2009
DOI: 10.1002/pssb.200982299
|View full text |Cite
|
Sign up to set email alerts
|

The anomaly of the $\nu$1‐resonance Raman band of bβ‐carotene in solution and in photosystem I and II

Abstract: We have studied the resonance Raman spectra of b-carotene in solution and in protein-complexes using laser excitation at various wavelengths in the visible region. Main focus was laid on the n 1 -band, which shows an anomalous behaviour upon variation of the excitation wavelength resulting in a frequency shift of the peak maximum. This shift is due to different excitation profiles of two closely spaced modes as shown previously for b-carotene in solution. In this work, we have extended the studies to the anten… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
10
0

Year Published

2010
2010
2020
2020

Publication Types

Select...
8

Relationship

1
7

Authors

Journals

citations
Cited by 19 publications
(10 citation statements)
references
References 19 publications
0
10
0
Order By: Relevance
“…Vibrational mode Assignment 747 γ(C-O-H) of COOH Pectin (Synytsya et al, 2003) 915 ν(C-O-C) in plane, symmetric Cellulose, lignin (Edwards et al, 1997) 1000 ν 3 (C-CH 3 stretching) and phenylalanine Carotenoids (Tschirner et al, 2009;Kurouski et al, 2015) 1048-1068…”
Section: Bandmentioning
confidence: 99%
“…Vibrational mode Assignment 747 γ(C-O-H) of COOH Pectin (Synytsya et al, 2003) 915 ν(C-O-C) in plane, symmetric Cellulose, lignin (Edwards et al, 1997) 1000 ν 3 (C-CH 3 stretching) and phenylalanine Carotenoids (Tschirner et al, 2009;Kurouski et al, 2015) 1048-1068…”
Section: Bandmentioning
confidence: 99%
“…Vibrational mode Assignment 747 γ(C─O─H) of COOH Pectin [25] 915 ν(C─O─C) in plane, symmetric Cellulose and lignin [26] 1,000 ν 3 (C─CH 3 stretching) and phenylalanine Carotenoids and protein [27,28] 1,155 asym ν(C─C) ring breathing Carbohydrates and cellulose [26] 1,184 ν(C─O─H) next to aromatic ring+σ (CH) Xylan [29,30] 1,218-1,226 δ(C─C─H) Aliphatic [31] and xylan [29] 1,247 C─O stretching (aromatic) Lignin [32] 1,288 δ(C─C─H) Aliphatic [31] 1,326 δCH 2 bending vibration Cellulose and lignin [26] 1,382 δCH 2 bending vibration Aliphatic [31] 1,440 δ (CH 2 ) + δ (CH 3 ) Aliphatic [31] 1,455 δCH 2 bending vibration Aliphatic [31] 1,488 δ (CH 2 ) + δ (CH 3 ) Aliphatic [31] 1,527-1,551 ─C═C─ (in plane) Carotenoids [33,34] 1,601 ν(C─C) aromatic ring+σ (CH) Lignin [35,36] 1,630 C═C─C (ring) Lignin [35][36][37] intensities of all other bands in the spectra collected from leaves of CA and HLB + BL exhibited only very small variations compared with the spectra collected from leaves of HL trees.…”
Section: Bandmentioning
confidence: 99%
“…30 Besides, Tschirner et al 28 found a wavelength-dependent variation of the peak maximum of the C=C stretch vibration for β-carotene in dichloromethane and photosystems I and II 28 that they attributed to different relative resonances of the two underlying modes, and pointed out that their quantum chemical calculations could not reproduce the effect. 28,31 According to their experimental data, the peak maximum shifts from 1525 cm −1 at 1064 nm to 1521 cm −1 at around 514 nm and up again to Raman spectra are mapped for excitation wavelengths between 446 nm and 534 nm, and the resonance profile of the strongest carotenoid Raman peak at ca. 1528 cm −1 (C=C stretch) is displayed here.…”
Section: Raman Peak Positionsmentioning
confidence: 99%