Superfluid density of thin<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">He</mml:mi></mml:mrow><mml:mprescripts/><mml:mrow/><mml:mrow><mml:mn>4</mml:mn></mml:mrow><mml:mrow/><mml:mrow/></mml:mmultiscripts></mml:mrow></mml:math>films adsorbed in porous Vycor glass
D. J. BishopLaboratory of Atomic and Solid State Physics and The Materials Science Center, Cornell University Ithaca, New York 14853Jonathan BertholdLaboratory of Atomic and Solid State Physics and The Materials Science Center, Cornell University Ithaca, New York 14853J. M. ParpiaLaboratory of Atomic and Solid State Physics and The Materials Science Center, Cornell University Ithaca, New York 14853J. D. ReppyLaboratory of Atomic and Solid State Physics and The Materials Science Center, Cornell University Ithaca, New York 14853
1981lv
ABI
Annotatsiya
We have studied the superfluid density of thin superfluid $^{4}\mathrm{He}$ films absorbed in porous Vycor glass. At low temperatures we have used a third-sound technique to examine the Landau elementary excitations. We observed phonons with a ${T}^{2}$ temperature dependence and rotons with a 5-K energy gap. At higher temperatures we have examined the superfluid density in the critical region. The superfluid density follows a power law similar to that of bulk $^{4}\mathrm{He}$ with an exponent at the bulk value. We conclude that these effects are due to the three-dimensional geometry of the substrate.
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