A. Freiberg et al., SUBPICOSECOND PUMP-SUPERCONTINUUM PROBE SPECTROSCOPY OF LH2 PHOTOSYNTHETIC ANTENNA PROTEINS AT LOW-TEMPERATURE, The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory, 102(23), 1998, pp. 4372-4380
Exciton relaxation and energy-transfer processes in the B850 circular
aggregate of bacteriochlorophyll a molecules from the purple nonsulfur
photosynthetic bacterium Rhodobacter sphaeroides were studied at temp
eratures below 18 K. Excitons were selectively excited by a 7 nm spect
ral bandwidth pump pulse resonant with the inhomogeneously broadened l
ong-wavelength side of the B850 ground-state absorption spectrum (betw
een 860 and 879 nm). The transient spectra were measured over the 786-
924 nm spectral range using a white light continuum probe pulse. Chara
cteristic changes of transient spectra were observed over 4 decades of
time, from about 10(-13) to about 10(-9) s. The spectral evolution wa
s pump wavelength-dependent, changes being least notable at far-red ex
citation. A simple model was put forward to interpret the data, assumi
ng that the sample consists of an ensemble of spectrally disorded exci
tons, each representing a separate B850 ring. It was found that the ex
citon coupling and diagonal disorder play almost equally important rol
es in the formation of the spectral and dynamical properties of Light
excitations in B850 antenna. The main effects of disorder considered w
ere the spectral shifts, splitting of the degenerate exciton levels, a
nd redistribution of the dipole strength of the transitions. Assuming
that the contribution of least disturbed excitons is largest near the
peak of the ground-state absorption spectrum and greatest near the edg
e, most of the known spectroscopic properties of LH2, complexes can be
well understood, at least qualitatively. Specifically, the rough 100
fs response time was assigned to interexciton level relaxation; the th
ree time constants, ca. 800 fs, ca. 15 ps, and ca. 150 ps, were attrib
uted to exciton energy transfer, most likely, between the B850 rings.
The ca. 1 ns decay time is due to the finite exciton lifetime. The cir
cular LH1 antennas likely possess similar properties.