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  • PhysRevLett.94.165301

    Rights statement: © 2005 The American Physical Society

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Superfluid Interfaces in Quantum Solids

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Superfluid Interfaces in Quantum Solids. / Burovski, Evgeni; Kozik, Evgeny; Kuklov, Anatoly et al.
In: Physical review letters, Vol. 94, No. 16, 165301, 28.04.2005.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

Burovski, E, Kozik, E, Kuklov, A, Prokof'ev, N & Svistunov, B 2005, 'Superfluid Interfaces in Quantum Solids', Physical review letters, vol. 94, no. 16, 165301. https://doi.org/10.1103/PhysRevLett.94.165301

APA

Burovski, E., Kozik, E., Kuklov, A., Prokof'ev, N., & Svistunov, B. (2005). Superfluid Interfaces in Quantum Solids. Physical review letters, 94(16), Article 165301. https://doi.org/10.1103/PhysRevLett.94.165301

Vancouver

Burovski E, Kozik E, Kuklov A, Prokof'ev N, Svistunov B. Superfluid Interfaces in Quantum Solids. Physical review letters. 2005 Apr 28;94(16):165301. doi: 10.1103/PhysRevLett.94.165301

Author

Burovski, Evgeni ; Kozik, Evgeny ; Kuklov, Anatoly et al. / Superfluid Interfaces in Quantum Solids. In: Physical review letters. 2005 ; Vol. 94, No. 16.

Bibtex

@article{62eb24eefd3d44ba827b7505fffdf3fe,
title = "Superfluid Interfaces in Quantum Solids",
abstract = "One scenario for the nonclassical moment of inertia of solid 4He discovered by Kim and Chan [ Nature (London) 427 225 (2004)] is the superfluidity of microcrystallite interfaces. On the basis of the most simple model of a quantum crystal—the checkerboard lattice solid—we show that the superfluidity of interfaces between solid domains can exist in a wide range of parameters. At strong enough interparticle interaction, a superfluid interface becomes an insulator via a quantum phase transition. Under the conditions of particle-hole symmetry, the transition is of the standard U(1) universality class in 3D, while in 2D the onset of superfluidity is accompanied by the interface roughening, driven by fractionally charged topological excitations.",
author = "Evgeni Burovski and Evgeny Kozik and Anatoly Kuklov and Nikolay Prokof'ev and Boris Svistunov",
note = "{\textcopyright} 2005 The American Physical Society",
year = "2005",
month = apr,
day = "28",
doi = "10.1103/PhysRevLett.94.165301",
language = "English",
volume = "94",
journal = "Physical review letters",
issn = "1079-7114",
publisher = "American Physical Society",
number = "16",

}

RIS

TY - JOUR

T1 - Superfluid Interfaces in Quantum Solids

AU - Burovski, Evgeni

AU - Kozik, Evgeny

AU - Kuklov, Anatoly

AU - Prokof'ev, Nikolay

AU - Svistunov, Boris

N1 - © 2005 The American Physical Society

PY - 2005/4/28

Y1 - 2005/4/28

N2 - One scenario for the nonclassical moment of inertia of solid 4He discovered by Kim and Chan [ Nature (London) 427 225 (2004)] is the superfluidity of microcrystallite interfaces. On the basis of the most simple model of a quantum crystal—the checkerboard lattice solid—we show that the superfluidity of interfaces between solid domains can exist in a wide range of parameters. At strong enough interparticle interaction, a superfluid interface becomes an insulator via a quantum phase transition. Under the conditions of particle-hole symmetry, the transition is of the standard U(1) universality class in 3D, while in 2D the onset of superfluidity is accompanied by the interface roughening, driven by fractionally charged topological excitations.

AB - One scenario for the nonclassical moment of inertia of solid 4He discovered by Kim and Chan [ Nature (London) 427 225 (2004)] is the superfluidity of microcrystallite interfaces. On the basis of the most simple model of a quantum crystal—the checkerboard lattice solid—we show that the superfluidity of interfaces between solid domains can exist in a wide range of parameters. At strong enough interparticle interaction, a superfluid interface becomes an insulator via a quantum phase transition. Under the conditions of particle-hole symmetry, the transition is of the standard U(1) universality class in 3D, while in 2D the onset of superfluidity is accompanied by the interface roughening, driven by fractionally charged topological excitations.

U2 - 10.1103/PhysRevLett.94.165301

DO - 10.1103/PhysRevLett.94.165301

M3 - Journal article

VL - 94

JO - Physical review letters

JF - Physical review letters

SN - 1079-7114

IS - 16

M1 - 165301

ER -