1995
DOI: 10.1016/0301-4622(95)00021-o
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Evidence for parallel photocycles and implications for the proton pump in bacteriorhodopsin

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Cited by 12 publications
(6 citation statements)
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“…Two primary models have been put forward to explain the M kinetics. The first is one of parallel photocycles, starting with two ground state bR species, which go through their own photocycle kinetics but have the same spectral intermediates (Balashov et al, 1991;Eisfeld et al, 1995;Hendler et al, 2001). The second model assumes that there is a transition between two M states that is spectrally silent in the visible region Lanyi, 1990, 1991b;Perkins et al, 1992;Oka et al, 2002).…”
Section: Resultsmentioning
confidence: 99%
“…Two primary models have been put forward to explain the M kinetics. The first is one of parallel photocycles, starting with two ground state bR species, which go through their own photocycle kinetics but have the same spectral intermediates (Balashov et al, 1991;Eisfeld et al, 1995;Hendler et al, 2001). The second model assumes that there is a transition between two M states that is spectrally silent in the visible region Lanyi, 1990, 1991b;Perkins et al, 1992;Oka et al, 2002).…”
Section: Resultsmentioning
confidence: 99%
“…This assumption has also been shown to be invalid. 2,14 Nevertheless, Morgan et al concluded that there is a pH dependence of a very small component, centered near 1885 cm À1 , that is part of a larger pH-invariant negative continuum absorbance band extending over most of the spectral region above 1600 cm À1 . They attributed the small component centered near 1885 cm À1 to a protonated water cation serving as the PRG.…”
Section: Discussionmentioning
confidence: 99%
“…2, 3, 916 Hendler and coworkers have pointed out many experimental observations that can not be explained by a homogeneous sequential linear cycle. 2, 10, 13, 14 Most important, when using short (~10 ns) laser pulses for actinic excitation of bR, the yield of any particular photointermediate produced from a homogeneous ground state is expected to rise linearly at low intensities, and then to exhibit a saturation curve with an exponential behavior. That is, the photoproduct yield as a function of incident pulse energy E (in photons per cm 2 ) should be in proportion to [1- exp(- kE )], where k is a constant dependent on the bR extinction coefficient and quantum yield.…”
Section: Methodsmentioning
confidence: 99%
“…In native bR, two primary models have been presented to account for the biexponential rise. The first model is of that of parallel photocycles: that there are two different ground state bR species, each going through their own photocycle with the same spectral intermediates (39)(40)(41). The other model assumes that there is only one photocycle but that there is a transition between two M states, M 1 and M 2 , that is spectrally silent in the visible region (35,(42)(43)(44).…”
Section: Resultsmentioning
confidence: 99%