EXCITED-STATES OF THE BACTERIOCHLOROPHYLL-B DIMER OF RHODOPSEUDOMONAS-VIRIDIS - A QM MM STUDY OF THE PHOTOSYNTHETIC REACTION-CENTER THAT INCLUDES MM POLARIZATION/
Ma. Thompson et Gk. Schenter, EXCITED-STATES OF THE BACTERIOCHLOROPHYLL-B DIMER OF RHODOPSEUDOMONAS-VIRIDIS - A QM MM STUDY OF THE PHOTOSYNTHETIC REACTION-CENTER THAT INCLUDES MM POLARIZATION/, Journal of physical chemistry, 99(17), 1995, pp. 6374-6386
We present a hybrid quantum mechanical/molecular mechanical (QM/MM) mo
del for microscopic solvation effects that includes polarizability in
the MM region (QM/MMpol). QM/MMpol treatment of both ground and excite
d states is presented in the formalism. We present QM/MMpol analysis o
f the ground and electronic excited states of the bacteriochlorophyll
b dimer (P) of the photosynthetic reaction center (RC) of Rhodopseudom
onas viridis using the INDO/S method. We treat P and five adjacent ami
no acid side chains quantum mechanically, and the remainder of the pro
tein, cofactors, and waters of crystallization with Polarizable MM (32
5 QM atoms embedded in the field of 20 158 polarizable MM atoms). Whil
e dimer formation alone is enough to account for the majority of the m
onomer BCh1b to P red-shift of the lowest electronic excited state of
P (Q(y1)), we demonstrate that explicit treatment of the protein is re
quired to properly interpret the experimental Stark effect data that d
escribe the charge transfer asymmetry of Q(y1). The static-charge pote
ntial from the MM model of the RC alone causes Q(y1) to have significa
ntly better agreement with the Stark effect results than isolated P. H
owever, consideration of the protein polarization potential is further
required to obtain more complete agreement with Stark effect experime
nts. Thus, we calculate a Q(y1) transition energy at 10 826 cm(-1) wit
h a ground to excited state change in dipole moment of 4.8 D; an absor
ption Stark effect angle of 43 degrees; a net shift of 0.15 electrons
from the L subunit to the M subunit of P; and a linear dichroism angle
(between the transition moment of Q(y1) and the pseudo-C-2 axis of th
e RC) of 81 degrees. These results are in good agreement with experime
nt. Interestingly, we find that net CT increase is greater for Q(y1) t
han for the second excited state of P (Q(y2)), a result that we antici
pated in an early model dimer study.