Rules for dissipationless topotronics

Author:

Yan Qing1ORCID,Li Hailong1ORCID,Jiang Hua23ORCID,Sun Qing-Feng14ORCID,Xie X. C.124ORCID

Affiliation:

1. International Center for Quantum Materials, School of Physics, Peking University, Beijing 100871, China.

2. Interdisciplinary Center for Theoretical Physics and Information Sciences (ICTPIS), Fudan University, Shanghai 200433, China.

3. Institute for Nanoelectronic Devices and Quantum Computing and State Key Laboratory of Surface Physics, Fudan University, Shanghai 200433, China.

4. Hefei National Laboratory, Hefei 230088, China.

Abstract

Topological systems hosting gapless boundary states have attracted huge attention as promising components for next-generation information processing, attributed to their capacity for dissipationless electronics. Nevertheless, recent theoretical and experimental inquiries have revealed the emergence of energy dissipation in precisely quantized electrical transport. Here, we present a criterion for the realization of truly no-dissipation design, characterized as N in = N tunl + N bs , where N in , N tunl , and N bs represent the number of modes participating in injecting, tunneling, and backscattering processes, respectively. The key lies in matching the number of injecting, tunneling, and backscattering modes, ensuring the equilibrium among all engaged modes inside the device. Among all the topological materials, we advocate for the indispensability of Chern insulators exhibiting higher Chern numbers to achieve functional devices and uphold the no-dissipation rule simultaneously. Furthermore, we design the topological current divider and collector, evading dissipation upon fulfilling the established criterion. Our work paves the path for developing the prospective topotronics.

Publisher

American Association for the Advancement of Science (AAAS)

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