On the birefringence of rods and cones

Modern technologies for retinal scanning and imaging: an introduction for the biomedical engineer

This review article is meant to help biomedical engineers and nonphysical scientists better understand the principles of, and the main trends in modern scanning and imaging modalities used in ophthalmology. It is intended to ease the communication between physicists, medical doctors and engineers, and hopefully encourage “classical” biomedical engineers to generate new ideas and to initiate projects in an area which has traditionally been dominated by optical physics. Most of the methods involved are applicable to other areas of biomedical optics and optoelectronics, such as microscopic imaging, spectroscopy, spectral imaging, opto-acoustic tomography, fluorescence imaging etc., all of which are with potential biomedical application. Although all described methods are novel and important, the emphasis of this review has been placed on three technologies introduced in the 1990’s and still undergoing vigorous development: Confocal Scanning Laser Ophthalmoscopy, Optical Coherence Tomography, and polarization-sensitive retinal scanning.

Foveal dark adaptation, photopigment regeneration, and aging

Foveal dark adaptation in 58 subjects and photopigment regeneration in 60 subjects from 10-78 years of age exhibit parallel slowing of recovery rate with increasing age, with significant correlation of the two functions among individuals. The data are suggestive of an initial slight decline in rate before age 50, followed by a greater decline occurring at different ages in different individuals. Longitudinal data for one subject from age 40-65 show an increase in pigment regeneration time constant consistent with this idea. Foveal sensitivity and photopigment density both decrease with increasing age and are significantly correlated among individuals, although sensitivity declines more with age than does photopigment density. In contrast to earlier proposals based upon the Rushton-Dowling equation, we found no universal constant of proportionality to relate log relative threshold to photopigment within our population.

Birefringence of the human foveal area assessed in vivo with Mueller-matrix ellipsometry

We have assessed retinal birefringence in the foveal and parafoveal regions by applying Mueller matrix ellipsometry on the human eye in vivo. Basically, a light beam passed the ocular media twice and was scattered at the fundus intermediately. Keeping the entry and exit positions on the cornea constant and varying the retinal location along a circle around the foveal center enabled us to separate the corneal and retinal components of the measured retardation. We conclude that the retina within the outer margin of the parafovea behaves as a uniaxial crystal, with its slow axis radially oriented from the fovea and a retardation of about 16 deg (to 70 deg in the corneal center). We believe that Henle's fiber layer causes retardation in this specific configuration of entrance and exit beams. The outer segments of the photoreceptors, although birefringent, have their optic axes aligned with these beams.

Acid polysaccharide content of frog rod outer segments determined by metachromatic toluidine blue staining

Sulfonation of periodate-oxidized vicinal hydroxyl groups on a polysaccharide backbone allows binding of toluidine blue (aldehyde bisulfite-toluidine blue or ABT staining) with a concurrent metachromatic shift of the dye's absorption peak from 630 nm (monomer) to 580 nm (isolated dimer interaction at vicinal sulfonate groups) or 540 nm (dye polymer interaction). A molar absorptivity of 2.358 +/- 0.134 X 10(4) at 540 nm for polymeric toluidine blue O chloride (TB) aggregates was determined by spectrophotometry of TB bound to hyaluronic acid (HA) and sulfonated glycogen (SG) in water. Microspectrophotometry of ABT stained frog rod outer segments (FROS) showed spectra similar to TB in aqueous HA and SG solutions with absorbances corresponding to 0.063 M dye bound to sugar. Given two dye molecules bound per sugar residue and a rhodopsin concentration of 3.25 mM in FROS, the above indicates 10 stainable sugars per rhodopsin are contained in these cells. Half of these sugars are sensitive to hyaluronidase digestion implying 5 glycosaminoglycan (GAG) repeating units and 5 stainable oligosaccharide sugar residues per rhodopsin in FROS. The GAGs in FROS appear to be primarily HA. Birefringence measurements at 475 nm indicate that this HA and the oligosaccharide of rhodopsin are anisotropically oriented in these cells.

Propagation in a weakly anisotropic waveguide

In this communication we have considered propagation in a weakly anisotropic dielectric waveguide. It is shown that for a positive anisotropy the fractional power carried by the guide core increases over the isotropic case and that the anisotropy has an increasing effect as cutoff is approached. For negative anisotropy the effect is reversed. The increase in the fractional power varies linearly with the value of anisotropy with slope increasing as cutoff is approached. The degeneracy between the HE(n+1,m) and EH(n+1,m) modes present in the isotropic weakly guiding approximation is broken, and it is physically significant to distinguish between EH and HE modes. The anisotropy in retinal receptors (considered as dielectric waveguides) increases the stability of modal power with variation of the wavelength, although the effect is too small to explain the observation.

Dark ionic flux and the effects of light in isolated rod outer segments

We have determined the permeability properties of freshly isolated frog rod outer segments by observing their osmotic behavior in a simple continuous flow apparatus. Outer segments obtained by gently shaking a retina are sensitive but nonideal osmometers; a small restoring force prevents them from shrinking or swelling quite as much as expected for ideal behavior. We find that Na(+), Cl(-), No(3) (-), glycerol, acetate, and ammonium rapidly enter the outer segment, but K(+), SO(4) (=), and melezitose appear impermeable. The Na flux is rectified; for concentration gradients in the physiological range, 2 x 10(9) Na(+) ions/sec enter the outer segment, but we detect no efflux of Na(+), under our conditions, when the gradient is reversed. Illumination of the outer segment produces a specific increase in the resistance to Na(+) influx, but has no effect on the flux of other solutes. This light-dependent Na(+) resistance increases linearly with the number of rhodopsin molecules bleached. We find that excitation of a single rhodopsin molecule produces a transient ( approximately 1 sec) "photoresistance" which reduces the Na(+) influx by about 1%, thus preventing the entry of about 10(7) Na(+) ions. At considerably higher light levels, a stable afterimage resistance appears which reduces the Na influx by one-half when 10(6) rhodopsin molecules are bleached per rod. We have incorporated these findings into a model for the electrophysiological characteristics of the receptor.