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Volumn 88, Issue 1, 2013, Pages

Transport in very dilute solutions of 3He in superfluid 4He

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EID: 84880793053     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.88.014512     Document Type: Article
Times cited : (11)

References (30)
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    • This experiment utilizes the absorption of ultracold polarized neutrons on polarized 3He atoms via the reaction n+3He→p+t+764 keV.
    • This experiment utilizes the absorption of ultracold polarized neutrons on polarized 3 He atoms via the reaction n + 3 He → p + t + 764 keV.
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    • The phonon contributions to the dissipative second viscosity terms in the superfluid acceleration equation vanish, see Ref..
    • The phonon contributions to the dissipative second viscosity terms in the superfluid acceleration equation vanish, see Ref..
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    • Note that in the implementation of this correction in Ref., the 3He effective mass is taken to be one third of its actual value, and therefore the effects of recoil are overestimated.
    • Note that in the implementation of this correction in Ref., the 3 He effective mass is taken to be one third of its actual value, and therefore the effects of recoil are overestimated.
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    • 3 becomes sufficiently small, the 3He no longer provides the mechanism for absorbing momentum from the phonons, and rather the phonon thermal conductivity becomes limited by viscous transfer of momentum from the phonons to the container walls.
    • 3 becomes sufficiently small, the 3 He no longer provides the mechanism for absorbing momentum from the phonons, and rather the phonon thermal conductivity becomes limited by viscous transfer of momentum from the phonons to the container walls.
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    • In fact, the viscosity for flow in a circular pipe plays a role only in a thin boundary layer, which for the concentrations and temperatures under consideration is of order millimeters thick.
    • In fact, the viscosity for flow in a circular pipe plays a role only in a thin boundary layer, which for the concentrations and temperatures under consideration is of order millimeters thick.
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    • PDE Solutions Inc., Spokane Valley, WA 99206, USA.
    • PDE Solutions Inc., Spokane Valley, WA 99206, USA.
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    • We note that the analysis here must be extended for the lower temperatures in the experiment to include scattering from the walls. For example, the phonon mean free path is larger than the diameter of the pipe for temperatures below about 0.37 K.
    • We note that the analysis here must be extended for the lower temperatures in the experiment to include scattering from the walls. For example, the phonon mean free path is larger than the diameter of the pipe for temperatures below about 0.37 K.
  • 27
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    • We are grateful to M. Hayden, private communication, for the details of the geometry.
    • We are grateful to M. Hayden, private communication, for the details of the geometry.
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    • and references therein.
    • and references therein.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.