Effect of magnetic fields on the Kondo insulator CeRhSb: magnetoresistance and high-field heat capacity measurements

Malik, S. K. ; Menon, Latika ; Pecharsky, V. K. ; Gschneidner, K. A. (1997) Effect of magnetic fields on the Kondo insulator CeRhSb: magnetoresistance and high-field heat capacity measurements Physical Review B, 55 (17). pp. 11471-11475. ISSN 0163-1829

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Official URL: http://prb.aps.org/abstract/PRB/v55/i17/p11471_1

Related URL: http://dx.doi.org/10.1103/PhysRevB.55.11471

Abstract

The compound CeRhSb is a mixed valent Ce-based compound which shows a gap in the electronic density of states at low temperatures. The gap manifests by a rise in electrical resistivity-below about 8 K from which the gap energy is estimated to be about 4 K. We have carried out heat capacity measurements on this compound in various applied fields up to 9.85 T. The magnetic contribution to the heat capacity, ΔC, is found to have a maximum in ΔC/T vs T at 10 K, below which ΔC/T is linear with T. This is attributed to the fact that below this temperature, in the gapped state, the electronic density of states decreases linearly with decreasing temperature. On application of a magnetic field, the electronic specific heat coefficient γ in the gapped state increases by ~4 mJ/mol K2. The maximum in ΔC/T vs T is observed in all fields, which shifts to lower temperatures ~1 K at 5.32 T and raises again at 9.85 T to about the same values as at H=0 T. This suggests that the gap exists for all fields up to 9.85 T. Above 10 K, in the mixed-valent state, ΔC/T vs T decreases with increasing temperature in zero field. There is hardly any effect of application of field in the mixed-valent state, since the applied fields are too small to change the already large density of states at the Fermi level. We have also carried out magnetoresistance measurements on CeRhSb up to fields of 5.5 T at 2, 4.5, 10, 20, and 30 K. The magnetoresistance in CeRhSb is positive at temperatures of 4.5 K and above, in applied fields up to 5.5 T. At 5.5 T, the magnetoresistance is maximum at 4.5 K (6%) and decreases with increasing temperature. The observation of the maximum is consistent with the observation of a maximum in ΔC/T vs T and is due to a change in the density of states. At a temperature of 2 K, a negative magnetoresistance is observed for magnetic fields greater than ~3.5 T which suggests reduction in the gap.

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