1972
DOI: 10.1103/physrevlett.29.920
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New Magnetic Phenomena in LiquidHe3below 3 mK

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Cited by 352 publications
(178 citation statements)
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“…This was actually the motivation for Pethick and Pines [17] to apply the t-matrix to the description of transport in heavy Fermion superconductors, since the experiments showed transport parameters vanishing at low T instead of staying constant below T c . It is quite amazing, that the T -dependence of Y (1) aa (T ) is close to the power laws T 3.5 in the B 1g -and T 1.5 in the B 2g -case, as predicted by Moreno and Coleman for the ultrasound attenuation [26]. In Fig.…”
Section: The Resonant Impurity Scattering Modelsupporting
confidence: 68%
See 1 more Smart Citation
“…This was actually the motivation for Pethick and Pines [17] to apply the t-matrix to the description of transport in heavy Fermion superconductors, since the experiments showed transport parameters vanishing at low T instead of staying constant below T c . It is quite amazing, that the T -dependence of Y (1) aa (T ) is close to the power laws T 3.5 in the B 1g -and T 1.5 in the B 2g -case, as predicted by Moreno and Coleman for the ultrasound attenuation [26]. In Fig.…”
Section: The Resonant Impurity Scattering Modelsupporting
confidence: 68%
“…During the last few decades a large variety of so-called unconventional superconductors have been discovered, among these the superfluid phases of 3 He [1][2][3][4], the heavy Fermion systems [5][6][7], the cuprates [8,9] and the Ruddlesden-Popper system Sr 2 RuO 4 [10]. The unconventional pairing correlations in these systems manifest themselves on the one hand in an anisotropy of the pair potential or energy gap of less symmetry than the underlying band structure or in the occurrence of additional spontaneously broken symmetries besides the U (1) gauge symmetry.…”
Section: Introductionmentioning
confidence: 99%
“…The relevance of ferromagnetic fluctuations [62], [63] for anisotropic BCS states was illustrated by the p wave superfluidity of liquid 3 He [64]. The p wave T C in nearly ferromagnetic metals was first calculated in 1971 [65] and in both FM and PM phases in 1980 [66].…”
Section: Methodsmentioning
confidence: 99%
“…Research on the subject then exploded following the unexpected discovery 8 in 1972 of this superfluid at temperatures below 0.003 K. At first, the observations were interpreted as spontaneous nuclear magnetic ordering in solid helium-3, but shortly afterwards, they were correctly identified as the transition to a superfluid 9 . Nuclear magnetic ordering in solid helium-3 was discovered 10 two years later at a temperature of 0.001 K.…”
Section: Years Agomentioning
confidence: 99%