2008
DOI: 10.1103/physrevlett.100.017004
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Field-Angle-Dependent Specific Heat Measurements and Gap Determination of a Heavy Fermion SuperconductorURu2Si2

Abstract: To identify the superconducting gap structure in URu2Si2, we perform field-angle-dependent specific heat measurements for the two principal orientations in addition to field rotations, and a theoretical analysis based on microscopic calculations. The Sommerfeld coefficient gamma(H)'s in the mixed state exhibit a distinctly different field dependence. This comes from point nodes and the substantial Pauli paramagnetic effect of URu2Si2. These two features combined give rise to a consistent picture of superconduc… Show more

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Cited by 75 publications
(78 citation statements)
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“…We have provided examples that involve first-order antiferromagnetic transitions, first-order valence transitions as well as the enigmatic case of URu 2 Si 2 . Here, d-wave superconductivity with broken time-reversal symmetry occurs near an antiferromagnetic quantum phase transition at nonzero pressure, 122,123 raising the possibility for the relevance of antiferromagnetic order to superconductivity. However, T c appears to diminish on approach to the antiferromagnetic order, and is nonzero only in the presence of the hidden order (cf.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…We have provided examples that involve first-order antiferromagnetic transitions, first-order valence transitions as well as the enigmatic case of URu 2 Si 2 . Here, d-wave superconductivity with broken time-reversal symmetry occurs near an antiferromagnetic quantum phase transition at nonzero pressure, 122,123 raising the possibility for the relevance of antiferromagnetic order to superconductivity. However, T c appears to diminish on approach to the antiferromagnetic order, and is nonzero only in the presence of the hidden order (cf.…”
Section: Discussionmentioning
confidence: 99%
“…120 The "weak" antiferromagnetic order, which seems to occur within the hidden order phase, is most likely due to static antiferromagnetically ordered regions that exist in a small part of the sample, phase separated from the surrounding hidden order region. 121 Thus, d-wave superconductivity 122,123 seems to microscopically coexist with the hidden order but not with antiferromagnetism. 121 …”
mentioning
confidence: 99%
“…Only out of the HO state evolves a highly unconventional (d-wave, even parity, spin-singlet) multi-gap superconducting ground state with T c ≈ 1.5 K Matsuda et al, 1996), being the focus of recent investigations (Kasahara et al, 2007(Kasahara et al, , 2009Morales and Escudero, 2009;Okazaki et al, 2008;Yano et al, 2008). Now the question arises: Is the HO phase generic, i.e., can it, as defined above, be found in other materials with different types of interactions?…”
Section: What Is Hidden Ordermentioning
confidence: 99%
“…Such investigations were pioneered by Amitsuka and Sakakibara (1994) and spanned a decade of experimentation (Yokoyama et al, 2002). The important questions posed here are: Can dilute U in a non-magnetic matrix support a single-impurity Kondo effect or even a multichannel Kondo behavior (Cox, 1987)?…”
Section: High Magnetic Fields and Rh-dopingmentioning
confidence: 99%
“…From these behaviors, we can estimate the strength of the paramagnetic effect, µ. The H-dependence of γ(H) for H � c and H � ab was used to identify the pairing symmetry and paramagnetic effect in URu 2 Si 2 (Yano et al, 2008).…”
Section: Field Dependence Of Paramagnetic Susceptibility and Zero-enementioning
confidence: 99%