Probing FeSi, a d -electron topological Kondo insulator candidate, with magnetic field, pressure, and microwaves

Author:

Breindel Alexander J.1,Deng Yuhang1,Moir Camilla M.1,Fang Yuankan1,Ran Sheng1,Lou Hongbo2,Li Shubin23,Zeng Qiaoshi2ORCID,Shu Lei45ORCID,Wolowiec Christian T.1ORCID,Schuller Ivan K.1,Rosa Priscila F. S.6,Fisk Zachary7,Singleton John6,Maple M. Brian1

Affiliation:

1. Department of Physics, University of California San Diego, La Jolla, CA 92093

2. Center for High Pressure Science and Technology Advanced Research, Pudong, Shanghai 201203, People’s Republic of China

3. Univ Lyon, Université Claude Bernard Lyon 1, CNRS, Institut Lumière Matière, Villeurbanne 69100, France

4. State Key Laboratory of Surface Physics, Department of Physics, Fudan University, Shanghai 200433, People’s Republic of China

5. Shanghai Research Center for Quantum Sciences, Shanghai 201315, People’s Republic of China

6. Los Alamos National Laboratory, Los Alamos, NM 87545

7. University of California Irvine, Irvine, CA 92967

Abstract

Recently, evidence for a conducting surface state (CSS) below 19 K was reported for the correlated d -electron small gap semiconductor FeSi. In the work reported herein, the CSS and the bulk phase of FeSi were probed via electrical resistivity ρ measurements as a function of temperature T , magnetic field B to 60 T, and pressure P to 7.6 GPa, and by means of a magnetic field-modulated microwave spectroscopy (MFMMS) technique. The properties of FeSi were also compared with those of the Kondo insulator SmB 6 to address the question of whether FeSi is a d -electron analogue of an f -electron Kondo insulator and, in addition, a “topological Kondo insulator” (TKI). The overall behavior of the magnetoresistance of FeSi at temperatures above and below the onset temperature T S = 19 K of the CSS is similar to that of SmB 6 . The two energy gaps, inferred from the ρ( T ) data in the semiconducting regime, increase with pressure up to about 7 GPa, followed by a drop which coincides with a sharp suppression of T S . Several studies of ρ( T ) under pressure on SmB 6 reveal behavior similar to that of FeSi in which the two energy gaps vanish at a critical pressure near the pressure at which T S vanishes, although the energy gaps in SmB 6 initially decrease with pressure, whereas in FeSi they increase with pressure. The MFMMS measurements showed a sharp feature at T S ≈ 19 K for FeSi, which could be due to ferromagnetic ordering of the CSS. However, no such feature was observed at T S ≈ 4.5 K for SmB 6 .

Funder

U.S. Department of Energy

National Science Foundation

Publisher

Proceedings of the National Academy of Sciences

Subject

Multidisciplinary

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