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Electron transport through two interacting channels in Azurin-based solid-state junctions.
Li, Ping'an; Bera, Sudipta; Kumar-Saxena, Shailendra; Pecht, Israel; Sheves, Mordechai; Cahen, David; Selzer, Yoram.
Afiliación
  • Li P; Department of Chemical Physics, School of Chemistry, Tel Aviv University, Tel Aviv 69978, Israel.
  • Bera S; Department of Molecular Chemistry and Materials Science, Weizmann Institute of Science, Rehovot 76100, Israel.
  • Kumar-Saxena S; Department of Physics and Nanotechnology, College of Engineering and Technology, SRM Institute of Science and Technology, Kattankulathur 603203, Tamil Nadu, India.
  • Pecht I; Department of Regenerative Biology and Immunology, Weizmann Institute of Science, Rehovot 76100, Israel.
  • Sheves M; Department of Molecular Chemistry and Materials Science, Weizmann Institute of Science, Rehovot 76100, Israel.
  • Cahen D; Department of Molecular Chemistry and Materials Science, Weizmann Institute of Science, Rehovot 76100, Israel.
  • Selzer Y; Department of Chemical Physics, School of Chemistry, Tel Aviv University, Tel Aviv 69978, Israel.
Proc Natl Acad Sci U S A ; 121(33): e2405156121, 2024 Aug 13.
Article en En | MEDLINE | ID: mdl-39110736
ABSTRACT
The fundamental question of "what is the transport path of electrons through proteins?" initially introduced while studying long-range electron transfer between localized redox centers in proteins in vivo is also highly relevant to the transport properties of solid-state, dry metal-protein-metal junctions. Here, we report conductance measurements of such junctions, Au-(Azurin monolayer ensemble)-Bismuth (Bi) ones, with well-defined nanopore geometry and ~103 proteins/pore. Our results can be understood as follows. (1) Transport is via two interacting conducting channels, characterized by different spatial and time scales. The slow and spatially localized channel is associated with the Cu center of Azurin and the fast delocalized one with the protein's polypeptide matrix. Transport via the slow channel is by a sequential (noncoherent) process and in the second one by direct, off-resonant tunneling. (2) The two channels are capacitively coupled. Thus, with a change in charge occupation of the weakly coupled (metal center) channel, the broad energy level manifold, responsible for off-resonance tunneling, shifts, relative to the electrodes' Fermi levels. In this process, the off-resonance (fast) channel dominates transport, and the slow (redox) channel, while contributing only negligibly directly, significantly affects transport by intramolecular gating.
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Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Proc Natl Acad Sci U S A Año: 2024 Tipo del documento: Article País de afiliación: Israel

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Proc Natl Acad Sci U S A Año: 2024 Tipo del documento: Article País de afiliación: Israel