TY - JOUR
T1 - The nature of proton-coupled electron transfer in a blue light using flavin domain
AU - Zhou, Zhongneng
AU - Chen, Zijing
AU - Kang, X. W.
AU - Zhou, Yalin
AU - Wang, Bingyao
AU - Tang, Siwei
AU - Zou, Shuhua
AU - Zhang, Yifei
AU - Hu, Qiaoyu
AU - Bai, Fang
AU - Ding, Bei
AU - Zhong, Dongping
N1 - Publisher Copyright:
© 2022 National Academy of Sciences. All rights reserved.
PY - 2022/6/28
Y1 - 2022/6/28
N2 - Proton-coupled electron transfer (PCET) is key to the activation of the blue light using flavin (BLUF) domain photoreceptors. Here, to elucidate the photocycle of the central FMN-Gln-Tyr motif in the BLUF domain of OaPAC, we eliminated the intrinsic interfering W90 in the mutant design. We integrated the stretched exponential function into the target analysis to account for the dynamic heterogeneity arising from the active-site solvation relaxation and the flexible H-bonding network as shown in the molecular dynamics simulation results, facilitating a simplified expression of the kinetics model. We find that, in both the functional wild-type (WT) and the nonfunctional Q48E and Q48A, forward PCET happens in the range of 105 ps to 344 ps, with a kinetic isotope effect (KIE) measured to be ∼1.8 to 2.4, suggesting that the nature of the forward PCET is concerted. Remarkably, only WT proceeds with an ultrafast reverse PCET process (31 ps, KIE = 4.0), characterized by an inverted kinetics of the intermediate FMNH. Our results reveal that the reverse PCET is driven by proton transfer via an intervening imidic Gln.
AB - Proton-coupled electron transfer (PCET) is key to the activation of the blue light using flavin (BLUF) domain photoreceptors. Here, to elucidate the photocycle of the central FMN-Gln-Tyr motif in the BLUF domain of OaPAC, we eliminated the intrinsic interfering W90 in the mutant design. We integrated the stretched exponential function into the target analysis to account for the dynamic heterogeneity arising from the active-site solvation relaxation and the flexible H-bonding network as shown in the molecular dynamics simulation results, facilitating a simplified expression of the kinetics model. We find that, in both the functional wild-type (WT) and the nonfunctional Q48E and Q48A, forward PCET happens in the range of 105 ps to 344 ps, with a kinetic isotope effect (KIE) measured to be ∼1.8 to 2.4, suggesting that the nature of the forward PCET is concerted. Remarkably, only WT proceeds with an ultrafast reverse PCET process (31 ps, KIE = 4.0), characterized by an inverted kinetics of the intermediate FMNH. Our results reveal that the reverse PCET is driven by proton transfer via an intervening imidic Gln.
KW - kinetic isotope effect
KW - photoreceptors
KW - proton rocking
KW - proton-coupled electron transfer
KW - stretched dynamics
UR - https://www.scopus.com/pages/publications/85132687312
U2 - 10.1073/pnas.2203996119
DO - 10.1073/pnas.2203996119
M3 - 文章
C2 - 35737837
AN - SCOPUS:85132687312
SN - 0027-8424
VL - 119
JO - Proceedings of the National Academy of Sciences of the United States of America
JF - Proceedings of the National Academy of Sciences of the United States of America
IS - 26
M1 - e2203996119
ER -