Superconducting and Magnetic Transitions in the Heavy-Fermion System U<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Ru</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">Si</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msub></mml:mrow></mml:math>

T. M. Palstra, T.; Menovsky, A.A.; van den Berg, Jaap; Dirkmaat, A.J.; H. Kes, P.; Nieuwenhuys, G.J.; A. Mydosh, J.

doi:10.1103/physrevlett.55.2727

Public

Superconducting and Magnetic Transitions in the Heavy-Fermion System URu2Si2

Published in Physical Review Letters • Dec 9, 1985

Authors:

T. T. M. Palstra

A.A. Menovsky

Jaap van den Berg

Abstract

The intermetallic compound U${\mathrm{Ru}}_{2}$${\mathrm{Si}}_{2}$ can be classified as a heavy-fermion system because of its large linear specific-heat coefficient $\ensuremath{\gamma}=180$ mJ/mol\ifmmode\cdot\else\textperiodcentered\fi{}${\mathrm{K}}^{2}$. Susceptibility, magnetization, and specif...

Subject

Intermetallic

Superconductivity

Condensed matter physics

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