinetic component (70 ms). The slow phase corresponds to a light-stimulated resumption of ATPase activity (this has been dealt with in a previous paper) whereas the fast component reflects an immediate response of the energized disk to the metarhodopsin I to metarhodopsin II transition. The latter effect is the subject of this paper. A variety of experiments, using different ATPase inhibitors, ionophores and membrane-permeable salts, have been carried out; they are all consistent with notion that AL originates in the disk interior and probes the existence of a proton electrochemical potential difference delta mu (H+) across the disk membrane. A model is presented which can explain all given properties of AL satisfactorily. According to this model the photolysis of rhodopsin causes a proton release in the disk lumen. This, in turn, results in osmotic swelling of the disks, provided that the internal buffer sites have been (at least partially) titrated with protons prior to the flash. Such conditions, i.e. a low internal pH, are provided by the proton transport across the disk membrane, which presumably takes place during the course of the preceding AD signal.

Optical probes of intradiskal processes in rod photoreceptors. I: Light-scattering study of ATP-dependent dark reactions

ATP can cause dramatic structural changes in the outer segment of rod photoreceptors. These changes can be visualized by means of a concomitant light-scattering signal AD, a decrease in scattered light intensity of over 20%. The large size of the signal suggests that major structural changes occur. The underlying molecular events may reflect an important, yet still unknown, part of the photoreceptor machinery. AD signals reflect ATPase-driven transmembrane events which occur in and at the disk membrane. Their only structural prerequisite is the structural integrity of the disk compartment. The angular dependence of AD, which can be mimicked by an osmotically-induced disk-swelling, suggests that the disk compartment swells during the production of the AD signal. AD signals proceed with first-order kinetics (half-life = 1 min at 20 degrees C and ATP concentrations of greater than 100 microM) and are accompanied by the hydrolysis of approximately 4 mol ATP (mol rhodopsin)-1. The AD signal is inhibited by a number of transport ATPase inhibitors (quercetin, NBD.Cl, vanadate, DCCD), but not by oligomycin, azide and ouabain. The sensitivity to DCCD, together with the fact that except magnesium no other cation has to be present, points to a proton translocation. This proton transport appears to be electrogenic, since AD signals require the presence of a permeant anion. In physiological saline this is chloride, and the chloride flux is facilitated by a DIDS-sensitive anion transport unit in the disk membrane.

Photic modulation of a highly sensitive, near-infrared light-scattering signal recorded from intact retinal photoreceptors

On stimulation by green flashes, the isolated, aspartate-treated bovine retina exhibits transient changes in the scattering of near-infrared (880 nm) light. A single component, termed the "ATR" (a flash-induced scattering signal, where ATR designates amplified transient-retina), dominates the amplitude and rising-phase kinetics of the initial peak of the light-scattering response. Superfusion with physiological solution containing low Na+ concentration reversibly abolishes the photoreceptor electroretinographic response but preserves the ATR signal, indicating a receptoral origin for the ATR. The increase of ATR amplitude (A/Amax) with flash intensity (R*/R, where R indicates rhodopsin) is described by A/Amax = (1- e-kR*/R), with R*/R = k-1 occurring on generation of approximately two photoactivated rhodopsins (R*s) per disc surface in the rod outer segment. Weak background light and bright flashes reversibly depress the ATR. Kinetic and sensitivity data suggest a basis of the ATR in stochastic, unit activation events, each initiated by a single R*. They further suggest an essential invariance of the unit event under differing conditions of illumination. A delay, apparently governed by the lifetime of a light-activated substance regulating ATR generation, precedes ATR recovery after a bright flash. The flash dependence of the delay period indicates an upper limit of 3 s for the lifetime of R* in the ATR-generating process. The unit event appears to be an R*-catalyzed and disc-localized reaction of phototransduction.

Sub-second turnover of transducin GTPase in bovine rod outer segments. A light scattering study

A fast, regenerative light scattering signal from bovine ROS, the PA-signal, reflects the light-induced, transient activation of transducin. Its rate of recovery depends on the number of photolysed rhodopsin molecules, indicating that rhodopsin deactivation and not GTPase activity is rate limiting in our in vitro system. When rhodopsin deactivation is accelerated (in the presence of NH2OH), PA-signal recovery is also accelerated. A GTPase turnover number of more than 2 s-1 (at 37 degrees C) can be derived from these experiments. This is more than one order of magnitude faster than the GTPase rates so far described in the literature and is rapid enough for a physiological shut-off mechanism. The fast GTPase is attributed to a highly intact disk stack, which never releases transducin into the free aqueous space.

Kinetic study on the equilibrium between membrane-bound and free photoreceptor G-protein

Formation of the complex between photoreceptor G-protein (G) and photoactivated rhodopsin (RM) leads to a change in the light scattering of the disk membranes (binding signal or signal P). The signal measured on isolated disks (so-called PD signal) is exactly stoichiometric in its final level to bound G-protein but its kinetics are much slower than the RMG binding reaction. In this study on isolated disks, recombined with G-protein, we analyzed the PD-signal level and kinetics as a function of flash intensity and compared it to the RMG-complex formation monitored spectroscopically (by extra metarhodopsin II). The basic observation is that the initial slopes of the PD signals decrease with flash intensity when the signals are normalized to the same final level. This finding prevents an explanation of the scattering signal by a slow postponed reaction of the RMG complex. We propose to interpret the scattering change as a redistribution of G-protein between a membrane-bound and a solved state. The process is driven by the complexation of membrane-bound G to flash-activated rhodopsin (RM). The experimental evidence for this two-state model is the following: The intensity dependence of the initial rate of the PD signal is explained by the model. Under the assumption of a bimolecular reaction of free G with sites at the membrane, equal to rhodopsin in their concentration, the measured rates yield a KD of 10(-5) M. Evaluation of the extra MII kinetics yields a biphasic rise at saturating flashes. The measured rates fit to the supply of free and membrane-bound G-protein for the reaction with RM. Quantitative estimation of the expected scattering intensity changes gives a comprehensive description of binding signal and dissociation signal by the gain and loss of G-protein scattering mass. The temperature dependence of the PD-signal rate leads to an activation energy of the membrane-association process of E alpha = 44 kJ/mol.

A simple and rapid procedure for the isolation of intact bovine rod outer segments (ROS)

A method is described which allows the rapid isolation and purification of intact rod outer segments (ROS) from cattle eyes. It requires very fresh retinal material and can be completed within less than 2 h of the death of the animals. Cattle eyes are dissected in the usual manner, the retinae are isolated and the ROS are separated from the rest of the retina by gentle vortexing and filtration through a nylon mesh. The resulting crude ROS suspension is purified on a discontinuous sucrose density gradient. Two fractions are obtained, the major one consisting of mostly intact ROS, the minor one of RIS-ROS, i.e. of ROS which are still connected to part of their inner segment. The ROS are washed once and can be stored on ice for several days without loosing their intact plasma membrane. They can be transformed to leaky ROS by a quick freeze/thawing cycle or, if one wants unobstructed access to the interdiskal space, they can be subjected to a mild lysis treatment. The resulting ROS material is characterised using light microscopy, electron microscopy, light scattering, gel electrophoresis and absorption spectroscopy. It contains unusually low levels of 48k-protein and very high levels of G-protein. The latter cannot be washed out in the presence of GTP-gamma-S, even in the case of leaky ROS.

Mg2+-ATP induces filament growth from retinal rod outer segments with disrupted plasma membranes

Mg2+-ATP produces a large decrease in near-IR light scattering when added to suspensions of rod outer segments (ROS) when the plasma membranes have been disrupted by a gentle dialysis procedure. When this process is studied by light microscopy with video-enhanced image contrast, the Mg2+-ATP-dependent signal is seen to be associated with the formation of filaments which extend only from those ROS lacking plasma membranes. Both the IR light scattering signal and filament growth are inhibited by vanadate and DCCD but not by colchicine, colcemid or cytochalasins.

A functional link between the dark Mg-ATPase activity and the light-induced enzymatic cascade in rod outer segments

The characterization of a light-induced scattering change in suspensions of rod fragments, which requires previous swelling of the disks by the dark Mg-ATPase described by Uhl et al. [FEBS Lett. 107, 317-322 (1979)] is reported here. Reconstitution experiments demonstrate that this signal is dependent on the presence of G-protein, GTP and cGMP phosphodiesterase. Fast reversal associated with regenerability requires in addition the presence of some protein(s) of the cytoplasm (probably the rhodopsin kinase) and ATP. The amount of excited rhodopsin which saturates the signal is the same as that which saturates the previously described 'dissociation signal' [Kühn et al. (1981) Proc. Natl Acad. Sci. USA 78, 6873-6877] associated with the formation of the phosphodiesterase activator G alpha GTP (alpha subunit of the G-protein with GTP bound). The kinetics of the signal is slightly slower than that of the dissociation signal and its amplitude is proportional to the extent of swelling of the disks. These results suggest that the interaction between G alpha GTP and the phosphodiesterase modifies some structural feature of the disks and provide evidence for the existence of a functional link between the dark Mg-ATPase and the light-induced enzymatic cascade.

Light- and nucleotide-dependent binding of phosphodiesterase to rod disk membranes: correlation with light-scattering changes and vesicle aggregation

Under conditions in which large guanosine cyclic 3',5'-phosphate (cGMP)- and phosphodiesterase (PDE)-dependent changes in near-infrared transmission and vesicle aggregation and disaggregation occur, we have observed a striking change in the binding of PDE to rod disk membranes. The change in PDE binding is nucleotide and light dependent as are the light-scattering changes. The cGMP- and PDE-dependent light-scattering signal can be produced by a 500-nm light flash which bleaches 1/(1 X 10(7] rhodopsin molecules. Mg ions are an essential cofactor for the nucleotide-dependent PDE binding and light-scattering changes. 3-Isobutyl-1-methylxanthine and other competitive inhibitors of PDE hydrolytic activity support increased PDE binding to the disk membrane, vesicle aggregation, and the light-scattering signal. However, treatments which block GTP-dependent activation of PDE hydrolytic activity (colchicine, GDP, or ethylenediaminetetraacetic acid) also block these phenomena. Thus, GTP-dependent activation of PDE rather than its hydrolytic activity appears to be correlated with the light-scattering signal.

Permeability of rod outer segment disk membranes as probed by Ficoll density gradient centrifugation and by turbidimetry

Osmotic volume changes of isolated disks prepared from bovine rod outer segments were investigated utilizing the capacity of osmotically intact disks to float on 2.5% (w/v) Ficoll under hypotonic conditions. The amount of floating disks decreases steadily and approximately linearly when the osmolarity is increased stepwise with an osmotically active solute. The slope of the decrease becomes smaller for partially permeable substances and no decrease in observed for fully permeable solutes. All ions assayed by this method as well as sucrose were osmotically fully active to disk membranes. The buffer molecules Tris and imidazole partially penetrated the disk membranes at pH 7, whereas the zwitterionic buffer Hepes was impermeable. Ethanol showed absolutely no osmotic activity to disk membranes and, therefore, can easily penetrate these membranes. concurrent turbidimetric measurements and, therefore, can easily penetrate these membranes. Concurrent turbidimetric measurements confirmed these results. Upon prolonged exposure of disk membranes to 5% (w/v) Ficoll, a considerable modification of the osmotic properties of disk membranes is observed, indicating a significant interaction of 5% (w/v) Ficoll with disk membranes. No influence of 2.5% (w/v) Ficoll on the osmotic properties of disk membranes was detected. The restriction of the use of Ficoll for disk membrane preparative purposes will be discussed.