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Electric circuits for non-Hermitian Chern insulators

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arxiv 1904.03823 v2 pith:YJXINQ5W submitted 2019-04-08 cond-mat.mes-hall

classification cond-mat.mes-hall
keywords non-hermitianimpedancephasechiralbecomeschernedgemass
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abstract

We analyze the non-Hermitian Haldane model where the spin-orbit interaction is made non-Hermitian. The Dirac mass becomes complex. We propose to realize it by an $LC$ circuit with operational amplifiers. A topological phase transition is found to occur at a critical point where the real part of the bulk spectrum is closed. The Chern number changes its value when the real part of the mass becomes zero. In the topological phase of a nanoribbon, two non-Hermitian chiral edges emerge connecting well separated conduction and valence bands. The emergence of the chiral edge states is signaled by a strong enhancement in impedance. Remarkably it is possible to observe either the left-going or right-going chiral edge by measuring the one-point impedance. Furthermore, it is also possible to distinguish them by the phase of the two-point impedance. Namely, the phase of the impedance acquires a dynamical degree of freedom in the non-Hermitian system.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Electric Circuit Realizations of Fracton Physics

    cond-mat.str-el 2019-08 conditional novelty 7.0 of 10

    Networks of capacitors connected by ideal transformers conserve dipole moment, making electric charge immobile like fractons, with a linear steady-state charge profile.

  2. Reciprocal skin effect and its realization in a topolectrical circuit

    cond-mat.mes-hall 2019-08 conditional novelty 7.0 of 10

    A reciprocal non-Hermitian 2D lattice shows skin-mode localization on opposite edges for opposite momenta, demonstrated experimentally in a passive RLC circuit.

  3. Transport across a topoelectrical Weyl semimetal heterojunction

    cond-mat.mes-hall 2019-08 conditional novelty 6.0 of 10

    Topoelectrical LC circuits can emulate Weyl semimetal heterojunctions, with energy flux transmission that depends on tilt orientation and an anti-Klein tunneling effect at the Type I to Type III phase transition.

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