2021
DOI: 10.1103/prxquantum.2.020320
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Quantum Dynamical Characterization and Simulation of Topological Phases With High-Order Band Inversion Surfaces

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Cited by 25 publications
(12 citation statements)
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“…We begin with an introduction of the nested-BIS method for constructing and characterizing HOTPs with arbitrary orders of topology in arbitrary dimensions [34]. This method is built on the BISs and high-order BISs used to dynamically characterize the first-order topological phases, where mth-order BISs are given by a special region in the Brillouin zone with m vanishing pseudo-spin components of the Hamiltonian, denoted as m-BISs [41,42]. Following the nested-BIS method, a dD Hamiltonian hosting nth-order topology can be constructed as…”
Section: The Nested Band Inversion Surfacesmentioning
confidence: 99%
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“…We begin with an introduction of the nested-BIS method for constructing and characterizing HOTPs with arbitrary orders of topology in arbitrary dimensions [34]. This method is built on the BISs and high-order BISs used to dynamically characterize the first-order topological phases, where mth-order BISs are given by a special region in the Brillouin zone with m vanishing pseudo-spin components of the Hamiltonian, denoted as m-BISs [41,42]. Following the nested-BIS method, a dD Hamiltonian hosting nth-order topology can be constructed as…”
Section: The Nested Band Inversion Surfacesmentioning
confidence: 99%
“…The starting point of this work is a method known as the nested band inversion surfaces (BISs), which has been employed to explore HOTPs in A and AIII classes of the AZ classes [34]. This method is built on the concept of BISs, which offers a powerful and innovative approach to probe 1st-order topological invariants through quantum dynamics [41][42][43]. Inhabiting this advantage, the nested-BIS method allows us to construct higher-order topology from 1st-order one of different parts of the system's Hamiltonian.…”
Section: Introductionmentioning
confidence: 99%
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“…Despite the fact that topological phases are defined at the ground state at equilibrium, quantum quenches in recent studies provide nonequilibrium way to investigate topological physics [14][15][16][17][18][19][20][21][22][23][24][25][26][27][28] . Particularly, as a momentum-space counterpart of the bulk-boundary correspondence, the dynamical bulksurface correspondence was proposed [29][30][31][32][33][34] , which relates the bulk topology of an equilibrium phase to nontrivial dynamical topological phase emerging on certain momentum subspaces called band-inversion surfaces (BISs) when quenching the system across topological transitions. This dynamical topology enables a broadly applicable way to characterize and detect topological phases by quantum dynamics, and has triggered many experimental studies in quantum simulations, such as in ultracold atoms 35,36 , nitrogen-vacancy defects in diamond [37][38][39] , nuclear magnetic resonance (NMR) 40 , and superconducting circuits 41 .…”
Section: Introductionmentioning
confidence: 99%
“…Introduction-Intriguing physical phenomena, such as topological phases, can emerge from symmetries, which play an important role in determining a system properties [1][2][3][4][5][6][7]. Symmetries can lead to general universality classes, so that, for example, phases of topological insulators can be arranged into a periodic table [1].…”
mentioning
confidence: 99%