Early picosecond events in the photocycle of bacteriorhodopsin

Applications of ultrafast laser spectroscopy for the study of biological systems

The discovery of mode-locked laser operation now nearly two decades ago has started a development which enables researchers to probe the dynamics of ultrafast physical and chemical processes at the molecular level on shorter and shorter time scales. Naturally the first applications were in the fields of photophysics and photochemistry where it was then possible for the first time to probe electronic and vibrational relaxation processes on a sub-nanosecond timescale. The development went from lasers producing pulses of many picoseconds to the shortest pulses which are at present just a few femtoseconds long. Soon after their discovery ultrashort pulses were applied also to biological systems which has revealed a wealth of information contributing to our understanding of a broadrange of biological processes on the molecular level.It is the aim of this review to discuss the recent advances and point out some future trends in the study of ultrafast processes in biological systems using laser techniques. The emphasis will be mainly on new results obtained during the last 5 or 6 years. The term ultrafast means that I shall restrict myself to sub-nanosecond processes with a few exceptions.

Picosecond time-resolved fluorescence spectroscopy of K-590 in the bacteriorhodopsin photocycle

The fluorescence spectrum of a distinct isometric and conformational intermediate formed on the 10(-11) s time scale during the bacteriorhodopsin (BR) photocycle is observed at room temperature using a two laser, pump-probe technique with picosecond time resolution. The BR photocycle is initiated by pulsed (8 ps) excitation at 565 nm, whereas the fluorescence is generated by 4-ps laser pulses at 590 nm. The unstructured fluorescence extends from 650 to 880 nm and appears in the same general spectral region as the fluorescence spectrum assigned to BR-570. The transient fluorescence spectrum can be distinguished from that assigned to BR-570 by a larger emission quantum yield (approximately twice that of BR-570) and by a maximum intensity near 731 nm (shifted 17 nm to higher energy from the maximum of the BR-570 fluorescence spectrum). The fluorescence spectrum of BR-570 only is measured with low energy, picosecond pulsed excitation at 590 nm and is in good agreement with recent data in the literature. The assignment of the transient fluorescence spectrum to the K-590 intermediate is based on its appearance at time delays longer than 40 ps. The K-590 fluorescence spectrum remains unchanged over the entire 40-100-ps interval. The relevance of these fluorescence data with respect to the molecular mechanism used to model the primary processes in the BR photocycle also is discussed.

Two pumps, one principle: light-driven ion transport in halobacteria

Comparison of the primary structure of the chloride pump halorhodopsin with that of the proton pump bacteriorhodopsin provides insight into light-driven ion transport by retinal proteins. Several conserved amino acid residues in the membrane-spanning region of both proteins and their interaction with different isomerization states of retinal are suggested to be the key element for ion transport in both proteins.

Nonproton ion release by purple membranes exhibits cooperativity as shown by determination of the optical cross-section

The amplitudes of the conductivity transients in photoexcited purple membranes were studied as a function of the energy of the actinic flash to determine the optical cross section of the process giving rise to the conductivity transient. Heating of the solution by the absorbed light causes an additional conductivity change and serves as an internal actinometer; the experiment directly yields the ratio of the cross section of ion release/uptake to that for light absorption. In effect, this counts the number of bacteriorhodopsin (bR) molecules involved in the conductivity transient per photon absorbed. At pH 7 in 0.4-0.5 M NaCl, where the conductivity signals are dominated by nonproton ions, the ratio is between 3 and 4, i.e., excitation of any one of several chromophores generates the same ion release signal. The simplest interpretation is that at pH 7 cooperative conformational changes cause a transient change in the surface charge distribution near all the affected bR molecules, resulting in the transient release of numerous counterions. As a comparison, at pH 4 where the signals are due to protons alone, the cross section data indicate that only a single bR molecule is involved in the proton movements. In this case, the results also show that the sum of the primary forward and reverse quantum yields (for the reactions: bR----K) is 0.88 +/- 0.09.

Excited-state structure and isomerization dynamics of the retinal chromophore in rhodopsin from resonance Raman intensities

Resonance Raman excitation profiles have been measured for the bovine visual pigment rhodopsin using excitation wavelengths ranging from 457.9 to 647.1 nm. A complete Franck-Condon analysis of the absorption spectrum and resonance Raman excitation profiles has been performed using an excited-state, time-dependent wavepacket propagation technique. This has enabled us to determine the change in geometry upon electronic excitation of rhodopsin's 11-cis-retinal protonated Schiff base chromophore along 25 normal coordinates. Intense low-frequency Raman lines are observed at 98, 135, 249, 336, and 461 cm-1 whose intensities provide quantitative, mode-specific information about the excited-state torsional deformations that lead to isomerization. The dominant contribution to the width of the absorption band in rhodopsin results from Franck-Condon progressions in the 1,549 cm-1 ethylenic normal mode. The lack of vibronic structure in the absorption spectrum is shown to be caused by extensive progressions in low-frequency torsional modes and a large homogeneous linewidth (170 cm-1 half-width) together with thermal population of low-frequency modes and inhomogeneous site distribution effects. The resonance Raman cross-sections of rhodopsin are unusually weak because the excited-state wavepacket moves rapidly (approximately 35 fs) and permanently away from the Franck-Condon geometry along skeletal stretching and torsional coordinates.

Direct observation of the femtosecond excited-state cis-trans isomerization in bacteriorhodopsin

Femtosecond optical measurement techniques have been used to study the primary photoprocesses in the light-driven transmembrane proton pump bacteriorhodopsin. Light-adapted bacteriorhodopsin was excited with a 60-femtosecond pump pulse at 618 nanometers, and the transient absorption spectra from 560 to 710 nanometers were recorded from -50 to 1000 femtoseconds by means of 6-femtosecond probe pulses. By 60 femtoseconds, a broad transient hole appeared in the absorption spectrum whose amplitude remained constant for about 200 femtoseconds. Stimulated emission in the 660- to 710-nanometer region and excited-state absorption in the 560- to 580-nanometer region appeared promptly and then shifted and decayed from 0 to approximately 150 femtoseconds. These spectral features provide a direct observation of the 13-trans to 13-cis torsional isomerization of the retinal chromophore on the excited-state potential surface. Absorption due to the primary ground-state photoproduct J appears with a time constant of approximately 500 femtoseconds.

Branching photocycle of sensory rhodopsin in halobacterium halobium

Temperature effect of the photocyle of sensory rhodopsin (sR) was studied by nanosecond spectroscopy. Though the formation yield of sR(M) (sR(370)) was sharply decreased with temperature, those of sR(K) (sR(680)) and sR(L) were insensitive to temperature changes. These results show the existence of the branching process back to sR from sR(L). The absorption maxima for sR(K) and sR(L) were 595 +/- 5 and 555 +/- 15 nm, respectively.

Primary charge motions and light-energy transduction in bacteriorhodopsin

The bacteriorhodopsin protein (bR) in the cell membrane of Halobacterium halobium is a light driven proton pump. Many details are known about its structure and the molecular mechanism of proton translocation. The events may be characterized by: (1) the changes in light absorption after photon excitation (the photocycle); (2) the charge motion cycle inside the protein: the steps taken by the proton during translocation; (3) the retinal cycle. changes in isomerization and protonation; and (4) the opsin cycle: alterations of protonation of different amino acids in the apoprotein. From a review of existing data a more or less concise picture of the parallelism of the above four cycles emerges, which may be valuable as a model for understanding other types of molecular pumps.