scholarly journals Femtosecond stimulated Raman spectroscopy of the dark S1 excited state of carotenoid in photosynthetic light harvesting complex.

2012 ◽  
Vol 59 (1) ◽  
Author(s):  
Masayuki Yoshizawa ◽  
Ryosuke Nakamura ◽  
Orihiro Yoshimatsu ◽  
Kenta Abe ◽  
Shunsuke Sakai ◽  
...  

Vibrational dynamics of the excited state in the light-harvesting complex (LH1) have been investigated by femtosecond stimulated Raman spectroscopy (FSRS). The native and reconstituted LH1 complexes have same dynamics. The ν(1) (C=C stretching) vibrational mode of spirilloxanthin in LH1 shows ultrafast high-frequency shift in the S(1) excited state with a time constant of 0.3 ps. It is assigned to the vibrational relaxation of the S(1) state following the internal conversion from the photoexcited S(2) state.

2013 ◽  
Vol 41 ◽  
pp. 08007 ◽  
Author(s):  
O. Yoshimatsu ◽  
K. Abe ◽  
S. Sakai ◽  
T. Horibe ◽  
R. Fujii ◽  
...  

2015 ◽  
Vol 6 (9) ◽  
pp. 1592-1598 ◽  
Author(s):  
Mariangela Di Donato ◽  
Elena Ragnoni ◽  
Andrea Lapini ◽  
Tomasz M. Kardaś ◽  
Boźena Ratajska-Gadomska ◽  
...  

2003 ◽  
Vol 382 (1-2) ◽  
pp. 81-86 ◽  
Author(s):  
Philipp Kukura ◽  
David W. McCamant ◽  
Paul H. Davis ◽  
Richard A. Mathies

2015 ◽  
Vol 119 (10) ◽  
pp. 3920-3930 ◽  
Author(s):  
Kamarniso Vrandecic ◽  
Margus Rätsep ◽  
Laura Wilk ◽  
Leonid Rusevich ◽  
Maksym Golub ◽  
...  

Molecules ◽  
2019 ◽  
Vol 24 (7) ◽  
pp. 1326 ◽  
Author(s):  
Noura Zamzam ◽  
Jasper van Thor

We present ground and excited state frequency calculations of the recently discovered extremely red-shifted chlorophyll f. We discuss the experimentally available vibrational mode assignments of chlorophyll f and chlorophyll a which are characterised by particularly large downshifts of 131-keto mode in the excited state. The accuracy of excited state frequencies and their displacements are evaluated by the construction of Franck–Condon (FC) and Herzberg–Teller (HT) progressions at the CAM-B3LYP/6-31G(d) level. Results show that while CAM-B3LYP results are improved relative to B3LYP calculations, the displacements and downshifts of high-frequency modes are underestimated still, and that the progressions calculated for low temperature are dominated by low-frequency modes rather than fingerprint modes that are Resonant Raman active.


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