Liquid helium at negative pressure

Czechoslovak Journal of Physics

Volumn 46, Issue SUPPL. 6, 1996, Pages 2943-2950

  Maris, Humphrey J ^a  

^a BROWN UNIVERSITY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 2342485975     PISSN: 00114626     EISSN: 15729486     Source Type: Journal    
DOI: 10.1007/BF02548095     Document Type: Review

References (40)

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5. This method has been used at finite temperatures by S. Hall and H.J. Maris (to be published).
6. H.J. Maris, Phys. Rev. Lett. 66, 45 (1991).
7. The plot shows estimates from refs. 5 and 6.
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11. When the phonons make the major contribution to the thermodynamics this calculation has to be performed using a self-consistent method. This is because the phonon part of the dispersion curve depends on the sound velocity, and the sound velocity in turn depends on the dispersion curve through Eq. 2.
12. I am grateful to E. Brezin for this suggestion. It is necessary to consider the extent to which the contribution from this type of excitation is independent of, and additive to, the contribution from the phonon excitations.
13. λ by this method it is necessary to allow for the temperature-dependence of the dispersion curve.
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29. Unpublished data of J. Classen.
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31. H. Lambaré, P. Roche, E. Rolley, S. Balibar, C. Guthmann, and H.J. Maris, this conference.
32. Note that it is necessary to apply a correction to the data to take account of the attenuation of the sound wave as it travels from the transducer to the focus. The attenuation has a maximum value at around 0.8 K. The data shown in Figs. 4 and 5 are not corrected for this effect. This is why the voltage required to produce cavitation at 0.75 K is greater than the voltage at 0.171 K.
33. P. Roche, H. Lambaré, E. Rolley, D. Lacoste, S. Balibar, C. Guthmann, and H.J. Maris, this conference.
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38. J. Classen, C.K. Su, and H.J. Maris, this conference.
39. J. Classen, C.K. Su, and H.J. Maris, to appear in Physical Review Letters.
40. The operation of helium bubble chambers has been considered by A.G. Tenner, Nucl. Inst. Methods. 22, 1 (1963).