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Unifying photocycle model for light adaptation and temporal evolution of cation conductance in channelrhodopsin-2

Although channelrhodopsin (ChR) is a widely applied light-activated ion channel, important properties such as light adaptation, photocurrent inactivation, and alteration of the ion selectivity during continuous illumination are not well understood from a molecular perspective. Herein, we address the...

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Detalles Bibliográficos
Autores principales: Kuhne, Jens, Vierock, Johannes, Tennigkeit, Stefan Alexander, Dreier, Max-Aylmer, Wietek, Jonas, Petersen, Dennis, Gavriljuk, Konstantin, El-Mashtoly, Samir F., Hegemann, Peter, Gerwert, Klaus
Formato: Online Artículo Texto
Lenguaje:English
Publicado: National Academy of Sciences 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6510988/
https://www.ncbi.nlm.nih.gov/pubmed/31004059
http://dx.doi.org/10.1073/pnas.1818707116
Descripción
Sumario:Although channelrhodopsin (ChR) is a widely applied light-activated ion channel, important properties such as light adaptation, photocurrent inactivation, and alteration of the ion selectivity during continuous illumination are not well understood from a molecular perspective. Herein, we address these open questions using single-turnover electrophysiology, time-resolved step-scan FTIR, and Raman spectroscopy of fully dark-adapted ChR2. This yields a unifying parallel photocycle model integrating now all so far controversial discussed data. In dark-adapted ChR2, the protonated retinal Schiff base chromophore (RSBH(+)) adopts an all-trans,C=N-anti conformation only. Upon light activation, a branching reaction into either a 13-cis,C=N-anti or a 13-cis,C=N-syn retinal conformation occurs. The anti-cycle features sequential H(+) and Na(+) conductance in a late M-like state and an N-like open-channel state. In contrast, the 13-cis,C=N-syn isomer represents a second closed-channel state identical to the long-lived P(480) state, which has been previously assigned to a late intermediate in a single-photocycle model. Light excitation of P(480) induces a parallel syn-photocycle with an open-channel state of small conductance and high proton selectivity. E90 becomes deprotonated in P(480) and stays deprotonated in the C=N-syn cycle. Deprotonation of E90 and successive pore hydration are crucial for late proton conductance following light adaptation. Parallel anti- and syn-photocycles now explain inactivation and ion selectivity changes of ChR2 during continuous illumination, fostering the future rational design of optogenetic tools.