Is There a Third Photoreceptor Involved in the Control of Chloroplast Movements in Mougeotia?

The photometric method was used to test a possibility proposed recently that a new photoreceptor with maximum activity at 620 nm is involved in mediating chloroplast rotation in Mougeotia (Z Lechowski, J Bialczyk [1988] Plant Physiol 88: 189-193). The hypothesis was tested under conditions of continuous dichromatic unilateral or mutually perpendicular irradiation with red light of wavelengths 620 or 660 (680) nanometers and far-red. When the red light was polarized parallel to the long cell axis, chloroplast response could be monitored by changing the direction of far-red irradiation. The level of the response obtained with red and far-red applied from the same direction depended on far-red intensity: at higher fluence rates the maximum response was shifted to longer wavelengths of red light. A high fluence rate of far-red inhibited the response. The absorption coefficients of Mougeotia chloroplasts were measured for the studied wave-lengths using the microphotometric method. Possible impact of absorption by the chloroplast on photoreception has been discussed. Current and previous results can be interpreted in terms of phytochrome action and do not support the involvement of the hypothetical 620 nanometer photoreceptor.     

Splitting of Plasmon Frequency in Spherical Metal Nanoparticles in Anisotropic Medium

The problem of plasmon resonance in spherical metal nanoparticles incorporated into an anisotropic dielectric medium is studied theoretically. Analytic solution is obtained in long-wavelength approximation for the case of weak uniaxial anisotropy. It is shown that medium anisotropy causes shifts of plasmon frequency from its position in an isotropic medium, which are different for plasmons with dipole momenta parallel and perpendicular to the axis of the medium. For the parallel and perpendicular orientations, which are determined by polarization of incident light, plasmon shifts differ by a factor of 4/3. Analytic expressions for field enhancement in the vicinity of a metal nanoparticle is obtained and analyzed for the cases of noble metals. The perspectives of experimental check of the obtained results and possible applications of plasmon anisotropy in plasmonics and sensorics are discussed.     

The directional absorption properties of rhodopsin and its photoproducts.

The experimental data on the absorption of a plane polarised light by a solution of cattle rhodopsin at -196 degrees C have been theoretically analysed to model the directional absorption properties of rhodopsin and its photoproducts. It is seen that these molecules behave like planar absorbers having a ratio of about 100 : 7 between the extinction coefficients along the long axis and perpendicular to it. Using this result and the experimental observations on absorption and dichroism in the retina in situ, a model for the configuration of chromophores in the disc membranes has been derived. In this model the plane of the chromophore is perpendicular to that of the disc and the long axis of the chromophore makes an angle of 6.6 degrees with the plane of the disc. The solution of the problem depends on the assumption that the absorption axes are the same for the rhodopsin, prelumirhodopsin and isorhodopsin.     

The directional absorption properties of rhodopsin and its photoproducts

The experimental data on the absorption of a plane polarised light by a solution of cattle rhodopsin at −196‡ C have been theoretically analysed to model the directional absorption properties of rhodopsin and its photoproducts. It is seen that these molecules behave like planar absorbers having a ratio of about 100∶7 between the extinction coefficients along the long axis and perpendicular to it. Using this result and the experimental observations on absorption and dichroism in the retina in situ, a model for the configuration of chromophores in the disc membranes has been derived. In this model the plane of the chromophore is perpendicular to that of the disc and the long axis of the chromophore makes an angle of 6.6‡ with the plane of the disc. The solution of the problem depends on the assumption that the absorption axes are the same for the rhodopsin, prelumirhodopsin and isorhodopsin. Work partially supported by Department of Science and Technology (India)     

Bimodal Polarotropism of Vaucheria to Polarized Blue Light: Parallel Polarotropism at High Fluence Rate Corresponds to Negative Phototropism

Vaucheria (Xanthophyceae) exhibited cruciform polarotropism when they were grown under polarized white or blue light for several days. The coexistence of two groups of branches growing perpendicular and parallel to the electric vector (E-vector) resulted in cruciform polarotropic orientation. Such polarotropic bending was, however, not detected within 24 hr. As the fluence rate of polarized white or blue light increased, parallel orientation to the E-vector became dominant. Polarized red light produced exclusively perpendicular polarotropism. This shift in pattern was much obvious in V. terrestris sensu G?tz than V. sessllis and V. dichotoma. Since the photoperception is restricted to the tip of the apical dome and since this region receives maximum photons when the E-vector is at a right angle to the cell axis, Vaucheria becomes oriented normal to the E-vector as far as the fluence rate is optimum. The direction of growth is expected to change into parallel to the E-vector when the fluence rate is supraoptimum. The perpendicular (normal) and parallel polarotropism of Vaucheria, thus, correspond to positive and negative phototropism, respectively. Orientation of photoreceptor molecules is suggested to be predominantly parallel to the surface of the apical dome. Received 14 June 1999/ Accepted in revised form 19 November 1999     

Polarized Raman spectra of oriented fibers of A DNA and B DNA: anisotropic and isotropic local Raman tensors of base and backbone vibrations.

Polarized Raman spectra of oriented fibers of calf thymus DNA in the A and B conformations have been obtained by use of a Raman microscope operating in the 180 degrees back-scattering geometry. The following polarized Raman intensities in the spectral interval 200-1800 cm-1 were measured with both 514.5 and 488.0 nm laser excitations: (1) Icc, in which the incident and scattered light are polarized parallel to the DNA helical axis (c axis); (2) Ibb, in which the incident and scattered light are polarized perpendicular to c; and (3) Ibc and Icb, in which the incident and scattered light are polarized in mutually perpendicular directions. High degrees of structural homogeneity and unidirectional orientation were confirmed for both the A and B form fibers, as judged by comparison of the observed Raman markers and intensity anisotropies with measurements reported previously for oligonucleotide single crystals of known three-dimensional structures. The fiber Raman anisotropies have been combined with solution Raman depolarization ratios to evaluate the local tensors corresponding to key conformation-sensitive Raman bands of the DNA bases and sugar-phosphate backbone. The present study yields novel vibrational assignments for both A DNA and BDNA conformers and also confirms many previously proposed Raman vibrational assignments. Among the significant new findings are the demonstration of complex patterns of A form and B form indicator bands in the spectral intervals 750-900 and 1050-1100 cm-1, the identification of highly anisotropic tensors corresponding to vibrations of base, deoxyribose, and phosphate moieties, and the determination of relatively isotropic Raman tensors for the symmetrical stretching mode of phosphodioxy groups in A and B DNA. The present fiber results provide a basis for exploitation of polarized Raman spectroscopy to determine DNA helix orientation as well as to probe specific nucleotide residue orientations in nucleoproteins, viruses, and other complex biological assemblies.     

Efficiency of light diffraction by cross-striated muscle fibers under stretch and during isometric contraction.

When light is diffracted by a single frog muscle fiber the intensities I kappa of the different orders kappa (kappa = 1,2,3) strongly depend on the angle between the axis of the incident beam and the fiber axis. Maximum intensity is not obtained with perpendicular incidence (omega = 0 degree) but at angles that can be calculated for each order number and sarcomere length using Bragg's formula. In analogy to techniques developed for x-ray structure analysis of mosaic crystals we have rotated the fiber around an axis perpendicular to the fiber axis and to the incident beam axis within an angular range delta omega = +/- 35 degrees and recorded the light intensities I kappa. Diffraction efficiencies defined as E kappa = integral of I kappa d omega were studied as a function of sarcomere length and during isometric contraction. The sarcomere length dependences of the efficiencies E kappa of the first three orders show characteristic trends. E1 increases with fiber stretch, E2 has a minimum at a sarcomere length near 2.8 micrometers, and E3 has a maximum near 2.5 micrometers. These trends as well as the observed efficiency ratios are in fairly good agreement with predictions by the intensity formula developed for x-ray structure analysis. During isometric contraction, the diffraction efficiencies of the fiber decrease, with the decreases becoming greater the higher the order number. These decreases might be caused by a longitudinal displacement of myofibrils of up to 0.4 micrometers. The efficiency of light diffraction strongly depends on the tonicity of the bathing fluid. Hypertonic (3/2 x normal) solution reduces E1 to less than half, hypotonic (2/3 x normal) solution increases E1 to almost twice the value obtained in normal Ringer's solution.     

Angular and spectral sensitivity of fly photoreceptors. I. Integrated facet lens and rhabdomere optics

Three optical components of a fly's eye determine the angular sensitivity of the photoreceptors: the light diffracting facet lens, the wave-guiding rhabdomere and the light-absorbing visual pigment in the rhabdomere. How the integrated optical system of the fly eye shapes the angular sensitivity curves is quantitatively analyzed in five steps: (1) scalar diffraction theory for low Fresnel-number lenses is applied to four different facet lenses, with diameter 10, 20, 40, and 80 micro m, respectively, assuming a constant F-number of 2.2; (2) optical waveguide theory is used to calculate waveguide modes propagating in circular cylindrical rhabdomeres with diameter 1.0, 2.0, and 4.0 micro m, respectively; (3) the excitation of waveguide modes is studied with the tip of the waveguide positioned in the focal plane as well as outside this plane; (4) the light absorption from the various propagated modes by the visual pigment in the rhabdomere is calculated as a function of the angle of the incident light wave; and (5) the angular sensitivity of the photoreceptor is obtained by normalizing the total light absorption. Four wavelengths are considered: 300, 400, 500 and 600 nm. The analysis shows that the wavelength dependency of the lens diffraction is strongly compensated by that of the waveguide modes, an effect which is further enhanced by the decrease in light absorption when the mode number increases. The angular sensitivity of fly photoreceptors is robust to defocus and largely wavelength independent for all except very slender rhabdomeres.     

Optical third harmonic generation study of the hydration of DNA films.

Optical third harmonic generation (THG) has been observed for the first time from DNA films. The THG signal is observed from NaDNA films exposed to relative humidities (RHs) between 0% and 98%. A strong enhancement (approximately 5x) of the THG signal from NaDNA is observed at 84% RH; no enhancement is observed for RbDNA. The most likely mechanism for such an enhancement is an increased coherence length. A model calculation using estimates of the refractive indices at both the fundamental and third harmonic frequencies supports this interpretation. The observed THG signal has the same polarization as the incident (fundamental) light. For the A conformation, the THG signal polarized perpendicular to the helical axis is approximately twice as strong as the signal polarized parallel to the helical axis. No such anisotropy is observed for either the disordered conformation (below about 50% RH) or the B conformation (above 92% RH).     

ORIENTATION AND LOCUS OF TROPIC PHOTORECEPTOR MOLECULES IN SPORES OF BOTRYTIS AND OSMUNDA

Study of the tropic responses of Botrytis cinerea and Osmunda cinnamomea spores to blue light shows the photoreceptor molecules to be highly dichroic and oriented: in Botrytis their axes of maximum absorption lie perpendicular to the nearby cell surface; in Osmunda, parallel. The chief evidence lies in a comparison of their responses to plane polarized light—both germinate parallel to the vibration planes (defined by the axis of vibration of the electric vector and the axis of light propagation)—with those to partial illumination with unpolarized light: Botrytis grows from its brighter part; Osmunda, from its darker. The degree of orientation produced by polarized light corresponds, at high intensities, to that produced by the imposition of such large (about 100 per cent) intensity differences across a cell as to preclude all alternatives to oriented dichroic receptors. The photoreceptors of the Botrytis spore lie within the cell wall's inner half. The chief evidence lies in the component of its tropic responses to polarized light within the vibration plane: germination peaks about 10° off the vibration axis. This deviation arises from focusing which is effective only in the wall's inner half. At high intensities, anomalies appear in Botrytis which are interpreted as "centering," i.e., a tendency toward growth from the center of two or more equally illuminated points of a cell rather than from one of them.     

Color image detection by biomolecular photoreceptor using bacteriorhodopsin-based complex LB films

A biomolecular photoreceptor consisting of bacteriorhodopsin (bR)-based complex Langmuir–Blodgett (LB) films was developed for color image detection. By mimicking the functions of the pigments in retina of human visual system, biomolecules with photoelectric conversion function were chosen and used as constituents for an artificial photoreceptor. bR and flavin were deposited onto the patterned (9-pixelized) ITO glass by LB technique. A 9-pixel biomolecular photoreceptor was fabricated with a sandwich-type structure of ITO/LB films/electrolyte gel/Pt. Since each functional molecule shows its own response characteristic according to the light illumination in the visible region, the simplified knowledge-based algorithm for interpretation of the incident light wavelength (color) was proposed based on the basic rule describing the relationship between the photoelectric response characteristics and the incident light wavelength. When simple color images were projected onto the photoreceptor, the primary colors in visible light region, red, green, and blue were clearly recognized, and the projected color images were fairly well reproduced onto the color monitor by the proposed photoreceptor with the knowledge-based algorithm. It is concluded that the proposed device has a capability of recognizing the color images and can be used as a model system to simulate the information processing function of the human visual system.     

A quantitative model of Phycomyces phototropism

A quantitative model accounting for phototropism in the wild type and in behavioural mutants of Phycomyces is described.Photomecisms (changes in the sporangiophore's growth velocity in response to changes in light intensity) are produced by a system composed of two sets of linear transducers separated by an adaptation mechanism, the first transducer being the photoreceptor.Phototropism under asymmetrical light distributions is caused by the summation of local photomecisms in the distal half of the sporangiophore, where two bright bands are produced by refraction of the incident light. The photoreceptors turn around the sporangiophore axis; they are approximately adapted to local intensity everywhere except upon entrance to the first bright band. Thus, a continuous photomecism originates at this band while the rest of the sporangiophore remains practically unstimulated.The mutants suffer a reduction in the efficiency of transduction.The behaviour of the wild type and of the mutants has been quantitatively simulated by computer. The predictions from the model fit the experimental results.     

Calculations of scattered light from rigid polymers by Shifrin and Rayleigh-Debye approximations.

We show that the commonly used Rayleigh-Debye method for calculating light scattering can lead to significant errors when used for describing scattering from dilute solutions of long rigid polymers, errors that can be overcome by use of the easily applied Shifrin approximation. In order to show the extent of the discrepancies between the two methods, we have performed calculations at normal incidence both for polarized and unpolarized incident light with the scattering intensity determined as a function of polarization angle and of scattering angle, assuming that the incident light is in a spectral region where the absorption of hemoglobin is small. When the Shifrin method is used, the calculated intensities using either polarized or unpolarized scattered light give information about the alignment of polymers, a feature that is lost in the Rayleigh-Debye approximation because the effect of the asymmetric shape of the scatterer on the incoming polarized electric field is ignored. Using sickle hemoglobin polymers as an example, we have calculated the intensity of light scattering using both approaches and found that, for totally aligned polymers within parallel planes, the difference can be as large as 25%, when the incident electric field is perpendicular to the polymers, for near forward or near backward scattering (0 degrees or 180 degrees scattering angle), but becomes zero as the scattering angle approaches 90 degrees. For randomly oriented polymers within a plane, or for incident unpolarized light for either totally oriented or randomly oriented polymers, the difference between the two results for near forward or near backward scattering is approximately 15%.     

Experimental tendon repair: glycosaminoglycan arrangement in newly synthesized collagen fibers.

Changes in the macromolecular orientation and metachromasy of glycosaminoglycans (GAG) in newly synthesized and assembled collagen fibers in rat Achilles tendon after tendon excision were investigated in toluidine blue (TB)-stained preparations, based in the selective absorption of polarized light (= linear dichroism, LD) and of absorption of unpolarized light in situ. Extrinsic LD was observed microspectrophotometrically from the early phases of tendon repair onwards, although the absorption peaks in both parallel and perpendicular directions with respect to the plane of polarized light and the long axis of the collagen fibers occurred at the same wavelength, and thus differed from the pattern situation in normal adult controls. Compared to normal adult tendons, the pattern of LD in newly synthesized and assembled fibers was still not fully attained 110 days after surgical tendon removal. This incomplete recovery possibly reflected the influence of aging during the repair process. There was no correlation between LD and metachromasy. The highest absorption values for metachromatic staining occurred on the 7th day after tendon removal, at a time when LD was not intense. Treatment with hyaluronidase showed that the LD in the early stages of tendon repair was mostly due to hyaluronate whereas the LD in the later stages was due to chondroitin sulfates. The changes in LD during Achilles tendon repair were attributed to gradual modifications in the composition and macromolecular orientation of GAGs relative to the long axis of the collagen fibers.     

Effects of sodium azide on phototaxis of the blue-green alga Anabaena variabilis and consequences to the two-photoreceptor systems-hypothesis

Experiments with sodium azide support the earlier report that two different photoreceptor systems participate in the absorption of the phototactically active light in Anabaena variabilis. The one of them, represented by the phycobiliproteins and chlorophyll a, is responsible for positive and negative phototaxis around 440 nm and between 580 and 700 nm. This system is sensitive to sodium azide which is able to reverse the negative reaction at high fluence rates to a positive one. The second one which absorbs light between 500 and 560 nm and above 700 nm is insensitive to azide. It triggers only negative responses in absence and presence of azide as well. P750 is obviously not a photoreceptor pigment of this system, since there is no indication for its occurrence in Anabaena. Even photobleaching of the photosynthetic pigments at high fluence rates is prevented by azide. The noncyclic photosynthetic electron transport is not severely inhibited by azide because photokinesis is only in part impaired. Therefore, the hypothesis is suggested that the phototactic reaction-sign reversal generator of Anabaena is controlled by the level of an active oxygen species, probably singlet oxygen, which is quenched by azide.     

Green light reversal of blue-light-stimulated stomatal opening is found in a diversity of plant species

Reversal by green light of blue-light-stimulated stomatal opening was found across a number of plant species, including leguminous and nonleguminous dicots and grass and nongrass monocots. Simultaneous exposure to equal fluence rates of blue and green light resulted in ～50% reversal of normal blue light opening. Complete reversal occurred when the fluence rate of green light was approximately twice that of blue light. These results suggest that blue-green reversibility of stomatal opening is a basic photobiological property of guard cells. The blue-green reversibility of stomatal opening has been hypothesized to ensue from the cycling of two interconvertible, isomeric forms of the blue-light photoreceptor, zeaxanthin. Testing of blue-green reversibility could provide a valuable diagnostic tool for zeaxanthin-mediated blue-light photoperception.     

Phototropism and polarotropism of primary chloronemata of the moss Physcomitrella patens: responses of mutant strains

The phototropic and polarotropic responses of primary chloronemata grown from germinated minated spores of three mutant strains of the moss, Physcomitrella patens, have been studied and compared with those of the wild-type. The mutants and wild-type show the same qualitative tropic responses but differ with respect to the light conditions under which they are expressed. In both the wild-type and mutants the responses are controlled by phytochrome. In monochromatic red light, at low fluence rates, wild-type primary chloronemata grow positively phototropically in unidirectional light or perpendicular to the electrical vector (E) in polarised light; at high fluence rates growth in unidirectional light is lateral to the incident light or, in polarised light, parallel to E. The mutants, however, show only the lateral phototropic or parallel polarotropic responses at all fluence rates of red light tested. In far-red light, the wild-type primary chloronemata adopt a positive phototropic or a perpendicular polarotropic response; the mutants show the same responses but in a lower percentage of filaments. These results and those at other wavelengths indicate either that the mutants are impaired in their ability to adopt the positive phototropic and perpendicular polarotropic responses or that in the mutants the transition between the “low light” (positive phototropic-perpendicular polarotropic) and the “high light” (lateral phototropic-parallel polarotropic) responses is shifted to a lower photon fluence rate. Possible explanations of this phenotypic difference are discussed.     

LIGHT ABSORPTION AND QUANTUM YIELD FOR GROWTH IN FIVE SPECIES OF MARINE MACROALGA1

Light utilization efficiency in five species of marine macroalgae was measured in laboratory growth experiments (13–41 days duration) at different irradiances at 7°C. All species acclimated to irradiance by changing their light absorption, resulting in a peak in light absorption between 2 and 15 μmol·m^?2.s^?1. Light absorption increased with thallus-specific chlorophyll and carbon content according to linear inverse relationships between chlorophyll content (chlarea^?1) and log[transmission] and between log[carbon content, Carea^?1] and log[transmission]. Quantum yields for light-limited growth and estimated gross photosynthesis were calculated based on incident and absorbed light. Quantum yield for photosynthesis based on light absorbed by pigments was high (mean = 114 mmol C·mol^?1 photons) and similar among the species. Quantum yield for net growth based on incident light was also high but more variable, between 22 and 75 mmol C·mol^?1 photons. Differences among species were mainly due to differences in light absorption. In conclusion, all species acclimated to low light by increasing light absorption to the maximum attainable, and growth efficiencies based on absorbed light were close to the maximum theoretically possible.     

New evidence for the mechanism of phototactic orientation ofEuglena gracilis

When rotated horizontally in a cuvette in a strong lateral light beam, the flagellateEuglena gracilis effectively corrects its course and shows negative phototaxis, provided the angular velocity does not exceed 20⁰s^–1. Faster rotations cannot be corrected effeciently. In two strong light beams of equal illuminance perpendicular to each other, the cells move along the resultant away from the light beams. Decreasing the illuminance of one beam causes increasing numbers of the organisms to orient with respect to the stronger light source. In two perpendicular low illuminance beams (>200lx), the population splits into two components moving towards either light source. The percentage of cells in each component depends on the relative illuminances. The results can be explained by the shading hypothesis combined with a dichroic orientation of the photoreceptor molecules perpendicular to the long axis of the cells. Externally applied electric dc fields have no effect on positive or negative phototaxis; this supports the hypothesis that electrical potential changes are not involved in the sensory transduction chain of photoorientation inEuglena.