2020
DOI: 10.1103/physrevb.101.165309
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Chiral Hall effect in strained Weyl semimetals

Abstract: In this paper, the chiral Hall effect of strained Weyl semimetals without any external magnetic field is proposed. The electron-phonon coupling emerges in the low-energy fermionic particle through a pseudogauge potential. We show, by using chiral kinetic theory, that the chiral Hall effect emerges as a response of a real time-varying electric field in the presence of the structural distortion and it leads to a spatial chirality and charges separation in the system. We also show that the coupling of the electro… Show more

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Cited by 25 publications
(11 citation statements)
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“…[ 12–14 ] Recently, interest has focused on the exploitation of the unusual properties of their electronic structure to observe unique physical phenomena, such as the chiral [ 15–17 ] and axial‐gravitational anomaly, [ 18 ] the circular photogalvanic effect, [ 19–20 ] chiral sound waves, [ 21–22 ] the surface‐state enhanced Edelstein effect [ 23 ] or the recently proposed chiral Hall‐effect. [ 24 ] The observation of most of these effects depends on whether the topological electronic states of the WSMs can be readily accessed. In this regard, the ability to suppress non‐topological (trivial) surface states, as well as to modify the Fermi‐level position to get a desired Fermi surface topology, would allow full access to unveil the role of topological surface states on physical observables, and, in addition, to construct on‐demand Fermi‐surfaces to harness electrical, acoustic or optical measurable outputs.…”
Section: Introductionmentioning
confidence: 99%
“…[ 12–14 ] Recently, interest has focused on the exploitation of the unusual properties of their electronic structure to observe unique physical phenomena, such as the chiral [ 15–17 ] and axial‐gravitational anomaly, [ 18 ] the circular photogalvanic effect, [ 19–20 ] chiral sound waves, [ 21–22 ] the surface‐state enhanced Edelstein effect [ 23 ] or the recently proposed chiral Hall‐effect. [ 24 ] The observation of most of these effects depends on whether the topological electronic states of the WSMs can be readily accessed. In this regard, the ability to suppress non‐topological (trivial) surface states, as well as to modify the Fermi‐level position to get a desired Fermi surface topology, would allow full access to unveil the role of topological surface states on physical observables, and, in addition, to construct on‐demand Fermi‐surfaces to harness electrical, acoustic or optical measurable outputs.…”
Section: Introductionmentioning
confidence: 99%
“…Two years after this theoretical work, Weyl points were experimentally observed in the microwave frequency range [8]. Following this first experimental demonstration, the realization of Weyl points has been achieved using photonic crystals [9,10,43,44,[55][56][57][58][59][60], phononic crystals [3,14,[61][62][63][64][65][66], metals [67][68][69][70] and semimetals [71][72][73][74][75][76][77].…”
Section: Band Degeneraciesmentioning
confidence: 97%
“…For example, elastic gauge field interactions ("pseudo-magnetic fields") have been addressed in Refs. [70,[99][100][101][102][103], and piezoelectric interactions can be important in WSMs with broken inversion symmetry [104]. With minor modifications, those couplings can be included in our theory, see also Ref.…”
Section: Electron-phonon Interactionmentioning
confidence: 99%