Resonance Raman spectroscopy has been used to obtain structural and kinetic information on the primary photointermediates of bacteriorhodopsin with 3-ps time resolution. A synchronously pumped dye laser was amplified at 50 Hz to produce a probe pulse at 589 nm while a second, spectrally distinct, pump pulse at 550 nm was generated by amplification of a 10-nm portion of a continuum produced from the probe pulse. This apparatus was used to record Stokes Raman spectra of the photoproduct from 0 ps to 13 ns as well as anti-Stokes spectra from 0 to 10 ps. At 0 ps, the Stokes spectrum, assigned to J, has strong hydrogen out-of-plane (HOOP) intensity at 1000 and 956 cm-1, the fingerprint region consists of a broad band of lines from 1155 to 1200 cm-1, and the ethylenic line is found at 1518 cm-1. By 3 ps the relative HOOP intensity drops to its lowest value and the fingerprint collapses to a single strong mode at 1189 cm-1, while the ethylenic remains at 1518 cm-1. The lifetime of the initially strong anti-Stokes scattering is ∼2.5 ps, indicating that the J → K transition is due, in large part, to vibrational cooling of the chromophore. We conclude that the chromophore in J is highly twisted and thermally excited but that it cools and conformationally relaxes to a more planar 13-cis chromophore within 3 ps to form K. Between 3 and 40 ps there is a resurgence in Stokes HOOP intensity which remains large and nearly constant thereafter and the ethylenic frequency shifts from 1518 to 1521 cm-1 within 200 ps. These changes are assigned to the conversion of K to a more twisted and bluer-absorbing KL species between 20 and 100 ps which must be caused by an isomerization-induced protein conformational change. © 1991 American Chemical Society.
CITATION STYLE
Doig, S. J., Reid, P. J., & Mathies, R. A. (1991). Picosecond time-resolved resonance Raman spectroscopy of bacteriorhodopsin’s J, K, and KL intermediates. Journal of Physical Chemistry, 95(16), 6372–6379. https://doi.org/10.1021/j100169a054
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