The vibrational spectrum (800−1700 cm -1 region) of the J-625 intermediate, formed within 200−500 fs (3.5 ps decay time to K-590) in the room-temperature bacteriorhodopsin (BR) photocycle, is measured via picosecond time-resolved coherent anti-Stokes Raman spectroscopy (PTR/CARS). An examination of the excitation conditions and BR photocycle kinetics, as well as the vibrational CARS data, convincingly demonstrates that these PTR/CARS spectra can be quantitatively analyzed in terms of primarily BR-570 and J-625 by using third-order nonlinear susceptibility (χ (3) ) relationships. The resultant background-free (Lorentzian line shapes) CARS spectrum contains 24 distinct vibrational features which provide the most complete structural characterization of J-625 yet reported. Comparisons of the J-625 vibrational spectrum with those of ground-state BR-570 and the K-590 intermediate show that J-625 maintains some structural similarities with BR-570 while it has a significantly different structure than that of K-590. Specifically, J-625 has (i) an all- trans retinal configuration, (ii) increased electron density in the C C stretching modes as manifested by increased C C stretching frequencies relative to those in both BR-570 and K-590, (iii) significant delocalized hydrogen out-of-plane motion not observed in any other BR species, (iv) decreased C−CH 3 in-plane wagging motion, and (v) a Schiff-base bonding environment similar to that of BR-570 and distinctively different from that in K-590. Comparisons between the PTR/CARS spectra of J-625 and T5.12, an intermediate found in the photoreaction of the artificial BR pigment, BR5.12, containing a five-membered ring spanning the C 12 −C 13 C 14 bonds (thereby blocking C 13 C 14 isomerization), support the conclusion that the J-625 structure reflects the reaction coordinates in the BR photocycle that precede C 13 C 14 isomerization. Since these PTR/CARS data show J-625 to have an all- trans retinal, C 13 C 14 isomerization cannot be the primary reaction coordinate described in numerous models for the BR photocycle. The all- trans to 13- cis isomerization must occur as J-625 transforms into K-590, and other changes in the retinal structural and/or retinal−protein interactions must comprise the primary reaction coordinates that precede C 13 C 14 isomerization. These results require that significant changes in the mechanistic model describing the room-temperature BR photocycle be considered.
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Atkinson et al. (1999) studied this question.
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