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Physical Review

Theory of Superfluidity

F.W. Cummings, James R. Johnston

Published Dec 5, 1967• 1 citation
Publisher
DOI
10.1103/physrev.164.270

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The modern theory of Bose-Einstein condensation, superfluidity, and superconductivity is reviewed. The thermodynamic principle for superfluid flow and the equation of motion for condensed bosons are given. Computer simulations of Lennard-Jones 4^44He give the λλλ-transition and the superfluid viscosity. The statistical mechanical theory of high-temperature superconductivity is presented. Critical comparison is made with older approaches, such as ground energy state condensation, irrotational superfluid flow, and the macroscopic wavefunction.
In a Galilean superfluid, the depletion of superfluid density with rising temperature can be attributed to thermally excited non-interacting phonons. For systems without Galilean symmetry, it has been shown [1] that ``phonon wind" is no longer responsible for the depletion of superfluid density. In this work, we develop the theory of superfluid density at low temperature (TTT) and provide detailed derivations of all results announced in [1]. Using Popov's hydrodynamic action, we show that the theory of low-temperature depletion in a ddd-dimensional quantum superfluid maps onto the problem of finite-size (LLL) corrections in a (d+1)(d+1)(d+1)-dimensional anisotropic (pseudo-)classical-field system with U(1)-symmetric complex-valued action. In addition to generalizing Landau's (canonical) formula, we develop the grand canonical theory, which in a broader context reveals a universal scaling, Td+1T^{d+1}Td+1 and 1/Ld+11/L^{d+1}1/Ld+1, for finite-TTT and finite-LLL effects of many thermodynamic quantities. We validate our theory with numeric simulations of interacting lattice bosons and the J-current model.