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Fermi surface magnetization of Fe-doped NbSb$_2$ investigated by magnetic quantum oscillations

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arxiv 2104.07948 v2 pith:6FKOWBSL submitted 2021-04-16 cond-mat.mes-hall

classification cond-mat.mes-hall
keywords fermisurfacephasemagneticmagnetizationmqosnbsbdoped
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abstract

Magnetic quantum oscillations (MQOs) have been widely used as a tool for probing Fermi surfaces. The shape and topology of the Fermi surface and the related physical parameters, such as the cyclotron mass and relaxation time, can be verified by carefully analyzing the frequency, amplitude, and phase of MQOs. In particular, phase analysis, from which we can obtain the Berry phase, has received much attention with the growing interest in the topology of condensed matter physics. Here, beyond the conventional uses of MQOs, we show that MQOs can be used to determine the Fermi surface magnetization. We doped dilute magnetic element Fe into the Dirac semimetal NbSb$_2$ to only introduce magnetism without changing the shape of the Fermi surface. We observed a phase shift in magnetically doped Fe-NbSb$_2$, which is in contrast to the lack of a phase shift in pristine NbSb$_2$ and nonmagnetic Bi-doped NbSb$_2$, indicating the strong exchange interaction between doped magnetic impurities and Fermi surface electrons. We estimated the Fermi surface magnetization introduced by magnetic Fe doping from the phase shift. This work demonstrates not only how tiny magnetic impurities can significantly change the Fermi surface magnetization but also how the Fermi surface magnetization can be investigated by phase analysis of MQOs.

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Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. OpenAlex reports about 2 citations worldwide. Full citation record

  1. Inhomogeneity identification by measuring magnetic quantum oscillations

    cond-mat.mtrl-sci 2025-07 conditional novelty 5.0 of 10

    Inhomogeneous Cr doping in NbSb2 produces a phase shift and nonlinear amplitude in de Haas-van Alphen oscillations that the authors model with an asymmetric Fermi-energy distribution.

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