Department of Physics , Concordia University , 7141 Sherbrooke Street West , Montreal H4B 1R6 , Quebec , Canada.
Department of Chemistry , Kansas State University , Manhattan , Kansas 66506 , United States.
J Phys Chem B. 2019 Jul 18;123(28):6007-6013. doi: 10.1021/acs.jpcb.9b03806. Epub 2019 Jul 2.
For the first time, we combined Monte Carlo and nonphotochemical hole burning (NPHB) master equation approaches to allow for ultrahigh-resolution (<0.005 cm, smaller than the typical homogeneous line widths at 5 K) simulations of the NPHB spectra of dimers and trimers of interacting pigments. These simulations reveal significant differences between the zero-phonon hole (ZPH) action spectrum and the site-distribution function (SDF) of the lowest-energy state. The NPHB of the lowest-energy pigment, following the excitation energy transfer (EET) from the higher-energy pigments which are excited directly, results in the shifts of all excited states. These shifts affect the ZPH action spectra and EET times derived from the widths of the spectral holes burned in the donor-dominated regions. The effect is present for a broad variety of realistic antihole functions, and it is maximal at relatively low values of interpigment coupling ( ≤ 5 cm) where the use of the Förster approximation is justified. These findings need to be considered in interpreting various optical spectra of photosynthetic pigment-protein complexes for which SDFs (describing the inhomogeneous broadening) are often obtained directly from the ZPH action spectra. Water-soluble chlorophyll-binding protein (WSCP) was considered as an example.
我们首次结合蒙特卡罗和非光化学孔烧蚀(NPHB)主方程方法,实现了相互作用的二聚体和三聚体的 NPHB 光谱的超高分辨率(<0.005cm,小于 5K 时的典型均匀线宽)模拟。这些模拟揭示了零声子孔(ZPH)作用光谱与最低能量态的局域分布函数(SDF)之间的显著差异。最低能量色素的 NPHB,在直接激发更高能量色素的激发能量转移(EET)之后,导致所有激发态的位移。这些位移影响了从供体主导区域中烧蚀的光谱孔的宽度得出的 ZPH 作用光谱和 EET 时间。对于各种实际的反孔函数,这种效应都存在,并且在相对较低的色素间耦合(≤5cm)时最大,在这种情况下,福斯特近似是合理的。对于其中经常直接从 ZPH 作用光谱获得局域分布函数(描述非均匀展宽)的各种光合色素 - 蛋白复合物的各种光学光谱,需要考虑这些发现。水溶性叶绿素结合蛋白(WSCP)被认为是一个例子。