Third sound, two-dimensional hydrodynamics, and elementary excitations in very thin helium films

1978 ◽  
Vol 18 (5) ◽  
pp. 2155-2168 ◽  
Author(s):  
J. E. Rutledge ◽  
W. L. McMillan ◽  
J. M. Mochel ◽  
T. E. Washburn
2002 ◽  
Vol 65 (16) ◽  
Author(s):  
J. Klier ◽  
A. Würl ◽  
P. Leiderer ◽  
G. Mistura ◽  
V. Shikin

1990 ◽  
Vol 04 (01) ◽  
pp. 47-51 ◽  
Author(s):  
J. SREEKUMAR ◽  
V. M. NANDAKUMARAN

Large amplitude local density fluctuations in a thin superfluid 4 He film is considered. It is shown that these large amplitude fluctuations travel and behave like "quasi-solitons" under collision, even when the full nonlinearity arising from the Van der Waals potential is taken into account.


1970 ◽  
Vol 3 (3) ◽  
pp. 225-234 ◽  
Author(s):  
I. Rudnick ◽  
J. C. Fraser

1980 ◽  
Vol 44 (4) ◽  
pp. 266-269 ◽  
Author(s):  
W. Thomlinson ◽  
J. A. Tarvin ◽  
L. Passell

From an experimental investigation of superfluid film transfer in narrow beakers in helium II it emerges that there are probably two kinds of film. A ‘normal’ film is formed by superfluid creep over a dry substrate. A ‘thick’ film remains when liquid has drained from a substrate that has previously been immersed in the liquid helium bath. A comparison has been made of the superfluid flow between the two types of film. Scatter of values of transfer rate associated with a normal film is attributed to third sound generated by bath waves impinging on the meniscus at the base of the film. The thick film shows an enhanced rate of transfer which can persist for long periods of time in quiet conditions, but which can be abruptly diminished by disturbances such as bath surface agitation. There is a maximum stable length for a thick film exhibiting the full enhanced rate. The enhanced rate can be as much as 60% greater than the normal rate at 1° K, but the difference between the two rates of transfer disappears above 1.8 °K. No enhanced rate of transfer at any temperature is observed in beakers as large as 8 mm diameter.


It is argued that the thermodynamic approach used by Goodstein and Saffman in their theory of thin superfluid helium films is incorrect. Their theory does not explain Keller’s experiment. The value they obtained for the convection velocity of third sound in a film with superfluid flow is consequently unfounded theoretically. Their calculation of third sound attenuation is shown to be incomplete.


2013 ◽  
Vol 15 (2) ◽  
pp. 025039 ◽  
Author(s):  
Michael Woerner ◽  
Wilhelm Kuehn ◽  
Pamela Bowlan ◽  
Klaus Reimann ◽  
Thomas Elsaesser

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