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Phys. Rev. B 76, 064503 (2007) [10 pages]

Boson localization and excitations of liquid 4He confined in gelsil

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Francesco Albergamo1, Jacques Bossy2, Jonathan V. Pearce3,4, Helmut Schober3, and Henry R. Glyde4
1European Synchrotron Radiation Facility, Boîte Postale 220, F-38043 Grenoble Cedex, France
2Centre de Recherche sur les Très Basses Températures, CNRS, BP 166, 38042 Grenoble Cedex 9, France
3Institut Laue-Langevin, BP 156, 38042 Grenoble, France
4Department of Physics and Astronomy, University of Delaware, Newark, Delaware 19716-2570, USA

Received 20 December 2006; revised 17 May 2007; published 6 August 2007

We present neutron scattering measurements of the phonon-roton (P-R) modes of liquid 4He at saturated vapor pressure confined in 44 Å mean pore diameter gelsil in the wave vector range 0.4⩽Q⩽2.15 Å−1. Layer modes, modes which propagate in the liquid layers adjacent to the porous media walls, were also observed at wave vectors in the roton region (Q≃1.95 Å−1) but not at Q≲1.7 Å−1. The first goal is to document the filling dependence of the dynamic response and of the P-R mode energies and widths more systematically than has been done in the past. As the gelsil is filled with 4He, the P-R and layer modes are first observed at a fractional filling of f=76% at low temperature (T=0.4 K). At fillings f=76%, the P-R mode energies lie below the bulk superfluid 4He values in the wave vector range 0.4⩽Q⩽1.7 Å−1, especially at Q≃1.1 Å−1, as observed in helium films. As filling is increased, the intensity in the P-R mode increases markedly and the P-R mode energies move toward bulk superfluid values taking bulk values at full filling. The second goal is to determine the temperature dependence of the intensity in the P-R modes in a media in which the superfluid-normal transition temperature Tc=1.92 K is independently known and lies well below the bulk liquid value Tλ=2.17 K. As temperature is increased, the intensity in the P-R and layer modes decreases. However, a well-defined P-R mode is observed at temperatures up to T≃2.15 K, above Tc=1.92 K. Since well-defined modes exist because there is Bose-Einstein condensation (BEC), this suggests that there is BEC above Tc, probably localized. Localized BEC appears to exist up to TTλ.

© 2007 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.76.064503
DOI:
10.1103/PhysRevB.76.064503
PACS:
67.40.Db, 61.12.Ex