TY - JOUR
T1 - Unreliability of two-band model analysis of magnetoresistivities in unveiling temperature-driven Lifshitz transition
AU - Xu, Jing
AU - Wang, Yu
AU - Pate, Samuel E.
AU - Zhu, Yanglin
AU - Mao, Zhiqiang
AU - Zhang, Xufeng
AU - Zhou, Xiuquan
AU - Welp, Ulrich
AU - Kwok, Wai Kwong
AU - Chung, Duck Young
AU - Kanatzidis, Mercouri G.
AU - Xiao, Zhi Li
N1 - Funding Information:
Magnetotransport measurements and data analysis were supported by the U.S. Department of Energy (DOE), Office of Science, Basic Energy Sciences, Materials Sciences and Engineering. Crystal growth at Penn State was supported by the DOE under Grant No. DE-SC0019068. S.E.P. and Z.L.X. received support from the National Science Foundation (Grant No. DMR-1901843). Work performed at the Center for Nanoscale Materials, a DOE Office of Science User Facility, was supported by the DOE, Office of Basic Energy Sciences, under Contract No. DE-AC02-06CH11357.
Publisher Copyright:
© 2023 American Physical Society.
PY - 2023/1/15
Y1 - 2023/1/15
N2 - Recently, anomalies in the temperature dependences of the carrier density and/or mobility derived from analysis of the magnetoresistivities using the conventional two-band model have been used to unveil intriguing temperature-induced Lifshitz transitions in various materials. For instance, two temperature-driven Lifshitz transitions were inferred to exist in the Dirac nodal-line semimetal ZrSiSe, based on two-band model analysis of the Hall magnetoconductivities where the second band exhibits a change in the carrier type from holes to electrons when the temperature decreases below T=106K and a dip is observed in the mobility vs temperature curve at T=80K. Here, we revisit the experiments and two-band model analysis on ZrSiSe. We show that the anomalies in the second band may be spurious because the first band dominates the Hall magnetoconductivities at T>80K, making the carrier type and mobility obtained for the second band from the two-band model analysis unreliable. That is, care must be taken in interpreting these anomalies as evidence for temperature-driven Lifshitz transitions. Our skepticism on the existence of such phase transitions in ZrSiSe is further supported by the validation of Kohler's rule for magnetoresistances for T≤180K. In this paper, we showcase potential issues in interpreting anomalies in the temperature dependence of the carrier density and mobility derived from the analysis of magnetoconductivities or magnetoresistivities using the conventional two-band model.
AB - Recently, anomalies in the temperature dependences of the carrier density and/or mobility derived from analysis of the magnetoresistivities using the conventional two-band model have been used to unveil intriguing temperature-induced Lifshitz transitions in various materials. For instance, two temperature-driven Lifshitz transitions were inferred to exist in the Dirac nodal-line semimetal ZrSiSe, based on two-band model analysis of the Hall magnetoconductivities where the second band exhibits a change in the carrier type from holes to electrons when the temperature decreases below T=106K and a dip is observed in the mobility vs temperature curve at T=80K. Here, we revisit the experiments and two-band model analysis on ZrSiSe. We show that the anomalies in the second band may be spurious because the first band dominates the Hall magnetoconductivities at T>80K, making the carrier type and mobility obtained for the second band from the two-band model analysis unreliable. That is, care must be taken in interpreting these anomalies as evidence for temperature-driven Lifshitz transitions. Our skepticism on the existence of such phase transitions in ZrSiSe is further supported by the validation of Kohler's rule for magnetoresistances for T≤180K. In this paper, we showcase potential issues in interpreting anomalies in the temperature dependence of the carrier density and mobility derived from the analysis of magnetoconductivities or magnetoresistivities using the conventional two-band model.
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U2 - 10.1103/PhysRevB.107.035104
DO - 10.1103/PhysRevB.107.035104
M3 - Article
AN - SCOPUS:85146340995
SN - 2469-9950
VL - 107
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 3
M1 - 035104
ER -