2019
DOI: 10.48550/arxiv.1908.01645
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Topological nodal line in superfluid $^3$He and the Anderson theorem

Abstract: We have found an experimental evidence for the existence of the Dirac nodal line in the quasiparticle spectrum of the polar phase of superfluid 3 He. The polar phase is stabilized by confinement of 3 He between nm-sized cylinders. The temperature dependence of the gap, measured via frequency shift in the NMR spectrum, follows expected ∝ T 3 dependence. The results support the Fomin extension of the Anderson theorem to the polar phase with columnar defects: perfect columnar non-magnetic defects do no perturb th… Show more

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Cited by 16 publications
(21 citation statements)
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References 25 publications
(34 reference statements)
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“…The reason for the appearance of the polar phase in nafen is the analog of the Anderson theorem applied for the polar phase in the presence of the columnar defects (nafen strands), see Refs. [15,16]. While for all the other phases of superfluid 3 He the transition temperature is suppressed by these impurities.…”
Section: жэтфmentioning
confidence: 95%
“…The reason for the appearance of the polar phase in nafen is the analog of the Anderson theorem applied for the polar phase in the presence of the columnar defects (nafen strands), see Refs. [15,16]. While for all the other phases of superfluid 3 He the transition temperature is suppressed by these impurities.…”
Section: жэтфmentioning
confidence: 95%
“…Orbital anisotropy vector m is locked along the nafen strands, while the node line in the energy spectrum develops in the plane perpendicular to the strands. Owing to the extension of the Anderson theorem [30][31][32], these features are robust against disorder, introduced by the nafen strands.…”
Section: Vortices In the Polar Phasementioning
confidence: 99%
“…It has been found recently that the celebrated Anderson theorem [1], which implies that the bulk properties of an s-wave paired superfluid phase are insensitive to the impurity strength, is satisfied in the p-wave polar superfluid phase [2,3] of liquid 3 He realized in highly anisotropic aerogels with a structure consisting of columnar defects [4][5][6]. Consequently, the normal to polar superfluid transition there has no quantum critical point (QCP), and the polar phase is stabilized as the high-temperature superfluid phase.…”
Section: Introductionmentioning
confidence: 99%