1977
DOI: 10.1088/0022-3719/10/16/018
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Small objects in superfluid 3He

Abstract: Distortions in the superfluid order parameter around a small object in 3He are calculated, together with the supercurrents and the angular momentum induced by it in the liquid. The forces acting on the impurity due to the liquid texture structure are also considered.

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Cited by 98 publications
(51 citation statements)
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“…The transport cross section is reasonably approximated in the normal state by the geometric cross section err 2, and from the Einstein relation we find Op2/kBT = 3~2/p20"tr ~ 3.n'/(pvR) 2 (17) Typically pFR = 10 and thus Dp 2/kB T ~ 0.1. The constancy of the resulting mobility e/tz ~-n3pF~R 2, agrees well with experiment down to To.…”
Section: Equation For the Mobilitymentioning
confidence: 59%
“…The transport cross section is reasonably approximated in the normal state by the geometric cross section err 2, and from the Einstein relation we find Op2/kBT = 3~2/p20"tr ~ 3.n'/(pvR) 2 (17) Typically pFR = 10 and thus Dp 2/kB T ~ 0.1. The constancy of the resulting mobility e/tz ~-n3pF~R 2, agrees well with experiment down to To.…”
Section: Equation For the Mobilitymentioning
confidence: 59%
“…This was analyzed quasiclassically by Choi and Muzikar (1989a), based on an earlier work of Rainer and Vuorio (1977), who considered the inhuence of small scattering centers on superfluid He [another treatment of the problem was offered by Mineev (1989)]. We shall here consider the Ginzburg-Landau approach to this problem, which is only valid in the region of a slow variation of the order parameter.…”
Section: The Magnetic Effect Of Impurities or Lattice Defectsmentioning
confidence: 99%
“…The classical correlation function then leads to the following additional contribution to the homogeneous kernel in Eq. (4.11) (see Rainer and Vuorio, 1977): where do(r, r')/dQ is the differential cross section [o(r)= f dQ'der(r, r')/dQ]. This formula contains both the scattering (first cross-section term) and the shadow scattering (second cross-section term).…”
Section: The Magnetic Effect Of Impurities or Lattice Defectsmentioning
confidence: 99%
“…Moreover, since for a given value of the maximum gap A the A-phase gap is smaller, on the average, than in the B phase, one finds that both/Zlf and tz• are less than/ZB, the B-phase ion mobility at the same value of A/T. In order to compare the constant-cross-section calculation with experiment, let us evaluate the mobility increase in the superfluid near Tc using (23) and (24). Within weak coupling theory one has AZ(T) = 5 2 ~ABcs(T), where A(T) is the maximum gap in the ABM state.…”
Section: Ion Mobility Tensormentioning
confidence: 99%