2020
DOI: 10.1063/1.5129467
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Magnetic exchange induced Weyl state in a semimetal EuCd2Sb2

Abstract: Magnetic Weyl semimetals (WSMs) bearing long-time pursuing are still very rare. We herein identified magnetic exchange induced Weyl state in EuCd 2 Sb 2 , a semimetal in type IV magnetic space group, via performing high magnetic field

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Cited by 52 publications
(38 citation statements)
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“…We are confident that the conductance scaling uncovered in this work can be observed in experiment, considering the recent efforts in manufacturing microstructured Weyl semimetals [38], creating strain-induced fields in type-II Weyl semimetals [39], and transport experiments in Dirac nanowires [40,41]. As our results rely on time-reversal symmetry-breaking materials, magneticexchange induced Weyl semimetals [42,43] are promising platforms for experiments. We have uncovered the conditions necessary to observe the unusual scaling of the conductivity: The sample's width needs to be larger than the magnetic length, and the sample's length in transport direction needs to be larger than the mean free path.…”
supporting
confidence: 59%
“…We are confident that the conductance scaling uncovered in this work can be observed in experiment, considering the recent efforts in manufacturing microstructured Weyl semimetals [38], creating strain-induced fields in type-II Weyl semimetals [39], and transport experiments in Dirac nanowires [40,41]. As our results rely on time-reversal symmetry-breaking materials, magneticexchange induced Weyl semimetals [42,43] are promising platforms for experiments. We have uncovered the conditions necessary to observe the unusual scaling of the conductivity: The sample's width needs to be larger than the magnetic length, and the sample's length in transport direction needs to be larger than the mean free path.…”
supporting
confidence: 59%
“…Other candidate materials to observe this effect include ferromagnetic Weyl semimetals which have been recently identified experimentally [11][12][13][17][18][19][20] and are also captured by our theory. Specifically, we consider EuCd 2 As 2 , whose ground state is an itinerant magnet where Eu ions form ferromagnetic layers stacked antiferromagnetically along the c-axis.…”
Section: Introduction-mentioning
confidence: 60%
“…The M(r) · b term breaks the TR symmetry, and M(r) = M (r)(sin θ(r) cos φ(r), sin θ(r) sin φ(r), cos θ(r)) corresponds to 3-dimensional (3d) magnetization or any field that transforms as magnetization under TR. It can be used to describe real materials such as 3d topological insulators (TI) with magnetic texture [14], topological insulator heterostructures [15,16] or ferromagnetic Weyl semimetals discovered recently [11][12][13][17][18][19][20]. Following the general method introduced in Refs.…”
Section: Introduction-mentioning
confidence: 99%
“…Here, we introduce 1D reactions with extreme transformation of the 2D‐Xene covalent framework and recruit them to illustrate the concept of reaction dimensionality and its use for synthesis control at the nanoscale. Starting with MX 2 , we produce films of layered MA 2 X 2 phases—a numerous class of materials best known for thermoelectric properties [ 26 ] but also boasting topological properties established by both theory [ 27–29 ] and recent experiments on magnetically induced Weyl [ 30–32 ] and Dirac [ 33 ] states. We prove that 1D reactions make a synthetic route to produce MA 2 X 2 for a selection of M and X, probe different templates, establish the reaction mechanism.…”
Section: Introductionmentioning
confidence: 99%