Bulletin of the American Physical Society
APS March Meeting 2021
Volume 66, Number 1
Monday–Friday, March 15–19, 2021; Virtual; Time Zone: Central Daylight Time, USA
Session J51: Dirac and Weyl Semimetals: Materials and Modeling -- Transport
3:00 PM–6:00 PM,
Tuesday, March 16, 2021
Sponsoring
Units:
DMP DCMP
Chair: Jin Hu, University of Arkansas
Abstract: J51.00009 : Giant magnetoresistance and CDW instability in the quantum limit of correlated Dirac semimetal CaIrO3
5:24 PM–5:36 PM
Live
Presenter:
Rinsuke Yamada
(Department of Applied Physics, University of Tokyo)
Authors:
Rinsuke Yamada
(Department of Applied Physics, University of Tokyo)
Jun Fujioka
(Faculty of Material Science, University of Tsukuba)
Minoru Kawamura
(CEMS, RIKEN)
Shiro Sakai
(CEMS, RIKEN)
Motoaki Hirayama
(CEMS, RIKEN)
Ryotaro Arita
(CEMS, RIKEN)
Tatsuta Okawa
(Department of Applied Physics, University of Tokyo)
Daisuke Hashizume
(CEMS, RIKEN)
Takuro Sato
(CEMS, RIKEN)
Fumitaka Kagawa
(CEMS, RIKEN)
Ryosuke Kurihara
(ISSP, University of Tokyo)
Masashi Tokunaga
(ISSP, University of Tokyo)
Yoshinori Tokura
(CEMS, RIKEN)
In this study, we report the magnetoresistance up to 55 T for CaIrO3, which is a strongly-correlated Dirac semimetal on the verge of Mott transition[1,2]. We observed the giant positive longitudinal magnetoresistance in the QL, which steeply increases at 9 T, shows a peak around 18 T, and decreases at higher field. The activation energy derived by the Arrhenius plot also shows non-monotonic magnetic field dependence, which agrees well with the theoretical model of CDW instability[3]. Combining with the results of non-linear current-voltage property, we propose that disordered CDW is formed in the intermediate field region (9-25 T) of QL in CaIrO3.
[1] M. Zeb and H. Kee, PRB 86, 085149 (2012)
[2] J. Fujioka et al., Nat. Commun. 10, 362 (2019)
[3] H. Fukuyama, Solid State Commun. 26, 783 (1978)
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