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0009257615
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PRPLCM 0370-1573 10.1016/0370-1573(94)90084-1
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R. Golub and S. K. Lamoreaux, Phys. Rep. PRPLCM 0370-1573 10.1016/0370-1573(94)90084-1 237, 1 (1994).
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Golub, R.1
Lamoreaux, S.K.2
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2
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84880811254
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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.
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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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4
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18444417104
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EULEEJ 0295-5075 10.1209/epl/i2002-00408-4
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S. K. Lamoreaux, G. Archibald, P. D. Barnes, W. T. Buttler, D. J. Clark, M. D. Cooper, M. Espy, G. L. Greene, R. Golub, M. E. Hayden, C. Lei, L. J. Marek, J.-C. Peng, and S. Penttila, Europhys. Lett. EULEEJ 0295-5075 10.1209/epl/i2002-00408-4 58, 718 (2002).
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Lamoreaux, S.K.1
Archibald, G.2
Barnes, P.D.3
Buttler, W.T.4
Clark, D.J.5
Cooper, M.D.6
Espy, M.7
Greene, G.L.8
Golub, R.9
Hayden, M.E.10
Lei, C.11
Marek, L.J.12
Peng, J.-C.13
Penttila, S.14
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7
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0009933613
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PHRVAO 0031-899X 10.1103/PhysRev.164.235
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G. Baym and C. Ebner, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.164.235 164, 235 (1967).
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Phys. Rev.
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Baym, G.1
Ebner, C.2
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8
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0000823496
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RMPHAT 0034-6861 10.1103/RevModPhys.49.341
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H. J. Maris, Rev. Mod. Phys. RMPHAT 0034-6861 10.1103/RevModPhys.49.341 49, 341 (1977).
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Maris, H.J.1
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10
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0036591829
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EULEEJ 0295-5075 10.1209/epl/i2002-00409-9
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R. M. Bowley, Europhys. Lett. EULEEJ 0295-5075 10.1209/epl/i2002-00409-9 58, 725 (2002).
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Europhys. Lett.
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Bowley, R.M.1
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11
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84880808178
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The phonon contributions to the dissipative second viscosity terms in the superfluid acceleration equation vanish, see Ref..
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The phonon contributions to the dissipative second viscosity terms in the superfluid acceleration equation vanish, see Ref..
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13
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0043063651
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Ref. 12, Chap. 25;
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I. M. Khalatnikov, Ref. 12, Chap. 25; I. M. Khalatnikov and V. N. Zharkov, Zh. E. T. F. 32, 1108 (1957)
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Zh. E. T. F.
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Khalatnikov, I.M.1
Khalatnikov, I.M.2
Zharkov, V.N.3
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17
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0037534732
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PHRVAO 0031-899X 10.1103/PhysRev.170.346
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G. Baym and C. Ebner, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.170.346 170, 346 (1968).
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Phys. Rev.
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Baym, G.1
Ebner, C.2
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18
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84880803842
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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.
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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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19
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84880778868
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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.
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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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20
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33646623554
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PYLAAG 0375-9601 10.1016/0375-9601(67)90693-7
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C. Boghosian and H. Meyer, Phys. Lett. A PYLAAG 0375-9601 10.1016/0375-9601(67)90693-7 25, 352 (1967).
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Boghosian, C.1
Meyer, H.2
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22
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0001133158
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PHRVAO 0031-899X 10.1103/PhysRev.188.309
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B. M. Abraham, C. G. Brandt, Y. Eckstein, J. Munarin, and G. Baym, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.188.309 188, 309 (1969).
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Abraham, B.M.1
Brandt, C.G.2
Eckstein, Y.3
Munarin, J.4
Baym, G.5
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23
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84880812285
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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.
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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.
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24
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5244319824
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PRBMDO 1098-0121 10.1103/PhysRevB.23.2152
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D. S. Greywall, Phys. Rev. B PRBMDO 1098-0121 10.1103/PhysRevB.23.2152 23, 2152 (1981).
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Greywall, D.S.1
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25
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84880795555
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PDE Solutions Inc., Spokane Valley, WA 99206, USA.
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PDE Solutions Inc., Spokane Valley, WA 99206, USA.
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26
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84880787668
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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.
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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.
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27
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84880798771
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We are grateful to M. Hayden, private communication, for the details of the geometry.
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We are grateful to M. Hayden, private communication, for the details of the geometry.
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28
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0000158092
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PHRVAO 0031-899X 10.1103/PhysRev.125.873
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C. B. Satterthwaite, Phys. Rev. PHRVAO 0031-899X 10.1103/PhysRev.125.873 125, 873 (1962);
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Satterthwaite, C.B.1
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29
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0017958625
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Superconducting aluminum heat switch and plated press-contacts for use at ultralow temperatures
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DOI 10.1063/1.1135452
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R. M. Mueller, C. Buchal, T. Oversluizen, and F. Pobell, Rev. Sci. Instrum. 10.1063/1.1135452 49, 515 (1978) (Pubitemid 8596408)
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Mueller, R.M.1
Buchal, C.2
Oversluizen, T.3
Pobell, F.4
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30
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84880797262
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and references therein.
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and references therein.
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