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Titlebook: Quantum Statistics and the Many-Body Problem; Samuel B. Trickey,Wiley P. Kirk,James W. Dufty Book 1975 Plenum Press, New York 1975 dispers

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樓主: Retina
51#
發(fā)表于 2025-3-30 11:30:38 | 只看該作者
52#
發(fā)表于 2025-3-30 16:17:18 | 只看該作者
53#
發(fā)表于 2025-3-30 16:40:26 | 只看該作者
Spin Waves and Magnetization Oscillation in Superfluid 3He,s, though extremely small, will lift partially the high degeneracy of the ground state. The dipole interaction introduces correlations between the orbital and the spin configuration of the condensate, giving rise to an additional shift in the NMR frequencies for example.
54#
發(fā)表于 2025-3-30 23:12:28 | 只看該作者
55#
發(fā)表于 2025-3-31 02:27:10 | 只看該作者
Thermal Boundary Resistance Between Solid 3He and Cerium Magnesium Nitrate,. At temperatures below 70 mK and fields greater than ~55G, the observed measurements of the magnetic Kapitza resistance are consistent with the T. dependence of that resistance predicted by R. A. Guyer. for the solid He and the T dependence for the liquid observed by others at lower temperatures. and theoretically predicted..
56#
發(fā)表于 2025-3-31 06:50:26 | 只看該作者
57#
發(fā)表于 2025-3-31 09:18:10 | 只看該作者
58#
發(fā)表于 2025-3-31 14:59:38 | 只看該作者
Sound Propagation in Normal and Superfluid 3He,rfluid zero sound regime of 3He. The velocity and attenuation were studied at a frequency of 20.24 MHz and at pressures of 17.00, 21.00, 21.50, 21.80, 22.00, 23.17, 26.00, and 28.00 bar in the zero sound regime. In the hydrodynamic region the temperature dependence of the attenuation was studied at
59#
發(fā)表于 2025-3-31 21:18:54 | 只看該作者
Phonon Propagation in Liquid and Solid Helium,escers and tunnel junctions as sources and detectors of high frequency phonons. In addition, a short discussion of recent observations of ballistic phonons in solid .He is given. Implications for specific heat measurements are discussed.
60#
發(fā)表于 2025-4-1 01:04:47 | 只看該作者
Thermal Boundary Resistance Between Solid 3He and Cerium Magnesium Nitrate, cm./mole, ~15ppm He4) and liquid He. (S.V.P.) at several different applied magnetic field strengths in the temperature range between 45 mK and 250 mK. At temperatures below 70 mK and fields greater than ~55G, the observed measurements of the magnetic Kapitza resistance are consistent with the T. de
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