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Photoinduced hole hopping through tryptophans in proteins.

Authors :
Záliš S
Heyda J
Šebesta F
Winkler JR
Gray HB
Vlček A
Source :
Proceedings of the National Academy of Sciences of the United States of America [Proc Natl Acad Sci U S A] 2021 Mar 16; Vol. 118 (11).
Publication Year :
2021

Abstract

Hole hopping through tryptophan/tyrosine chains enables rapid unidirectional charge transport over long distances. We have elucidated structural and dynamical factors controlling hopping speed and efficiency in two modified azurin constructs that include a rhenium(I) sensitizer, Re(His)(CO) <subscript>3</subscript> (dmp) <superscript>+</superscript> , and one or two tryptophans (W <subscript>1</subscript> , W <subscript>2</subscript> ). Experimental kinetics investigations showed that the two closely spaced (3 to 4 Å) intervening tryptophans dramatically accelerated long-range electron transfer (ET) from Cu <superscript>I</superscript> to the photoexcited sensitizer. In our theoretical work, we found that time-dependent density-functional theory (TDDFT) quantum mechanics/molecular mechanics/molecular dynamics (QM/MM/MD) trajectories of low-lying triplet excited states of Re <superscript>I</superscript> (His)(CO) <subscript>3</subscript> (dmp) <superscript>+</superscript> -W <subscript>1</subscript> (-W <subscript>2</subscript> ) exhibited crossings between sensitizer-localized (*Re) and charge-separated [Re <superscript>I</superscript> (His)(CO) <subscript>3</subscript> (dmp <superscript>•-</superscript> )/(W <subscript>1</subscript> <superscript>•+</superscript> or W <subscript>2</subscript> <superscript>•+</superscript> )] (CS1 or CS2) states. Our analysis revealed that the distances, angles, and mutual orientations of ET-active cofactors fluctuate in a relatively narrow range in which the cofactors are strongly coupled, enabling adiabatic ET. Water-dominated electrostatic field fluctuations bring *Re and CS1 states to a crossing where *Re(CO) <subscript>3</subscript> (dmp) <superscript>+</superscript> ←W <subscript>1</subscript> ET occurs, and CS1 becomes the lowest triplet state. ET is promoted by solvation dynamics around *Re(CO) <subscript>3</subscript> (dmp) <superscript>+</superscript> (W <subscript>1</subscript> ); and CS1 is stabilized by Re(dmp <superscript>•-</superscript> )/W <subscript>1</subscript> <superscript>•+</superscript> electron/hole interaction and enhanced W <subscript>1</subscript> <superscript>•+</superscript> solvation. The second hop, W <subscript>1</subscript> <superscript>•+</superscript> ←W <subscript>2</subscript> , is facilitated by water fluctuations near the W <subscript>1</subscript> /W <subscript>2</subscript> unit, taking place when the electrostatic potential at W <subscript>2</subscript> drops well below that at W <subscript>1</subscript> <superscript>•+</superscript> Insufficient solvation and reorganization around W <subscript>2</subscript> make W <subscript>1</subscript> <superscript>•+</superscript> ←W <subscript>2</subscript> ET endergonic, shifting the equilibrium toward W <subscript>1</subscript> <superscript>•+</superscript> and decreasing the charge-separation yield. We suggest that multiscale TDDFT/MM/MD is a suitable technique to model the simultaneous evolution of photogenerated excited-state manifolds.<br />Competing Interests: The authors declare no competing interest.

Details

Language :
English
ISSN :
1091-6490
Volume :
118
Issue :
11
Database :
MEDLINE
Journal :
Proceedings of the National Academy of Sciences of the United States of America
Publication Type :
Academic Journal
Accession number :
33836608
Full Text :
https://doi.org/10.1073/pnas.2024627118