Closing the spin gap in the Kondo insulator Ce3Bi4Pt3 at high magnetic fields

Kondo insulator materials—such as CeRhAs, CeRhSb, YbB12, Ce3Bi4Pt3 and SmB6—are 3d, 4f and 5f intermetallic compounds that have attracted considerable interest in recent years. At high temperatures, they behave like metals. But as temperature is reduced, an energy gap opens in the conduction band at the Fermi energy and the materials become insulating. This contrasts with other f-electron compounds, which are metallic at all temperatures. The formation of the gap in Kondo insulators has been proposed to be a consequence of hybridization between the conduction band and the f-electron levels, giving a ‘spin’ gap. If this is indeed the case, metallic behaviour should be recovered when the gap is closed by changing external parameters, such as magnetic field or pressure. Some experimental evidence suggests that the gap can be closed in SmB6 (refs 5, 8) and YbB12 (ref. 9). Here we present specific-heat measurements of Ce3Bi4Pt3 in d.c. and pulsed magnetic fields up to 60 tesla. Numerical results and the analysis of our data using the Coqblin–Schrieffer model demonstrate unambiguously a field-induced insulator-to-metal transition.

[1]  K. Schotte,et al.  Interpretation of Kondo experiments in a magnetic field , 1975 .

[2]  V. T. Rajan Magnetic Susceptibility and Specific Heat of the Coqblin-Schrieffer Model , 1983 .

[3]  A. Passner,et al.  Studies of the Kondo insulator Ce3Bi4Pt3 in 61 T pulsed magnetic fields , 1995 .

[4]  H. Kumigashira,et al.  Spectral Evidence for Pseudogap Formation in Kondo Insulators CeRhAs and CeRhSb , 1999 .

[5]  T. Kasuya,et al.  Field-Induced Metallic State in YbB12 under High Magnetic Field , 1988 .

[6]  D. Rickel,et al.  High Field Gap Closure in the Kondo Insulator SmB6 , 1999 .

[7]  A. Fujimori,et al.  Temperature-Dependent High-Resolution Photoemission Study of the Kondo Insulator YbB12 , 1999 .

[8]  Alex C. Hewson,et al.  The Kondo Problem to Heavy Fermions , 1993 .

[9]  A. Hewson,et al.  The Kondo Problem to Heavy Fermions: Addendum , 1993 .

[10]  T. Kasuya,et al.  Specific heat measurements of YbB12 and YbxLu1−xB12 , 1988 .

[11]  Schlottmann Impurity bands in Kondo insulators. , 1992, Physical Review B (Condensed Matter).

[12]  R. Howard,et al.  Heat Capacity Measurements on Small Samples at Low Temperatures , 1972 .

[13]  Fisk,et al.  Low-temperature thermal expansion of SmB6: Evidence for a single energy scale in the thermodynamics of Kondo insulators. , 1994, Physical review. B, Condensed matter.

[14]  L. Degiorgi The electrodynamic response of heavy-electron compounds , 1999 .

[15]  T. Takabatake,et al.  Metallic ground state of CeNiSn , 1999 .

[16]  Fisk,et al.  Hybridization gap in Ce3Bi4Pt3. , 1990, Physical review. B, Condensed matter.

[17]  E. V. Bogdanov,et al.  SmB6 at high pressures: The transition from insulating to the metallic Kondo lattice , 1985 .

[18]  Z. Fisk,et al.  Magnetoresistance of the Kondo insulator Ce3Bi4Pt3 , 1993 .

[19]  Z. Fisk,et al.  Thermodynamics and Transport in Ce3Bi4Pt3 and Related Materials , 1993 .

[20]  Fisk,et al.  209Bi NMR and NQR investigation of the small-gap semiconductor Ce3Bi4Pt3. , 1994, Physical review. B, Condensed matter.

[21]  Fisk,et al.  Gap in the magnetic excitation spectrum of Ce3Bi4Pt3. , 1991, Physical review. B, Condensed matter.

[22]  Z. Fisk,et al.  Evidence for a ‘coherence’ gap in Ce3Bi4Pt3 , 1991 .