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Zero-point motion and superfluid helium

Identifieur interne : 002A81 ( Main/Exploration ); précédent : 002A80; suivant : 002A82

Zero-point motion and superfluid helium

Auteurs : S. R. Shenoy [Inde] ; A. C. Biswas [Inde]

Source :

RBID : ISTEX:5B8F6B83659FD6808134B364A4CC18A0E26CE97B

English descriptors

Abstract

Abstract: We propose that He II exhibits macroscopic [σ P /N ∼O(1)] quantum zero-point motion in momentum space, i.e., that a nonzero root-mean-square superfluid velocity exists even in an equilibrium superfluid system at rest. At absolute zero, using coherent states, we relate the uncertainty σ P /N in the total momentumP (per particle) to the long-range-order (LRO) part of the phase gradient correlation function, which is proposed as an order parameter. The local equilibrium equation for the superfluid velocity potential derived by Biswas and Rama Rao yields, in the strict equilibrium limit, the equation determining this order parameter in terms of fluctuation correlations that remain to be determined. The order parameter is interaction dependent, nonzero atT=0 if $$\tilde \mu$$ (0)−ρ0V0>0, and can vanish at some transition temperatureT λ when fluctuation terms become comparable to theT=0 value. (HereV 0 ρ0, and $$\tilde \mu$$ (0) are the uniform parts of the potential, density, and chemical potential with shifted zero of energy, respectively.) A characteristic length Λ(T), diverging atT=T λ, appears naturally, with its defining relation reducing to a macroscopic uncertainty relation (σ P /N)Λ(0)=ħ/2 atT=0. With certain assumptions it is shown that atT=0, LRO in the phase gradient correlation function is incompatible with off-diagonal long-range order (ODLRO) in the 〈ω†(r′)ω(r)〉 correlation function, and with nonzero condensate function.

Url:
DOI: 10.1007/BF00668214


Affiliations:


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<term>Bose</term>
<term>Bose statistics</term>
<term>Certain approximation</term>
<term>Certain assumptions</term>
<term>Classical hydrodynamics</term>
<term>Coherent motion</term>
<term>Coherent states</term>
<term>Collective variables</term>
<term>Condensate</term>
<term>Condensate approach</term>
<term>Condensate fraction</term>
<term>Density matrix</term>
<term>Elementary excitation spectrum</term>
<term>Equilibrium superfluid system</term>
<term>Exact density matrix</term>
<term>Excitation</term>
<term>Extra term</term>
<term>First correlation function</term>
<term>Fluctuation</term>
<term>Fluctuation terms</term>
<term>Ground state</term>
<term>Hamiltonian</term>
<term>Hard core</term>
<term>Helium atom</term>
<term>Ideal bose</term>
<term>Invariance</term>
<term>Length scale</term>
<term>Liquid helium</term>
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<term>Transition temperature</term>
<term>Translational invariance</term>
<term>Uncertainty principle</term>
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<div type="abstract" xml:lang="en">Abstract: We propose that He II exhibits macroscopic [σ P /N ∼O(1)] quantum zero-point motion in momentum space, i.e., that a nonzero root-mean-square superfluid velocity exists even in an equilibrium superfluid system at rest. At absolute zero, using coherent states, we relate the uncertainty σ P /N in the total momentumP (per particle) to the long-range-order (LRO) part of the phase gradient correlation function, which is proposed as an order parameter. The local equilibrium equation for the superfluid velocity potential derived by Biswas and Rama Rao yields, in the strict equilibrium limit, the equation determining this order parameter in terms of fluctuation correlations that remain to be determined. The order parameter is interaction dependent, nonzero atT=0 if $$\tilde \mu$$ (0)−ρ0V0>0, and can vanish at some transition temperatureT λ when fluctuation terms become comparable to theT=0 value. (HereV 0 ρ0, and $$\tilde \mu$$ (0) are the uniform parts of the potential, density, and chemical potential with shifted zero of energy, respectively.) A characteristic length Λ(T), diverging atT=T λ, appears naturally, with its defining relation reducing to a macroscopic uncertainty relation (σ P /N)Λ(0)=ħ/2 atT=0. With certain assumptions it is shown that atT=0, LRO in the phase gradient correlation function is incompatible with off-diagonal long-range order (ODLRO) in the 〈ω†(r′)ω(r)〉 correlation function, and with nonzero condensate function.</div>
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