Disorder and the Superfluid Transition in Liquid<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>
Moses H. W. ChanThe Laboratory of Atomic and Solid State Physics, and the Materials Science Center, Cornell University, Ithaca, New York 14853K. I. BlumThe Laboratory of Atomic and Solid State Physics, and the Materials Science Center, Cornell University, Ithaca, New York 14853Sheena MurphyThe Laboratory of Atomic and Solid State Physics, and the Materials Science Center, Cornell University, Ithaca, New York 14853Gane Ka‐Shu WongThe Laboratory of Atomic and Solid State Physics, and the Materials Science Center, Cornell University, Ithaca, New York 14853J. D. ReppyThe Laboratory of Atomic and Solid State Physics, and the Materials Science Center, Cornell University, Ithaca, New York 14853
1988lv
ABI
Аннотация
The influence of quenched disorder on the critical behavior of superfluid $^{4}\mathrm{He}$ is studied by confinement of the helium to the pores of three different porous media: Vycor, xerogel, and aerogel glasses. In each case a well defined power-law behavior for the superfluid density is observed as the transition temperature is approached. In Vycor the superfluid critical exponent is bulklike, whereas strikingly different critical exponents are seen in the other two media.
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