The gapped state in Kondo semiconductors CeNiSn and CeRhSb has been investigated by measurements of nuclear-spin laftice relaxation rate, 1/T~ of ll9Sn and 1235b and Knight shift of 1195n and 12~Sb. The T-dependences of T 1 and the shift in both compounds have revealed a novel feature for the gap st
High-field magnetism of Kondo semiconductors CeNiSn and CeRhSb
β Scribed by K. Sugiyama; T. Inoue; K. Oda; T. Takabatake; H. Tanaka; H. Fujii; K. Kindo; M. Date
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 213 KB
- Volume
- 211
- Category
- Article
- ISSN
- 0921-4526
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β¦ Synopsis
The longitudinal magnetoresistance of the Kondo semiconductor single crystals CeNiSn and CeRhSb are i~vestigated up to 36T below 4.2 K. Large negative magnetoresistances are found at low temperatures with the field along the b-and c-axis, similar to the field direction along the a-axis in the previous study.
The equiatomic ternary compounds CeNiSn and CeRhSb show a small band gap of the order of 10 K at low temperatures and they are ranked as the Ce-based Kondo insulators [1,2]. Both compounds crystallize in an orthorhombic structure which is closely related to the e-TiNiSi-type structure. The electrical and magnetic properties of CeNiSn are highly anisotropic as expected from the low crystal symmetry. The magnetic easy axis is the a-axis and the amount of the magnetization along the a-axis is large compared with those along the other two axes [3]. The gap energy of CeNiSn is also anisotropic and is estimated from the electrical resistivity p as 2.4, 5.5 and 5.0 K along the a-, b-and c-axes, respectively [1].
The large negative magnetoresistance of CeNiSn up to 15 T with the field along the a-axis reveals that the energy gap is quenched around 15T, and the magnetization along the a-axis up to 36 T shows a broad metamagnetic magnetization around 15 T [3]. However, small negative magnetoresistances are found with the field along the
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We review the methods of studying the spin-lattice and magnetization relaxation at high magnetic fields taking as an example the results obtained for semimagnetic semiconductors. The role of phonons which cannot be described by the Debye approximation is shown. The different relaxation paths are dis