Location via proxy:   [ UP ]  
[Report a bug]   [Manage cookies]                

Making Topologically Trivial Non-Hermitian Systems Nontrivial via Gauge Fields

W. B. Rui, Y. X. Zhao, and Z. D. Wang
Phys. Rev. Lett. 131, 176402 – Published 25 October 2023
PDFHTMLExport Citation

Abstract

Non-Hermiticity significantly enriches the concepts of symmetry and topology in physics. Particularly, non-Hermiticity gives rise to the ramified symmetries, where the non-Hermitian Hamiltonian H is transformed to H. For time-reversal (T) and sublattice symmetries, there are six ramified symmetry classes leading to novel topological classifications with various non-Hermitian skin effects. As artificial crystals are the main experimental platforms for non-Hermitian physics, there exists the symmetry barrier for realizing topological physics in the six ramified symmetry classes: while artificial crystals are in spinless classes with T2=1, nontrivial classifications dominantly appear in spinful classes with T2=1. Here, we present a general mechanism to cross the symmetry barrier. With an internal parity symmetry P, the square of the combination T˜=PT can be modified by appropriate gauge fluxes. Using the general mechanism, we systematically construct spinless models for all non-Hermitian spinful topological phases in one and two dimensions, which are experimentally realizable. Our Letter suggests that gauge structures may significantly enrich non-Hermitian physics at the fundamental level.

  • Figure
  • Figure
  • Figure
  • Received 2 December 2022
  • Revised 15 February 2023
  • Accepted 22 September 2023

DOI:https://doi.org/10.1103/PhysRevLett.131.176402

© 2023 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied PhysicsAtomic, Molecular & OpticalInterdisciplinary Physics

Authors & Affiliations

W. B. Rui*, Y. X. Zhao, and Z. D. Wang

  • Department of Physics and HK Institute of Quantum Science & Technology, The University of Hong Kong, Pokfulam Road, Hong Kong, China

  • *wbrui@hku.hk
  • yuxinphy@hku.hk
  • zwang@hku.hk

Article Text (Subscription Required)

Click to Expand

Supplemental Material (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 131, Iss. 17 — 27 October 2023

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×

Images

  • Figure 1
    Figure 1

    (a) Classification of spinless (upper table) and spinful (lower table) classes with ramified time-reversal and sublattice symmetries for point-gap topological phases [22, 42]. See Ref. [43] for the connection of our convention to the previous convention of the symmetry classes. The symmetry barrier between spinless and spinful classes can be crossed by gauge field. (b) Rectangle with π gauge flux, invariant under the projective twofold rotation. (c) Twisted rectangle with π gauge flux, invariant under the projective mirror reflection. Blue and red denote the + and hopping amplitudes, respectively. The gauge transformations (G) are specified by the signs in the two middle panels.

    Reuse & Permissions
  • Figure 2
    Figure 2

    (a) Schematic picture for the 1D spinless chain. The unit cell is constructed by the rectangle in Fig. 1, which is marked by gray. (b) The Z2 non-Hermitian skin effect. For the Hamiltonian with 100 unit cells under the open boundary conditions, we compute all the energy eigenstates |ψE with energy E. For each E, we plot PE(x)=α|x,α|ψE|2, where |x,α is the on-site state at αth site in the xth unit cell. (c) The energy spectra and (d) the generalized Brillouin zone (blue and red) of the system. The black circle in (d) denotes |β|=1. The parameters are JR=JI=1.5, t=μ=1, γ=2.

    Reuse & Permissions
  • Figure 3
    Figure 3

    (a1) Schematic picture for the 2D lattice in AII class. The unit cell marked in gray. (a2) The nonreciprocal hoppings in the y direction. (a3) The PBC spectrum, and (a4) the topological invariant of the system. (a5) The non-Hermitian flux skin effect, which is localized at the cores of the π flux defects. At the (x,y) position, the density is ρ(x,y)=α,β|x,y,α|ψβ|2, where α runs over all internal degrees of unit cell and β all eigenstates. Full PBC is taken to avoid boundary effects. The parameters are JR=JI=1.5, γ=tr=2, t=tl=1. (b1) Schematic picture for the bilayer hexagonal lattice. The two layers are connected by lattice blocks adjusted from Fig. 1, as shown in the right. (b2) The PBC spectrum of the system, and (b3) the Wilson loop spectrum. The parameters are t=JI=1, JR=0.1.

    Reuse & Permissions
×

Sign up to receive regular email alerts from Physical Review Letters

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×