2022
DOI: 10.48550/arxiv.2203.04254
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Field-dependent Shubnikov-de Haas oscillations in ferromagnetic Weyl semimetal Co3Sn2S2

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“…A common source is due to the non-ideal placement of contacts, which can result in a finite percentage of longitudinal resistance in the transverse signal. In addition, it has been recently shown that the band structure of this compound is not symmetric between parallel and antiparallel configurations of M with respect to the c-axis, a property which has been reflected in quantum Shubnikov-de Haas oscillation [42]. Consequently, we may expect an additional asymmetry of the transverse resistivity between the parallel and antiparallel orientation of the magnetization with the c-axis (β = 0 • versus β = 180 • ).…”
Section: Experimental Setup and Methodsmentioning
confidence: 94%
“…A common source is due to the non-ideal placement of contacts, which can result in a finite percentage of longitudinal resistance in the transverse signal. In addition, it has been recently shown that the band structure of this compound is not symmetric between parallel and antiparallel configurations of M with respect to the c-axis, a property which has been reflected in quantum Shubnikov-de Haas oscillation [42]. Consequently, we may expect an additional asymmetry of the transverse resistivity between the parallel and antiparallel orientation of the magnetization with the c-axis (β = 0 • versus β = 180 • ).…”
Section: Experimental Setup and Methodsmentioning
confidence: 94%