Annual Review of Condensed Matter Physics, volume 16, issue 1, pages 209-228

Transverse Quantum Superfluids

Anatoly Kuklov 1, 2
Lode Pollet 3, 4, 5
Nikolay Prokof'ev 6, 7
Boris Svistunov 6, 7
1
 
1Department of Physics and Astronomy, The College of Staten Island, and the Graduate Center, City University of New York, New York, NY, USA; email: Anatoly.Kuklov@csi.cuny.edu
2
 
1Department of Physics and Astronomy, The College of Staten Island, and the Graduate Center, City University of New York, New York, NY, USA; email: Anatoly.Kuklov@csi.cuny.edu
3
 
3Munich Center for Quantum Science and Technology (MCQST), München, Germany
5
 
2Arnold Sommerfeld Center for Theoretical Physics, Ludwig-Maximilians-Universität, München, Germany; email: Lode.Pollet@lmu.de
7
 
4Department of Physics, University of Massachusetts, Amherst, Massachusetts, USA; email: prokofev@physics.umass.edu, svistunov@physics.umass.edu
Publication typeJournal Article
Publication date2025-03-10
scimago Q1
SJR9.821
CiteScore47.4
Impact factor14.3
ISSN19475454, 19475462
Abstract

Even when ideal solids are insulating, their states with crystallographic defects may have superfluid properties. It became clear recently that edge dislocations in 4He featuring a combination of microscopic quantum roughness and superfluidity of their cores may represent a new paradigmatic class of quasi-one-dimensional superfluids. The new state of matter, termed transverse quantum fluid (TQF), is found in a variety of physical setups. The key ingredient defining the class of TQF systems is infinite compressibility, which is responsible for all other unusual properties such as the quadratic spectrum of normal modes (or even the absence of sharp quasiparticles), irrelevance of the Landau criterion, off-diagonal long-range order at T = 0, and the exponential dependence of the phase slip probability on the inverse flow velocity. From a conceptual point of view, the TQF state is a striking demonstration of the conditional character of many dogmas associated with superfluidity, including the necessity of elementary excitations, in general, and the ones obeying the Landau criterion in particular.

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