Abstract:Absorption and CD spectra of a photosynthetic bacterial antenna complex are calculated on the basis of the crystal structure of the LH2 (B800-850) complex from Rhodopseudomonas acidophila. This complex contains a ring of 18 tightly coupled bacteriochlorophylls (B850) and a ring of 9 more weakly coupled bacteriochlorophylls (B800). Molecular orbitals for bacteriochlorophylls with the three different geometries seen in the crystal structure are obtained by semiempirical quantum mechanical calculations (QCFF/PI).… Show more
“…3 In our simulations of the B850 absorption band we have taken into account the interactions between the Q y transitions of BChls, neglecting their mixing with Q x , B y , B x transitions as well as with charge transfer states. 8 We supposed that the interaction energies between the BChl molecules are M 12 ) 400 cm - 16 For the LH2 complex of Rb. sphaeroides an analysis of the CD spectrum yielded M 12 ) 300 cm -1 and M 23 ) 233 cm -1 .…”
Section: Model Of the Bacterial Light-harvesting Antennamentioning
We report the results of relative difference absorption measurements for the LH2 antenna of Rhodobacter sphaeroides and the B820 subunit of Rhodospirillum rubrum at room temperature. It is shown that significant differences between shapes and amplitudes of photoinduced, absorption changes reflect a different degree of exciton delocalization in the intact antenna compared with the dimeric subunit. Using the exciton model in the presence of static disorder, we have obtained a consistent and quantitative fit of the amplitudes and shapes of the pump-probe spectra of the LH2 antenna and the B820 subunit. We estimate that the nearest-neighbors interaction energy in the antenna is about 400 cm -1 and the diagonal disorder is about 450 cm -1 . For these values the coherence length (FWHM) of the steady-state exciton wavepacket corresponds to 5 BChl molecules at room temperature. The amplitude of the difference absorption reflects a cooperative behavior within at least 12 BChls of the B850 antenna. The calculations suggest that the dimeric subunit is characterized by a decrease of the interaction energy to 300 cm -1 together with an increase of the disorder value to about 600 cm -1 .
“…3 In our simulations of the B850 absorption band we have taken into account the interactions between the Q y transitions of BChls, neglecting their mixing with Q x , B y , B x transitions as well as with charge transfer states. 8 We supposed that the interaction energies between the BChl molecules are M 12 ) 400 cm - 16 For the LH2 complex of Rb. sphaeroides an analysis of the CD spectrum yielded M 12 ) 300 cm -1 and M 23 ) 233 cm -1 .…”
Section: Model Of the Bacterial Light-harvesting Antennamentioning
We report the results of relative difference absorption measurements for the LH2 antenna of Rhodobacter sphaeroides and the B820 subunit of Rhodospirillum rubrum at room temperature. It is shown that significant differences between shapes and amplitudes of photoinduced, absorption changes reflect a different degree of exciton delocalization in the intact antenna compared with the dimeric subunit. Using the exciton model in the presence of static disorder, we have obtained a consistent and quantitative fit of the amplitudes and shapes of the pump-probe spectra of the LH2 antenna and the B820 subunit. We estimate that the nearest-neighbors interaction energy in the antenna is about 400 cm -1 and the diagonal disorder is about 450 cm -1 . For these values the coherence length (FWHM) of the steady-state exciton wavepacket corresponds to 5 BChl molecules at room temperature. The amplitude of the difference absorption reflects a cooperative behavior within at least 12 BChls of the B850 antenna. The calculations suggest that the dimeric subunit is characterized by a decrease of the interaction energy to 300 cm -1 together with an increase of the disorder value to about 600 cm -1 .
“…14, [18][19][20][21][22][23][24][25][26][27][28][29][30] Various spectroscopic measurements, such as absorption, 4,5 fluorescence, 11,12 pump-probe, 12 and photon echo, 6,7 have been employed for probing exciton motions in molecular aggregates.…”
Fluorescence line shapes and cooperative spontaneous emission in disordered one-dimensional molecular aggregates are calculated using closed expressions derived by applying the method of optimal fluctuation. A simple scaling relation L s ∼ ω s -1/2 is established between the low temperature disorder-induced Stokes shift ω s and the superradiance enhancement factor L s . Scaling of the Stokes shift with aggregate size, and the time-dependent Stokes shift are discussed as well. Excellent agreement is obtained with numerical simulations.
“…In this equation, the Lorentz correction factor is used (20). Using this formula, we found that integration over the Voigt-type absorption band previously described, provides a transition dipole moment of (5.2 Ϯ 0.5) D for BChl-ser in PBS, pH ϭ 7.4.…”
Section: Solvent Effects On the Absorptionmentioning
We investigated the dependence on solvents of optical absorption and emission of the bacteriochlorophyll a-serine (BChl-ser), a water soluble bacteriochlorophyll (BChl) derivative. Comparison between the experimental data and those collected for BChl in nonaqueous solvents shows that only a minor interaction takes place between serine and the macrocycle's -electron system. Nevertheless, the coupling with serine results in a small enhancement of the nonradiative relaxation rate from the first excited singlet state S 1 . In buffered aqueous solution (pH
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