RUS  ENG
Full version
JOURNALS // Pis'ma v Zhurnal Èksperimental'noi i Teoreticheskoi Fiziki // Archive

Pis'ma v Zh. Èksper. Teoret. Fiz., 2021 Volume 113, Issue 8, Pages 533–538 (Mi jetpl6409)

This article is cited in 4 papers

CONDENSED MATTER

Anisotropy of the hall effect in the paramagnetic phase of Ho$_{0.8}$Lu$_{0.2}$B$_{12}$ cage glass

A. L. Khoroshilova, A. N. Azarevicha, A. V. Bogacha, V. V. Glushkova, S. V. Demishevba, V. N. Krasnorusskya, K. M. Krasikova, A. V. Kuznetsovc, N. Yu. Shitsevalovad, V. B. Filipovd, N. E. Sluchankoa

a Prokhorov General Physics Institute, Russian Academy of Sciences, Moscow, 119991 Russia
b National Research University Higher School of Economics, Moscow, 101000 Russia
c National Research Nuclear University MEPhI (Moscow Engineering Physics Institute), Moscow, 115409 Russia
d Frantsevich Institute for Problems of Materials Science, National Academy of Sciences of Ukraine, Kyiv, 03680 Ukraine

Abstract: Detailed measurements of the Hall effect in the paramagnetic phase of Ho$_{0.8}$Lu$_{0.2}$B$_{12}$ antiferromagnet at the magnetic field up to $80$ kOe in the temperature range of $1.9$$300$ K have been performed. It has been found that the transition to the cage glass phase ($T<T^*\sim60\,$K) is accompanied by the appearance of a positive Hall resistance component in addition to that corresponding to the negative Hall effect. The amplitude and angular dependence of the former depend on the magnitude and direction of the applied magnetic field with respect to the crystallographic axes. The revealed anisotropy of the Hall effect in Ho$_{0.8}$Lu$_{0.2}$B$_{12}$ is attributed to the interaction of charge carriers with dynamic charge stripes.

Received: 16.02.2021
Revised: 17.03.2021
Accepted: 17.03.2021

DOI: 10.31857/S1234567821080073


 English version:
Journal of Experimental and Theoretical Physics Letters, 2021, 113:8, 526–531

Bibliographic databases:


© Steklov Math. Inst. of RAS, 2024