Competing interactions in the heavy-electron antiferromagnets Ce<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="italic">M</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Sn</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>(<i>M</i>=Ni, Ir, Cu, Rh, Pd, and Pt)

P. Beyermann, W.; F. Hundley, M.; C. Canfield, P.; D. Thompson, J.; Latroche, M.; Godart, C.; Selsane, M.; Fisk, Z.; L. Smith, J.

doi:10.1103/physrevb.43.13130

Public

Competing interactions in the heavy-electron antiferromagnets CeM2Sn2(M=Ni, Ir, Cu, Rh, Pd, and Pt)

Published in Physical review. B, Condensed matter • Jun 1, 1991

Authors:

W. P. Beyermann

M. F. Hundley

P. C. Canfield

Abstract

Specific-heat, magnetic-susceptibility, and resistivity measurements on annealed polycrystalline samples of Ce${\mathit{M}}_{2}$${\mathrm{Sn}}_{2}$, with M=Ni, Ir, Cu, Rh, Pd, and Pt, indicate that each of these compounds orders antiferromagnetically at N\'eel temperatures ${\mathit{T}}_{\mathit{N}}...

Subject

Physics

Kondo effect

Specific heat

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