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

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 SmB6 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 TS = 19 K of the CSS is similar to that of SmB6. 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 TS. Several studies of ρ(T) under pressure on SmB6 reveal behavior similar to that of FeSi in which the two energy gaps vanish at a critical pressure near the pressure at which TS vanishes, although the energy gaps in SmB6 initially decrease with pressure, whereas in FeSi they increase with pressure. The MFMMS measurements showed a sharp feature at TS ≈ 19 K for FeSi, which could be due to ferromagnetic ordering of the CSS. However, no such feature was observed at TS ≈ 4.5 K for SmB6.

[1]  A. Seitsonen,et al.  Atomistic investigation of surface characteristics and electronic features at high-purity FeSi(110) presenting interfacial metallicity , 2021, Proceedings of the National Academy of Sciences.

[2]  E. Maggio,et al.  Resistivity saturation in Kondo insulators , 2020, Communications Physics.

[3]  Z. Fisk,et al.  Bulk and Surface Properties of SmB6 , 2020, Rare-Earth Borides.

[4]  Z. Fisk,et al.  Hall-coefficient diagnostics of the surface state in pressurized SmB6 , 2019, Physical Review B.

[5]  T. McQueen,et al.  Dynamical Bonding Driving Mixed Valency in a Metal Boride. , 2019, Angewandte Chemie.

[6]  J. Jeffries,et al.  Pressure-driven valence increase and metallization in the Kondo insulator Ce3Bi4Pt3 , 2019, Physical Review B.

[7]  Z. Fisk,et al.  Transport gap in SmB6 protected against disorder , 2019, Proceedings of the National Academy of Sciences.

[8]  Seokmin Hong,et al.  Electrical detection of the surface spin polarization of the candidate topological Kondo insulator SmB6 , 2018, Physical Review B.

[9]  Z. Fisk,et al.  Quantum Oscillations in Flux-Grown SmB_{6} with Embedded Aluminum. , 2018, Physical review letters.

[10]  Y. Meng,et al.  Evidence for a conducting surface ground state in high-quality single crystalline FeSi , 2018, Proceedings of the National Academy of Sciences.

[11]  E. Weschke,et al.  Samarium hexaboride is a trivial surface conductor , 2015, Nature Communications.

[12]  P. Smet,et al.  Samarium Monosulfide (SmS): Reviewing Properties and Applications , 2017, Materials.

[13]  Z. Fisk,et al.  Quantum phase transition and destruction of Kondo effect in pressurized SmB6. , 2016, Science bulletin.

[14]  X. H. Chen,et al.  Magnetoresistance evidence of a surface state and a field-dependent insulating state in the Kondo insulatorSmB6 , 2015 .

[15]  I. Schuller,et al.  Magnetic field modulated microwave spectroscopy across phase transitions and the search for new superconductors , 2014, Reports on progress in physics. Physical Society.

[16]  Z. Fisk,et al.  Two-dimensional Fermi surfaces in Kondo insulator SmB6 , 2013, Science.

[17]  Z. Fisk,et al.  Topological surface state in the Kondo insulator samarium hexaboride. , 2013, Nature materials.

[18]  Z. Fisk,et al.  Surface Hall Effect and Nonlocal Transport in SmB6: Evidence for Surface Conduction , 2013, Scientific Reports.

[19]  V. Prakapenka,et al.  Phase relations in the Fe-FeSi system at high pressures and temperatures , 2013 .

[20]  Yoichi Ando,et al.  Topological Insulator Materials , 2013, 1304.5693.

[21]  Z. Fisk,et al.  Low-temperature surface conduction in the Kondo insulator SmB6 , 2012, 1211.5104.

[22]  E. Reich Hopes surface for exotic insulator , 2012, Nature.

[23]  R. Greene,et al.  Hybridization, Correlation, and In-Gap States in the Kondo Insulator SmB6 , 2012 .

[24]  G. Kotliar,et al.  Signatures of electronic correlations in iron silicide , 2011, Proceedings of the National Academy of Sciences.

[25]  V. Galitski,et al.  Topological Kondo insulators. , 2009, Physical review letters.

[26]  T. Oguchi,et al.  Angle-resolved photoemission study of the strongly correlated semiconductor FeSi , 2008 .

[27]  S. Parkin,et al.  Handbook of magnetism and advanced magnetic materials , 2007 .

[28]  P. Coleman Heavy Fermions: Electrons at the Edge of Magnetism , 2006, cond-mat/0612006.

[29]  T. Togashi,et al.  Ultraviolet laser photoemission spectroscopy of FeSi: Observation of a gap opening in density of states , 2005 .

[30]  Y. Paderno,et al.  Pressure-induced Fermi-liquid behavior in the Kondo insulator SmB 6 : Possible transition through a quantum critical point , 2003 .

[31]  Ott,et al.  Kondo insulators , 2002 .

[32]  P. Riseborough Heavy fermion semiconductors , 2000 .

[33]  John L. Sarrao,et al.  Low-temperature transport, thermodynamic, and optical properties of FeSi , 1997 .

[34]  K. Breuer,et al.  OBSERVATION OF A GAP OPENING IN FESI WITH PHOTOELECTRON SPECTROSCOPY , 1997 .

[35]  G. Aeppli,et al.  Metal-Insulator Transitions in the Kondo Insulator FeSi and Classic Semiconductors Are Similar , 1997 .

[36]  E. Bauer,et al.  Stoichiometric effects on the optical spectra and pressure response of Fe1−xMnxSi , 1997 .

[37]  A. Damascelli,et al.  Infrared spectroscopic study of phonons coupled to charge excitations in FeSi , 1996, cond-mat/9612045.

[38]  Z. Fisk,et al.  Studies of the correlated electron system SmB6 , 1996 .

[39]  Fisk,et al.  SmB6: Kondo insulator or exotic metal? , 1995, Physical review letters.

[40]  Fisk,et al.  Thermodynamics of FeSi. , 1995, Physical review. B, Condensed matter.

[41]  Fu,et al.  Model for a strongly correlated insulator: FeSi. , 1994, Physical review. B, Condensed matter.

[42]  Jones,et al.  Magnetic, transport, and structural properties of Fe1-xIrxSi. , 1994, Physical review. B, Condensed matter.

[43]  Zhang,et al.  Unconventional charge gap formation in FeSi. , 1993, Physical review letters.

[44]  G. Meisner,et al.  UFe4P12 and CeFe4P12: Nonmetallic isotypes of superconducting LaFe4P12 , 1985 .

[45]  T. Kasuya,et al.  A new and typical valence fluctuating system, YbB12 , 1983 .

[46]  Z. Fisk,et al.  Suppression of the energy gap in SmB6 under pressure , 1983 .

[47]  N. Mott Rare-earth compounds with mixed valencies , 1974 .

[48]  M. Maple,et al.  Demagnetization of Rare Earth Ions in Metals Due to Valence Fluctuations , 1974 .

[49]  M. Maple,et al.  Nonmagnetic 4 f Shell in the High-Pressure Phase of SmS , 1971 .

[50]  E. Buehler,et al.  MAGNETIC AND SEMICONDUCTING PROPERTIES OF SmB . , 1969 .

[51]  L. Walker,et al.  Paramagnetic Excited State of FeSi , 1967 .

[52]  Hiroshi Watanabe,et al.  Neutron Diffraction Study of the Intermetallic Compound FeSi , 1963 .