作者
Dion Tjhe,Xinglong Ren,Ian E. Jacobs,Gabriele D’Avino,Tarig Mustafa,T. R. Marsh,Lu Zhang,Yao Fu,Ahmed E. Mansour,Andreas Opitz,Yuxuan Huang,Wenjin Zhu,Ahmet Hamdi Unal,S. van der Hoek,Vincent Lemaur,Claudio Quarti,Qiao He,Jin‐Kyun Lee,Iain McCulloch,Martin Heeney,Norbert Koch,Yanting Jin,David Beljonne,Simone Fratini,Henning Sirringhaus
摘要
Abstract Conducting polymers are mixed ionic–electronic conductors that are emerging candidates for neuromorphic computing, bioelectronics and thermoelectrics. However, fundamental aspects of their many-body correlated electron–ion transport physics remain poorly understood. Here we show that in p-type organic electrochemical transistors it is possible to remove all of the electrons from the valence band and even access deeper bands without degradation. By adding a second, field-effect gate electrode, additional electrons or holes can be injected at set doping states. Under conditions where the counterions are unable to equilibrate in response to field-induced changes in the electronic carrier density, we observe surprising, non-equilibrium transport signatures that provide unique insights into the interaction-driven formation of a frozen, soft Coulomb gap in the density of states. Our work identifies new strategies for substantially enhancing the transport properties of conducting polymers by exploiting non-equilibrium states in the coupled system of electronic charges and counterions.