Electrical transport, heat capacity, and high-field magnetization study in intermetallic Ni2CeSn compound
J. Appl. Phys. 103, 07B915 (2008); doi:10.1063/1.2837885
Published 11 March 2008
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Magnetization, heat capacity, and electrical resistivity measurements were performed on a Ni2CeSn compound (orthorhombic structure) in the temperature range of 2–300 K. This compound is paramagnetic down to 6 K. At higher temperatures above T=150 K, the magnetic susceptibility obeys Curie–Weiss behavior yielding an effective magnetic moment µeff=2.56µB/f.u., which is very close to that of the free Ce3+ ion (2.54µB) with a high negative Curie–Weiss temperature,
CW=−170 K. As the temperature is decreased, the magnetic moment decreases gradually to 0.43µB/f.u. at 4.2 K. We also infer that, based on the high field (up to 23 T) magnetization and the magnetic susceptibility data, a crystal-field splitting of cerium atoms becomes significant at temperatures below 150 K. We used heat capacity and resistivity measurements to determine the crystal-field splitting of the Ce3+ magnetic sublevels. It is found that the ground magnetic state for the Ce3+ is a doublet of Jz=±1/2 states, with a first excited quartet of Jz=±3/2 and Jz=±5/2 states separated by ~107 K. The resistivity exhibits a shallow minimum at about 11 K, which may be due to the development of partial magnetic order based on these crystal-field-split states.
©2008 American Institute of Physics
CW=−170 K. As the temperature is decreased, the magnetic moment decreases gradually to 0.43µB/f.u. at 4.2 K. We also infer that, based on the high field (up to 23 T) magnetization and the magnetic susceptibility data, a crystal-field splitting of cerium atoms becomes significant at temperatures below 150 K. We used heat capacity and resistivity measurements to determine the crystal-field splitting of the Ce3+ magnetic sublevels. It is found that the ground magnetic state for the Ce3+ is a doublet of Jz=±1/2 states, with a first excited quartet of Jz=±3/2 and Jz=±5/2 states separated by ~107 K. The resistivity exhibits a shallow minimum at about 11 K, which may be due to the development of partial magnetic order based on these crystal-field-split states.
©2008 American Institute of Physics
| History: | Presented 7 November 2007; received 14 August 2007; accepted 16 November 2007; published 11 March 2008 |
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http://link.aip.org/link/?JAPIAU/103/07B915/1 |
KEYWORDS and PACS
cerium alloys,
crystal field interactions,
electrical resistivity,
ground states,
magnetic moments,
magnetic susceptibility,
magnetisation,
nickel alloys,
paramagnetic materials,
specific heat,
tin alloys
- 75.20.En
Diamagnetism and paramagnetism in metals and alloys - 72.15.Eb
Electrical and thermal conduction in crystalline metals and alloys - 75.40.Cx
Static properties of magnetic materials - 75.60.Ej
Magnetization curves, hysteresis, Barkhausen and related effects - 75.30.Cr
Saturation moments and magnetic susceptibilities in magnetically ordered materials - 71.70.Ch
Crystal and ligand fields - YEAR: 2008
RELATED DATABASES
PUBLICATION DATA
0021-8979 (print)
1089-7550 (online)
REFERENCES (4)
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- B. Chevalier, J. Garcia Soldavilla, J. I. Espeso, J. Rodriguez Fernández, J. C. Gómez Sal, and J. Etourneau,
Physica B 259-261, 44 (1999) . - V. V. Gridin, S. A. Sergeenov, A. M. Strydom, and P. de V. du Plessis, Phys. Rev. B 50, 12995 (1994).
- M. E. Huntelaar, A. S. Booij, E. H. P. Cordfunke, R. R. van der Laan, A. C. G. van Genderen, and J. C. van Miltenburg,
J. Chem. Thermodyn. 32, 465 (2000) . - Y. Öner, O. Kamer, E. Alveroglu, M. Acet, and T. Krenke,
J. Alloys Compd. 429, 64 (2007) .







