175 research outputs found

    Independent photocycles of the spectrally distinct forms of bacteriorhodopsin

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    Adaptation of pineal expressed teleost exo-rod opsin to non-image forming photoreception through enhanced Meta II decay

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    Photoreception by vertebrates enables both image-forming vision and non-image-forming responses such as circadian photoentrainment. Over the recent years, distinct non-rod non-cone photopigments have been found to support circadian photoreception in diverse species. By allowing specialization to this sensory task a selective advantage is implied, but the nature of that specialization remains elusive. We have used the presence of distinct rod opsin genes specialized to either image-forming (retinal rod opsin) or non-image-forming (pineal exo-rod opsin) photoreception in ray-finned fish (Actinopterygii) to gain a unique insight into this problem. A comparison of biochemical features for these paralogous opsins in two model teleosts, Fugu pufferfish (Takifugu rubripes) and zebrafish (Danio rerio), reveals striking differences. While spectral sensitivity is largely unaltered by specialization to the pineal environment, in other aspects exo-rod opsins exhibit a behavior that is quite distinct from the cardinal features of the rod opsin family. While they display a similar thermal stability, they show a greater than tenfold reduction in the lifetime of the signaling active Meta II photoproduct. We show that these features reflect structural changes in retinal association domains of helices 3 and 5 but, interestingly, not at either of the two residues known to define these characteristics in cone opsins. Our findings suggest that the requirements of non-image-forming photoreception have lead exo-rod opsin to adopt a characteristic that seemingly favors efficient bleach recovery but not at the expense of absolute sensitivity

    Energy Transfer in Rhodopsin, N-Retinyl-Opsin, and Rod Outer Segments

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    The quantum efficiency for the photochemical conversion of the purple membrane protein.

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    The quantum efficiency for the formation of M(412), an intermediate product in the photoconversion of the purple membrane protein of Halobacterium halobium, was determined to be 0.30 +/- 0.03 at -40 degrees C. This photochemical reaction was photoreversible to the original pigment and the ratio of the quantum efficiencies gamma PM(568 leads to M(412)/gamma M(412) leads to PM(568) was 0.39 +/- 0.02. No change was seen in either value when exciton interaction between chromophores was eliminated. The sum of gamma PM(568) leads to M(412) plus gamma M(412) leads to PM(568) was 1.07 +/- 0.10, approximately 1, suggesting that the pigment and its primary photoproduct share a common excited state

    Effect of high pressure on the absorption spectrum and isomeric composition of bacteriorhodopsin.

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    The effects of high pressure upon the absorption spectra and isomeric composition of the dark (bRD) and light adapted (bRL) forms of bacteriorhodopsin were examined. Pressure favors the 13-cis form of bacteriorhodopsin (bR13-cis). The equilibrium isomeric composition and absorption spectra of bacteriorhodopsin samples at a given pressure were the same starting from either light or dark adapted bacteriorhodopsin. From the effect of pressure on the equilibrium constant between bRall-trans in equilibrium bR13-cis in the dark, the molar volume change between bRall-trans and bR13-cis was found to be -7.8 +/- 3.2 ml/mol. This volume change suggests a difference in conformation between dark- and light-adapted bacteriorhodopsin, but the magnitude of the change is small, involving only a small number of the protein residues

    Photocurrent measurements of the purple membrane oriented in a polyacrylamide gel.

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    When illuminated, oriented purple membranes isolated from Halobacterium halobium give a photoelectric effect. The frequency response of a photocurrent measuring system for purple membranes oriented and immobilized in a polyacrylamide gel is analyzed from DC to 100 MHz. The waveform of the photocurrent can depend on both the sample conditions (including bathing solution) and the measuring system (electrode and ammeter) at both the low and high frequency ends. In the DC-1 kHz range (millisecond signals), the apparent lifetime of the photocurrent component is distorted if the electrode is not platinized and if the conductivity of the bathing solution is not low. In the 1 kHz to 1 MHz range (microsecond signals), the frequency response is flat under most conditions. In the MHz range (nanosecond signals), the apparent lifetime of the photocurrent component will be distorted if the conductivity of the bathing solution is not high and if the input impedance of the ammeter is not low and constant throughout the frequency range. With our optimized apparatus, we could measure the photocurrent components from oriented purple membrane with lifetimes from 70 ms to 32 ns without distortion by the measuring system

    Binding of a single divalent cation directly correlates with the blue-to-purple transition in bacteriorhodopsin.

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    Energy transfer in the purple membrane of Halobacterium halobium.

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    The absorption spectrum of the primary photoproduct (the bathoproduct, or K) of the purple membrane protein (PM) at-196 degrees C has a maximum at 628 nm and an extinction coefficient of 87,000. Knowing the absorption spectrum allowed us to calculate the quantum efficiencies for PM to K and K to PM conversion at -196 degrees C. Direct measurements of these quantum yeilds at -196 degrees C gave 0.33 +/- 0.05 and 0.67 +/- 0.04, respectively. Determination of relative quantum efficiencies for PM to K and K to PM conversion by analysis of the absorption spectra of several photostationary-state mixtures of PM and K at -196 degrees C, however, gave wavelength-dependent quantum efficiencies that appear to be greater than 1. These anomolous results can be readily explained in terms of energy transfer from PM to K within the trimer clusters of pigment molecules which exist in the purple membrane. A model for such a transfer predicts an efficiency of energy transfer from PM to K of about 43%
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