Anisotropic electrical and thermal magnetotransport in the magnetic semimetal GdPtBi

  • Clemens Schindler
  • , Stanislaw Galeski
  • , Walter Schnelle
  • , Rafał Wawrzyńczak
  • , Wajdi Abdel-Haq
  • , Satya N. Guin
  • , Johannes Kroder
  • , Nitesh Kumar
  • , Chenguang Fu
  • , Horst Borrmann
  • , Chandra Shekhar
  • , Claudia Felser
  • , Tobias Meng
  • , Adolfo G. Grushin
  • , Yang Zhang
  • , Yan Sun
  • , Johannes Gooth

Research output: Contribution to journalArticlepeer-review

32 Scopus citations

Abstract

The half-Heusler rare-earth intermetallic GdPtBi has recently gained attention due to peculiar magnetotransport phenomena that have been associated with the possible existence of Weyl fermions, thought to arise from the crossings of spin-split conduction and valence bands. On the other hand, similar magnetotransport phenomena observed in other rare-earth intermetallics have often been attributed to the interaction of itinerant carriers with localized magnetic moments stemming from the 4f shell of the rare-earth element. In order to address the origin of the magnetotransport phenomena in GdPtBi, we performed a comprehensive study of the magnetization, electrical, and thermal magnetoresistivity on two single-crystalline GdPtBi samples. In addition, we performed an analysis of the Fermi surface via Shubnikov-de Haas oscillations in one of the samples and compared the results to ab initio band structure calculations. Our findings indicate that the electrical and thermal magnetotransport in GdPtBi cannot be solely explained by Weyl physics and is strongly influenced by the interaction of both itinerant charge carriers and phonons with localized magnetic Gd ions and possibly also paramagnetic impurities.

Original languageEnglish
Article number125119
JournalPhysical Review B
Volume101
Issue number12
DOIs
StatePublished - Mar 15 2020

Funding

Cl.S. thanks R. Koban for providing technical support and C. Geibel for engaging in clarifying discussions. This work was financially supported by the ERC Advanced Grant No. 291472 “Idea Heusler” and ERC Advanced Grant No. 742068 “TOPMAT.” Cl.S. acknowledges financial support by the International Max Planck Research School for Chemistry and Physics of Quantum Materials (IMPRS-CPQM). A.G.G. thanks J. Cano, B. Bradlyn, and R. Ilan for engaging in clarifying discussions. A.G.G. acknowledges financial support from the Marie Curie programme under EC Grant Agreement No. 653846. T.M. acknowledges funding by the Deutsche Forschungsgemeinschaft through the Emmy Noether Programme ME 4844/1-1 and through SFB 1143.

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