Abstract
The superfluid density of liquid4He is computed from vortex renormalization theories for the case of a slab geometry with a slab height L. With increasing temperature there is a crossover from three dimensions to two as the size of the largest vortex rings approaches L and they intersect with the walls, forming vortex pairs. The superfluid density becomes anisotropic, with the component parallel to the slab undergoing the universal Kosterlitz-Thouless jump, while the perpendicular component remains finite. The results are in agreement with both finite-size scaling and Monte-Carlo simulations.
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References
V. Ambegaokar, B. Halperin, D. Nelson, and E. Siggia,Phys. Rev. B 21, 1806 (1980).
J. Kosterlitz and D. Thouless,J. Phys. C 6, 1181 (1973).
W. Janke and K. Nather,Phys.Rev. B 48, 15807 (1993).
T. Schneider and A. Schmidt,J. Phys. Soc. Jpn. 61, 2169 (1992); N. Schultka and E. Manousakis,Phys.Rev, B 51, 11712 (1995).
D. Nelson and J.M. Kosterlitz,Phys. Rev. Lett. 39, 1201 (1977).
I. Rhee, F. Gasparini, and D. Bishop,Phys. Rev. Lett. 63, 410 (1989).
J. Nissen, T. Chui, and J. Lipa,J. Low Temp. Phys. 92, 353 (1993).
G. A. Williams,Phys. Rev. Lett. 59, 1926 (1987).
S. R. Shenoy,Phys.Rev. B 40, 5056 (1989).
G. A. Williams,J. Low Temp. Phys. 93, 1079 (1993).
G. A. Williams,J. Low Temp. Phys., this volume (to be published).
F. Gallet and G.A. Williams,Phys. Rev: B 39, 4673 (1989).
V. Kotsubo and G.A. Williams,Phys. Rev. B 33, 6106 (1986).
G. A. Williams,J. Low Temp. Phys. 89, 91 (1992).