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Fluorescence hole-burning and site-selective studies of LHCII

机译:LHCII的荧光孔燃烧和定点研究

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摘要

We report the observation of two types of changes in fluorescence spectra of LHCII at 4.2 K following intense illumination of the sample with a spectrally narrow laser beam at wavelengths between 678 and 686 nm. Nonspecific changes (burning-wavelength independent) are characterized by two relatively broad bands: a positive one at ∼ 678.7 nm and a negative one at ∼ 680.8 nm. These changes reveal a ∼1.3-nm blue shift of the distribution of final emitters in LHCII, from 680.3 nm to ∼ 679.0 nm independent of the excitation wavelength. Specific fluorescence changes (burning-wavelength dependent) are characterized by a sharp hole exactly at the burning wavelength, and positive changes directly to the shorter-and longer-wavelength side of the narrow hole. The negative changes are interpreted as zero-phonon holes, while the positive features are assigned to non-photochemical products. In the low-burning intensity experiment, in addition to the zero-phonon holes, we observed also the holes to the longer wavelength of the zero-phonon hole, which were assigned to a sum of phonon and pseudo-phonon side bands. The shapes of these extra holes are identical to the shapes of the holes revealed in the fluorescence line narrowing experiment. On the basis of the low-burning intensity experiment we estimated the upper limit of the electron-phonon coupling strength for LHCII, characterized by a Huang-Rhys factor of 1.5.
机译:我们报告观察到的LHCII在4.2 K的荧光光谱的两种类型的变化,之后用光谱狭窄的激光束在678和686 nm之间的波长强烈照射了样品。非特异性变化(与燃烧波长无关)的特征在于两个相对较宽的波段:在〜678.7 nm处为正的一个波段,在〜680.8 nm处为负的一个波段。这些变化揭示了LHCII中最终发射极分布的〜1.3 nm蓝移,从680.3 nm到〜679.0 nm,与激发波长无关。特定的荧光变化(与燃烧波长有关)的特征是恰好在燃烧波长处有一个尖孔,而在窄孔的短波长和长波长侧直接有正变化。负的变化被解释为零声子孔,而正的特征被分配给非光化学产品。在低燃烧强度实验中,除了零声子孔,我们还观察到了零声子孔较长波长的孔,这些孔被分配给声子和伪声子边带之和。这些额外的孔的形状与荧光线变窄实验中揭示的孔的形状相同。在低燃烧强度实验的基础上,我们估计了LHCII的电子-声子耦合强度的上限,其特征为Huang-Rhys因子为1.5。

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