1986
DOI: 10.1007/bf01323427
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Superconductivity and magnetic order in a strongly interacting fermi-system: URu2Si2

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Cited by 514 publications
(282 citation statements)
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“…This is a consequence of multi-band superconductivity with compensated electronic structure in the hidden order state of this system. We provide strong evidence for a new type of unconventional superconductivity with two distinct gaps having different nodal topology.The heavy-Fermion compound URu 2 Si 2 has mystified researchers since the superconducting state (T c = 1.5 K) is embedded within the "hidden order" phase (T h = 17.5 K) [1,2,3]. Although several exotic order parameters have been proposed for the hidden order phase [4], it is not identified yet.…”
mentioning
confidence: 99%
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“…This is a consequence of multi-band superconductivity with compensated electronic structure in the hidden order state of this system. We provide strong evidence for a new type of unconventional superconductivity with two distinct gaps having different nodal topology.The heavy-Fermion compound URu 2 Si 2 has mystified researchers since the superconducting state (T c = 1.5 K) is embedded within the "hidden order" phase (T h = 17.5 K) [1,2,3]. Although several exotic order parameters have been proposed for the hidden order phase [4], it is not identified yet.…”
mentioning
confidence: 99%
“…The heavy-Fermion compound URu 2 Si 2 has mystified researchers since the superconducting state (T c = 1.5 K) is embedded within the "hidden order" phase (T h = 17.5 K) [1,2,3]. Although several exotic order parameters have been proposed for the hidden order phase [4], it is not identified yet.…”
mentioning
confidence: 99%
“…Although the microscopic order parameter has not yet been definitively established, a multitude of bulk property measurements indicate that a partial gapping of the Fermi surface is involved in the HO transition. In addition to the BCS-like specific heat anomaly, there are anomalies in the electrical resistivity, magnetic susceptibility [77][78][79], ultrasound [86], thermal expansion [87], and an increase in lattice thermal conductivity [88]. Additional evidence points to the opening of a large gap in the tunneling spectrum [89], the incommensurate spin excitation spectrum [90], and the crossing of the chemical potential by a heavy electron band [91].…”
Section: Uru 2 Simentioning
confidence: 99%
“…Both the magnetic susceptibility and electrical resistivity are anisotropic [78,79], and show characteristics typical of Kondo lattice materials. The magnetic susceptibility χ(T ) follows a Curie-Weiss law at high temperatures, reflecting a uranium free ion moment, but deviates from this behavior above 100 K and peaks at 50 K. At low temperatures, χ(T ) saturates to a value of χ 0 ≈ 0.005 cm 3 mol −1 .…”
Section: Uru 2 Simentioning
confidence: 99%
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