2020
DOI: 10.1103/physrevlett.124.104301
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Discovering Topological Surface States of Dirac Points

Abstract: Dirac materials, unlike the Weyl materials, have not been found in experiments to support intrinsic topological surface states, as the surface arcs in existing systems are unstable against symmetrypreserving perturbations. Utilizing the proposed glide and time-reversal symmetries, we theoretically design and experimentally verify an acoustic crystal of two frequency-isolated three-dimensional Dirac points with Z2 monopole charges and four gapless helicoid surface states. arXiv:2001.06205v1 [cond-mat.mtrl-sci]

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Cited by 48 publications
(40 citation statements)
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“…The design of our sonic crystal enables us to observe not only the hinge states in frequency-resolved spectroscopy but also their spatial localization in pressure-field distributions. Not only is this HO Dirac sonic crystal sharply different from the conventional solid-state Dirac semimetals that are characterized by surface Fermi arcs 3,16,17 , but it is also markedly different from the recently achieved non-symmorphic Dirac sonic crystals that feature symmetry-enforced Dirac points and quad-helicoid surface arcs 32,33 . Last but not at least, our scheme for achieving spinless 3D HO topological phases can be readily generalized to other classical wave systems such as photonic crystals with similar space groups.…”
Section: Co-dimensioncontrasting
confidence: 56%
“…The design of our sonic crystal enables us to observe not only the hinge states in frequency-resolved spectroscopy but also their spatial localization in pressure-field distributions. Not only is this HO Dirac sonic crystal sharply different from the conventional solid-state Dirac semimetals that are characterized by surface Fermi arcs 3,16,17 , but it is also markedly different from the recently achieved non-symmorphic Dirac sonic crystals that feature symmetry-enforced Dirac points and quad-helicoid surface arcs 32,33 . Last but not at least, our scheme for achieving spinless 3D HO topological phases can be readily generalized to other classical wave systems such as photonic crystals with similar space groups.…”
Section: Co-dimensioncontrasting
confidence: 56%
“…In addition, they are neighbors to many novel topological phases and thus serve as ideal platforms for investigating topological phase transitions 19 . Three-dimensional Dirac semimetals have been observed in both electronic systems and classical waves 19,[29][30][31] . In electronic systems, DNLSs are possible in the absence of spin-orbital couplings [16][17][18] .…”
Section: Introductionmentioning
confidence: 99%
“…The milestone of topological physics dates back to the discovery of quantum Hall phases, where 2D electron gas under a perpendicular magnetic field has quantized Hall conductance [28]. Because the magnetic field broke T, electrons in the quantum Hall effect propagate one way along the boundary, generating the chiral current.…”
Section: D Topological Semimetal Phasesmentioning
confidence: 99%
“…The number of gapless edge modes inside a bandgap is determined by the difference of gap Chern number, which is the summation of all band Chern numbers below the bandgap, also known as the bulk-edge correspondence. When T is broken with magnetic field, the photonic quantum Hall effect can also emerge in photonic crystals composed of magnetoelectric or gyromagnetic materials [14,15,[28][29][30]. The magnetoelectric materials have cross-coupling between electric and magnetic fields, where the constitutive relations take the form of D εE + χH and B μH + ζE.…”
Section: D Topological Semimetal Phasesmentioning
confidence: 99%