Low Temperature Physics-Lt 13 1974
DOI: 10.1007/978-1-4684-7864-8_131
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Peculiarities of Charged Particle Motion in 3He–4He Solutions in Strong Electric Fields

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“…The best fits of obtained diffusion by equation ( 2) with a variable prefactor η using bulk liquid densities and gap gives its values of η 1 = (2.65 ± 0.05) × 10 −6 cm 2 s −1 , η 2 = (2.30 ± 0.05) × 10 −6 cm 2 s −1 and η ⊥ 2 = (1.95 ± 0.05) × 10 −6 cm 2 s −1 instead of 3.3 × 10 −6 cm 2 s −1 in bulk (dashed, dotted and dash-dotted lines in figure 1, respectively). The reduced prefactor η indicates on the changes either of roton properties or a normal liquid density ρ n as 3 He-roton scattering cross-section σ * ir is expected to be nearly constant in this range of temperatures [36]. It should be noted that attempts to add a simple constant offset to bulk roton gap poorly fit the aerogel data and are not shown here.…”
Section: Aerogel Datamentioning
confidence: 91%
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“…The best fits of obtained diffusion by equation ( 2) with a variable prefactor η using bulk liquid densities and gap gives its values of η 1 = (2.65 ± 0.05) × 10 −6 cm 2 s −1 , η 2 = (2.30 ± 0.05) × 10 −6 cm 2 s −1 and η ⊥ 2 = (1.95 ± 0.05) × 10 −6 cm 2 s −1 instead of 3.3 × 10 −6 cm 2 s −1 in bulk (dashed, dotted and dash-dotted lines in figure 1, respectively). The reduced prefactor η indicates on the changes either of roton properties or a normal liquid density ρ n as 3 He-roton scattering cross-section σ * ir is expected to be nearly constant in this range of temperatures [36]. It should be noted that attempts to add a simple constant offset to bulk roton gap poorly fit the aerogel data and are not shown here.…”
Section: Aerogel Datamentioning
confidence: 91%
“…where Δ bulk = 8.68 − 0.0084 × T 7 [K] is the empirical equation for the roton gap in bulk helium [40] and the prefactor [36] in bulk is η = 3.3 × 10 −6 cm 2 s −1 . The density of the normal component in bulk mixtures ρ n for a given 3 He concentration x 3 could be found elsewhere [36].…”
Section: Bulk Datamentioning
confidence: 99%
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