LIGHT-INDUCED ABSORBANCE CHANGES IN CHLOROPLASTS AT -196°C*

Abstract— Absorbance changes induced by irradiating chloroplasts at — 196°C were measured in the region of 525–575 nm with a single-beam spectrophotometer. Irradiation at low temperature caused a bleaching at 556 nm due to oxidation of cytochrome b₅₅₉ but little or no change of cytochrome f. There occurred in addition a loss of absorbance at 547 nm and an increase at 543 nm. The bleaching at 547 nrn (and possibly the increase at 543 nm) could be induced chemically with dithionite or borohydride but not ascorbate. Subchloroplast particles with only Photosystem I activity showed no light-induced absorbance changes, while particles containing combined Photosystem I and Photosystem II activities showed the same changes as whole chloroplasts. Scenedesmus mutant No. 11 cells showed no absorbance changes while mutant No. 8 and wild-type cells showed the normal changes. It is concluded that the photooxidation of cytochrome b₅₅₉ and the photoreduction causing the bleaching at 547 nm are both mediated by Photosystem II.     

LASER FLASH PHOTOLYSIS OF RHODOPSIN AT ROOM TEMPERATURE

Abstract. Nanosecond flash photolysis of rhodopsin with 530 or 353 nm light produces an initial transient absorption spectrum with peaks at ˜57O and ˜420nm, and a subsequent transient species with a maximum absorption at 480 nm. These results are interpreted as the initial formation of prelumi-rhodopsin (570 nm) followed by its conversion to lumirhodopsin (470 nm). The peak at 420 nm in the first transient may be due to either hypsorhodopsin or isorhodopsin.     

ON THE SUMMATION OF QUANTA FOR THE PHOTOIONIZATION OF TYROSINE AND TRYPTOPHAN IN ALKALINE SOLUTIONS AT 80°K

Abstract— Some results of a study of the summation of quanta for the photoionization of tyrosine and tryptophan in frozen alkaline solution are presented. By means of a double-beam irradiation method it has been shown that the photoionization of aromatic amino acids in such solutions proceeds via a triplet state intermediate.     

UNSCHEDULED DNA SYNTHESIS IN FROG LENS AT 5°C

Abstract. Unscheduled DNA labeling occurs in the frog even at low temperatures. We conclude, tentatively, that the UV-induced labeling observed in these cold incubated lenses represents repair synthesis of DNA.     

PICOSECOND LASER PHOTOLYSIS OF SQUID RHODOPSIN AT ROOM AND LOW TEMPERATURES

Abstract. Squid rhodopsin extracted with 2% digitonin (pH 10.5 or 7.0) was excited with a 347 nm light pulse from a mode-locked ruby laser at room temperature. Within 19 ps after the excitation, absorbance at 430 nm due to hypsorhodopsin increased and subsequently decreased with a decay time of 45 ± 10 ps. Absorbance at 550 nm due to bathorhodopsin increased with a rise time of 50 ± 10 ps. These results are the first observations of hypsorhodopsin at room temperature and clearly show that hypsorhodopsin is a precursor of bathorhodopsin which has been considered to be the earliest photoproduct in the photobleaching process of rhodopsin.
Hypsorhodopsin appeared with a rise time of 70 ± 10 ps at 421 nm at liquid nitrogen temperature without any bathorhodopsin being observed during the formation of hypsorhodopsin. An experiment using an N₂ laser showed that squid bathorhodopsin converted to lumirhodopsin with a decay time of about 300 ns at room temperature.     

FLUORESCENCE OF THYMINE IN AQUEOUS SOLUTION AT 300° K

Abstract— –Fluorescence of thymine in neutral aqueous solution at room temperature has been detected using the multiscaling operation of a multichannel analyzer. The emission maximum (2.96 μm^-1) and 0-0 transition energy (3.37-3.45 μm^-1) are close to those determined at liquid nitrogen temperature in mixed solvents. The quantum efficiency of fluorescence excited at 3.77 μm^-1 is calculated to be 1.04 × 10^-4.
The corrected relative excitation spectrum shows significant differences from the absorption spectrum when both are determined under identical conditions of concentration and spectral bandwidth on the same instrument. The quantum yield of fluorescence decreases about 2-fold as the energy of excitation is increased beyond the 0-0' transition and follows the relation 1/φ°α E _excit..
This behavior is discussed in terms of (a) n π* and ππ* states, (b) emission from a minor tautomer and (c) kinetics of competing deactivation processes.     

SIMULATION ANALYSIS OF THE PHOTOCONVERSION PROCESS OF SQUID RHODOPSIN AT LIQUID HELIUM TEMPERATURE

The photoconversion process among squid rhodopsin, bathorhodopsin isorhodopsin and hypsorhodopsin was studied at liquid helium temperature. We evaluated the relative quantum yields of the photoconversion among four pigments by analysing the time-dependent change of absorption spectra. The result suggests that hypsorhodopsin is the common intermediate of rhodopsin and isorhodopsin, and there is no direct conversion between rhodopsin and isorhodopsin. Furthermore, rhodopsin converts to hypsorhodopsin or bathorhodopsin much more efficiently than does isorhodopsin, and bathorhodopsin does not convert directly to hypsorhodopsin. It was also found that rhodopsin and isorhodopsin convert to bathorhodopsin more efficiently than to hypsorhodopsin. In particular, the quantum yield of conversion from rhodopsin to bathorhodopsin was found to be about twice as large as that from rhodopsin to hypsorhodopsin. This result is somewhat in disagreement with the result obtained from the laser flash experiments at room and liquid nitrogen temperatures. The reason for the difference between the two experimental results is discussed.     

CIRCULAR DICHROISM OF BOVINE RHODOPSIN

Abstract— When rhodopsin is associated with membrane particles, phospholipid may be involved in maintaining a preferred conformation of the opsin and the asymmetric structure of the chromophore of rhodopsin.     

RETINAL-OPSIN LINKAGE OF CEPHALOPOD RHODOPSIN

Abstract— The pK_a of the Schiff base of N-retinylidene butylamine was determined in anionic (sodium dodecylsulfate), cationic (cetyltrimethylammonium bromide) and nonionic (polyoxyethylene (9) lauryl ether) detergent solutions. The pK_a of the Schiff base was raised from 6.4 to 9.9 by the effect of the neighboring anion. The rise of the pK_a was affected by the ion strength. Squid metarhodopsin behaved in a manner similar to the model Schiff base in the anionic detergent solution. The cationic group showed the opposite effect on the pK_a of the Schiff base. The retinal Schiff base in rhodopsin might be heavily influenced by adjacent anionic groups. The nature of the interaction is discussed.     

THE INVOLVEMENT OF WATER AT THE RETINAL BINDING SITE IN RHODOPSIN AND EARLY LIGHT-INDUCED INTRAMOLECULAR PROTON TRANSFER

Abstract Extensive dehydration of air-dried films of bovine rod outer segment membranes induces fully reversible changes in the absorption spectrum of rhodopsin, indicative of deprotonation of the retinylidene Schiff base in more than 50% of the rhodopsin molecules in the sample. This suggests that water is involved at the site of the Schiff base protonation in rhodopsin. In contrast, the spectrum of metarhodopsin I is resistant to similar dehydrating conditions, implying a significant difference in the mechanism for protonation in metarhodopsin I. The photochemistry of dehydrated membranes was also explored. Photoexcitation of deprotonated rhodopsin (λ_max 390 nm) induces a large bathochromic shift of the chromophore. The major photoproduct at room temperature was spectrally similar to metarhodopsin I (λ_max, 478 nm). These findings suggest that intramolecular proton transfer involving the Schiff base proton may occur in the earlier stages of the visual cycle, prior to or during the formation of metarhodopsin I.     

RECONSTITUTION OF SQUID RHODOPSIN IN RHABDOMAL MEMBRANES

Abstract— Squid opsin which is capable of combining with 11- cis or 9- cis retinal to reconstitute photo-pigment has been prepared by irradiation of rhabdomal membranes with orange light (> 530 nm) in the presence of 0.2 M hydroxylamine. When the irradiation is carried out either at concentrations of hydroxylamine higher than 0.2 M or with light of wavelength shorter than 530 nm, rhodopsin in the membranes is bleached quickly, but the ability of the resultant opsin to form rhodopsin is greatly reduced.
The optimum pH for rhodopsin regeneration in rhabdomal membranes was found to be between 6.5 and 8.5. The rate of regeneration of rhodopsin increases with raising temperature, and at about 20°C it is almost the same as that of isorhodopsin. Even after solubilization in digitonin solution, opsin still preserves the ability to reform rhodopsin.
All- trans retinal can be incorporated into retinochrome-bearing membranes, in which it is isomerized into 11- cis isomer by the photoisomerase activity of retinochrome. Rhabdomal membranes retaining active opsin can take up 11- cis retinal from retinochrome membranes so as to synthesize rhodopsin.     

THE POSSIBLE PRESENCE OF A THIRD INTERMEDIATE FOR IODOPSIN AT -195°C*

Abstract— From the theoretical analysis of the time variation of the change in absorbance of chicken iodopsin solution (at—195°C), the formation of a new intermediate during bleaching has been suggested.     

NANOSECOND LASER PHOTOLYSIS OF RHODOPSIN AND ISORHODOPSIN

Kinetic and spectral measurements have been carried out on the primary intermediate in the photolysis of rhodopsin and isorhodopsin, initiated by a 457 nm, 6 ns (FWHM) laser pulse. In rhodopsin the kinetic decay of bathorhodopsin was found to be 140 ± 15 ns at 20°C. The decay of bathorhodopsin to lumirhodopsin has an activation energy of 51 ± 4 kJ/mol (12.2 ± 1 kcal/mol). The decay kinetics of bathorhodopsin were found to be the same for rhodopsin in membrane and detergent solubilized suspensions. The kinetic decay of the batho product in the photolysis of isorhodopsin was found to be the same as rhodopsin.
The corrected transient spectrum 50 ns following excitation in rhodopsin has two peaks near 560 and 440 nm. A peak was also observed in isorhodopsin near 550 nm at 50 ns following excitation but no transient was observed in the blue. The 550 nm peak in isorhodopsin has an intensity similar to that in rhodopsin indicating that the quantum yields for the formation of batho products of rhodopsin and isorhodopsin are similar under the irradiation conditions used here. Transient spectra for rhodopsin and isorhodopsin 1 μs following excitation are also different. In isorhodopsin the corrected transient spectrum has a peak at 500 nm, similar to low temperature steady state irradiation spectra. The 1 μs transient spectrum in rhodopsin is more intense than in isorhodopsin and shows a peak at 475 nm.     

The system Ce–Zn–B at 800 °C

The isothermal section for the system Ce–Zn–B has been established at 800 °C using electron microprobe analysis and X-ray powder diffraction. No ternary compounds exist and mutual solid solubilities of binary phases are negligible. In the concentration range of 10.0–10.5 at% Ce two structural modifications have been confirmed: high temperature βCe₂Zn₁₇ above ∼750 °C with the Th₂Zn₁₇ type (R3?m, a=0.90916(4) nm, c=1.3286(1) nm) and low temperature αCeZn₇ (Ce_1−xZn_5+2x; x∼0.33) up to 750 °C for which we attributed the TbCu₇ type (P6/mmm, a=0.52424(2), c=0.44274(1) nm). The crystal structure of CeZn₇ was derived from the Rietveld refinement of X-ray powder intensities. Precise data on atom site distribution and positional parameters have been furthermore provided from X-ray single crystal refinements for two compounds, for which crystal structures hitherto have only been derived from X-ray diffraction photographs: Ce₃Zn₁₁ (Immm, a=0.45242(2) nm, b=0.88942(3) nm, c=1.34754(4) nm) and Ce₃Zn₂₂ (I4₁/amd; a=0.89363(2) nm, c=2.1804(5) nm).     

QUANTUM EFFICIENCIES OF THE REVERSIBLE PHOTOREACTION OF OCTOPUS RHODOPSIN

The classic method of photometric curves for photosensitivity determination has been extended to the case of photoreversible reactions and applied to the octopus rhodopsin --> acid metarhodopsin photoreaction. In such cases, measurements at one irradiation wavelength yield the sum of the photosensitivities of the forward and reverse processes. However, by using different irradiation wavelengths, together with appropriate molar extinction coefficients, the quantum efficiencies for both reactions may be resolved. For detergent-solubilized octopus rhodopsin at room temperature, pH 7, the quantum yields are found to be 0.69 (+/- 0.03) for rhodopsin --> metarhodopsin, in line with values observed in a range of vertebrate visual pigments, and 0.43 (+/- 0.02) for the reverse photoregeneration process. The similarities in overall photosensitivities of the forward and reverse reactions in the visible region are consistent with a significant physiological role for photoreversal in the cephalopod visual cycle.     

FEMTOSECOND STUDIES OF PRIMARY PHOTOPROCESSES IN OCTOPUS RHODOPSIN

Abstract— Femtosecond spectroscopy of octopus rhodopsin in H₂O and D₂O was performed over a very wide spectral region of 400–1000 nm. Transient gain and absorption from the excited state were observed for the first time around 650 and 700 nm, respectively, just after 300 fs pulse excitation. Bathorhodopsin was formed within 400 fs from the excited state; therefore, the cis-trans isomerization completes within 400 fs. The first intermediate "primerhodopsin" found in our previous paper is most likely "quasi-thermal" bathorhodopsin, in which the local thermalization of the chromophore is achieved. Then cooling down of the chromophore to the surrounding protein temperature takes place with 20 ± 10 ps along with blue-shifting of a spectrum of 10 ± 5 nm. In addition to these observations, a prominent gain in the region of > 850 nm was observed and decayed with 2–3 ps in H₂O. A similar time constant was estimated for a partial decay of an induced absorption around 600 nm. This process may be related with two forms of bathorhodopsin reported previously. In this scheme, two forms of bathorhodopsin are formed with time constants of about 400 fs and 2 ps. In the sample in D₂O, time constant of 3–4 ps was obtained for the slower process.     

THE 75°C THERMOLUMINESCENCE BAND OF GREEN TISSUES: CHEMILUMINESCENCE FROM MEMBRANE-CHLOROPHYLL INTERACTION

Abstract— Exposure of thylakoid membranes of green plants to high temperature promotes the appearance of free radicals resulting in a thermoluminesccnce (TL) band peaking around 75°C. The occurrence of this band with the same intensity in prcilluminated and in dark-adapted samples demonstrates that, contrary to several other TL bands, it is not a result of charge recombination. The high temperature TL band is oxygen dependent. Parallel to TL emission singlet oxygen is formed, as demonstrated by spin trapping EPR measurements and by the decrease of TL intensity in the presencc of sodium-azide, a singlet oxygen scavenger.
We suggest that the 75°C TL band is a result of a temperature-enhanced interaction between molecular oxygen and the photosynthetic membrane, possibly involving lipid peroxidation. The spectral maximum of the emission (around 720 nm) implics that light emission occurs upon energy transfer from an excited product to chlorophyll molecules destablized from pigment-protein complexes.