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Coherent intradimer dynamics in reaction centers of photosynthetic green bacterium Chloroflexus aurantiacus
Early-time dynamics of absorbance changes (light minus dark) in the long-wavelength Q(y) absorption band of bacteriochlorophyll dimer P of isolated reaction centers (RCs) from thermophilic green bacterium Chloroflexus (Cfx.) aurantiacus was studied by difference pump-probe spectroscopy with 18-fs re...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Nature Publishing Group UK
2020
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6959224/ https://www.ncbi.nlm.nih.gov/pubmed/31937882 http://dx.doi.org/10.1038/s41598-019-57115-1 |
Sumario: | Early-time dynamics of absorbance changes (light minus dark) in the long-wavelength Q(y) absorption band of bacteriochlorophyll dimer P of isolated reaction centers (RCs) from thermophilic green bacterium Chloroflexus (Cfx.) aurantiacus was studied by difference pump-probe spectroscopy with 18-fs resolution at cryogenic temperature. It was found that the stimulated emission spectrum gradually moves to the red on the ~100-fs time scale and subsequently oscillates with a major frequency of ~140 cm(−1). By applying the non-secular Redfield theory and linear susceptibility theory, the coherent dynamics of the stimulated emission from the excited state of the primary electron donor, bacteriochlorophyll dimer P*, was modeled. The model showed the possibility of an extremely fast transition from the locally excited state P(1)* to the spectrally different excited state P(2)*. This transition is clearly seen in the kinetics of the stimulated emission at 880 and 945 nm, where mostly P(1)* and P(2)* states emit, respectively. These findings are similar to those obtained previously in RCs of the purple bacterium Rhodobacter (Rba.) sphaeroides. The assumption about the existence of the second excited state P(2)* helps to explain the complicated temporal behavior of the ΔA spectrum measured by pump-probe spectroscopy. It is interesting that, in spite of the strong coupling between the P(1)* and P(2)* states assumed in our model, the form of the coherent oscillations is mainly defined by pure vibrational coherence in the excited states. A possible nature of the P(2)* state is discussed. |
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