Hidden magnetism and quantum criticality in the heavy fermion superconductor CeRhIn5

Tuson Park (), F. Ronning, H. Q. Yuan, M. B. Salamon, R. Movshovich, J. L. Sarrao and J. D. Thompson
Additional contact information
Tuson Park: Los Alamos National Laboratory
F. Ronning: Los Alamos National Laboratory
H. Q. Yuan: University of Illinois at Urbana-Champaign
M. B. Salamon: University of Illinois at Urbana-Champaign
R. Movshovich: Los Alamos National Laboratory
J. L. Sarrao: Los Alamos National Laboratory
J. D. Thompson: Los Alamos National Laboratory

Nature, 2006, vol. 440, issue 7080, 65-68

Abstract: Abstract With only a few exceptions that are well understood, conventional superconductivity does not coexist with long-range magnetic order (for example, ref. 1). Unconventional superconductivity, on the other hand, develops near a phase boundary separating magnetically ordered and magnetically disordered phases2,3. A maximum in the superconducting transition temperature Tc develops where this boundary extrapolates to zero Kelvin, suggesting that fluctuations associated with this magnetic quantum-critical point are essential for unconventional superconductivity4,5. Invariably, though, unconventional superconductivity masks the magnetic phase boundary when T

Date: 2006
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DOI: 10.1038/nature04571

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