We have computed the one-body density matrix rho(1) in solid He-4 at T=0 K using the shadow wave-function (SWF) variational technique. The accuracy of the SWF has been tested with an exact projector method. We find that off-diagonal long-range order is present in rho(1) for a perfect hcp and bcc solid He-4 for a range of densities above the melting one, at least up to 54 bars. This is first microscopic indication that Bose Einstein condensation (BEC) is present in perfect solid He-4. At melting, the condensate fraction in the hcp solid is 5x10(-6) and it decreases by increasing the density. The key process giving rise to BEC is the formation of vacancy interstitial pairs. We also present values for Leggett's upper bound on the superfluid fraction deduced from the exact local density.
Bose-Einstein condensation in solid He-4 / D.E. Galli, M. Rossi, L. Reatto. - In: PHYSICAL REVIEW. B, CONDENSED MATTER AND MATERIALS PHYSICS. - ISSN 1098-0121. - 71:14(2005), p. 140506.140506(R).
Bose-Einstein condensation in solid He-4
D.E. GalliPrimo
;M. RossiSecondo
;L. ReattoUltimo
2005
Abstract
We have computed the one-body density matrix rho(1) in solid He-4 at T=0 K using the shadow wave-function (SWF) variational technique. The accuracy of the SWF has been tested with an exact projector method. We find that off-diagonal long-range order is present in rho(1) for a perfect hcp and bcc solid He-4 for a range of densities above the melting one, at least up to 54 bars. This is first microscopic indication that Bose Einstein condensation (BEC) is present in perfect solid He-4. At melting, the condensate fraction in the hcp solid is 5x10(-6) and it decreases by increasing the density. The key process giving rise to BEC is the formation of vacancy interstitial pairs. We also present values for Leggett's upper bound on the superfluid fraction deduced from the exact local density.Pubblicazioni consigliate
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