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2009
DOI: 10.1063/1.3075937
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Viscosity and relaxation processes in the phonon-roton system of He II

Abstract: The viscosity of He4 in the temperature range 0.1–2.2K has been measured using a vibrating quartz tuning fork. A quantitative comparison is made of the experimental data and the conclusions of the modern theory of the phonon-roton system of superfluid helium. The complex hierarchy of relaxation processes is analyzed and the role and contribution of each process to the coefficient of viscosity are determined. Agreement between the experiments and theory is obtained in the hydrodynamic region. The transition fro… Show more

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Cited by 20 publications
(35 citation statements)
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“…However, it has been observed experimentally that for 4 He at very low temperature ballistic phonons can still efficiently damp the movement of immersed objects, see Refs. [47][48][49]. This damping can still be described by an effective or ballistic shear viscosity coefficient defined by ball 1 5 ph c s d; (2.18) where d is the typical size of the oscillating object, and is a coefficient that measures the probability that the phonons are diffused at the boundary with the object.…”
Section: B Shear Viscosity Due To Phonons In Superfluid Neutrons Stamentioning
confidence: 99%
“…However, it has been observed experimentally that for 4 He at very low temperature ballistic phonons can still efficiently damp the movement of immersed objects, see Refs. [47][48][49]. This damping can still be described by an effective or ballistic shear viscosity coefficient defined by ball 1 5 ph c s d; (2.18) where d is the typical size of the oscillating object, and is a coefficient that measures the probability that the phonons are diffused at the boundary with the object.…”
Section: B Shear Viscosity Due To Phonons In Superfluid Neutrons Stamentioning
confidence: 99%
“…However in this temperature region, there is a considerable contribution to the viscosity coefficient from phonon-roton interactions and it is necessary to take these processes into account. The deviation of the experimental points [24,25] from the theoretical curve at temperatures higher 0.7 K is due exactly to ignoring these phonon-roton interactions. In the intermediate temperature range (from 0.5 to 0.9 K) the contributions of three-phonon and four-phonon relaxation have the same order of magnitude and both processes should be taken into account for calculating the first viscosity coefficient.…”
Section: Calculation Of the Contribution Of Small And Large Angle Scamentioning
confidence: 88%
“…We note, that for the A quantities the following relations are valid ; curve 3 is a numerical calculation of the relaxation time from Eq. (59) without the contribution of small angles between p 1 and p 2 (i.e., the lower limit of integration over angles is equal to 30°); experimental points from Greywall [24] are marked by triangles, the squares show the experimental data from Zadorozhko et al [25].…”
Section: Calculation Of the Contribution Of Small And Large Angle Scamentioning
confidence: 99%
“…There are cases, however, when small-angle collisions may dominate, as it may turn out to be more efficient to achieve a large-angle collision by the addition of many small-angle scatterings. In the low T regime of superfluid 4 He where the viscosity is dominated by phonons, the 4-ph large-angle collisions give the leading contribution to the shear viscosity only in a restricted range of temperature [42], while 3-ph small-angle processes dominate for any temperature below 0.7 K [16].…”
Section: Shear Viscosity Due To Small-angle Collisionsmentioning
confidence: 99%