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  • 1995-1999  (9)
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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 113 (1998), S. 987-992 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We have measured the solubility of 4 He in liquid 3 He down to about 40 mK and at pressures from zero up to ∼ 24 atm. The solubility was obtained from the thickness of the superfluid film in contact with unsaturated solutions of 4 He in 3 He as a function of temperature. By fitting the solubility data to Fermi liquid theory, we obtained the parameters m 4 * and Δ as a function of pressure. Here, m 4 * is the effective mass of 4 He in liquid 3 He and Δ the difference in binding energy between 4 He in pure 4 He and 4 He in liquid 3He. This difference has a minimum near 10 atm. The average of the results for m 4 * , at different pressures, is (1.3 ± 0.2)m 4. This agrees with the many body calculations of de Saavedra et al., and with the Stokes hydrodynamic mass using the partial volume of 4 He in 3 He, v 4 * . The partial volume was obtained by taking the derivative of Δ with respect to pressure.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 116 (1999), S. 99-132 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We describe a simulation of the scattering in beams of helium atoms. The number of atoms N in the beams is reduced by a large scaling factor λ while the collision cross-section is increased by λ. This leaves the rate of scattering for each particle unchanged. As an example, we predict the outcome of a low temperature atomic beam experiment to measure the 4 He- 4 He atomic scattering cross-section σ at low energies. Because of the existence of a very weakly bound dimer, the low energy cross-section is expected to be unusually large, ∼1.83 × 10 5 Å 2 . In the simulation N/λ is small enough for the trajectories of all the scaled atoms to be calculated numerically. The simulation shows that the experiment is quite practicable. The proposed apparatus is just over 20 cm long, and a few centimeters wide, small enough to fit in a dilution refrigerator. The heaters and bolometers are assumed to be similar to those used in previous low temperature scattering experiments. We show that, using low intensity beams, the cross-section can be measured as a function of the relative velocity v r between ∼2 and ∼8 m/sec, corresponding to relative energies between ∼1 and ∼16 mK. By fitting σ(v r) one can determine the scattering length and effective range of the interaction. We predict that, at high intensity where multiple scattering is very important, the two beams coalesce into one.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 101 (1995), S. 167-175 
    ISSN: 1573-7357
    Keywords: 67.60.Dm ; 51.10.+y ; 67.55.Lf ; 67.55.Hc
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The diffusion coefficient D and the thermal diffusion factor γT, for4He in liquid3He at low temperatures T, have recently been calculated by solving the Boltzmann equation derived from Fermi-liquid theory. As T → 0, γT approaches a constant and D varies as 1/T. Both transport coefficients are determined solely by a 0 34 , the l = 0 forward scattering amplitude. Because a 0 34 can be found from thermodynamic data, e.g. the solubility of4He in liquid3He, X 4 sat , a strict test of the theory is possible. We have built an apparatus to measure D and X 4 sat as functions of pressure and temperature. The ratio of the capacitances of two parallel plate capacitors measures the number of4He atoms diffusing out of the liquid into the superfluid film. A bellows initiates the diffusion by changing the pressure in the liquid and thus the equilibrium concentration. A change of ∼ 10−8 in the4He concentration can be detected.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 101 (1995), S. 1023-1035 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We show that conventional kinetic theory, based on Fermi liquid theory, disagrees with the recent measurements by Greenwood et al. of the thermomechanical effect in normal liquid3He. The theory predicts that, in the Knudsen or long-free-path regime, dP/dT across a porous plug should be 1/3 of the entropy per unit volume ps. Experimentally, the ratio decreases from ∼4 to ∼1 between 2 mK and 20 mK. The theoretical result does not depend on whether the quasiparticles exchange energy with the walls or whether the scattering is partly specular. We consider possible reasons for the discrepancy between theory and experiment. One alternative approach, which treats the3He in the porous plug as a mesoscopic system, gives the same result as conventional kinetic theory. The relation between the thermomechanical effect in3He and thermoelectricity in metals is also discussed.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 104 (1996), S. 317-338 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Using a heater and bolometer as source and detector, the reflection of a pulsed beam of phonons at the free surface of liquid4He at ∼ 0.05 K has been measured for angles of incidence between 30 ° and 80 °. The energy distribution of the incident beam was obtained from the theory of phonon decay in the accompanying paper (I). The average incident phonon energy was ∼ 0.3 K, corresponding to an effective beam temperature of about 0.1 K. Both heater and bolometer were made from graphite resistor board with a layer of poly aniline fibers to increase the absorptivity for rotons. The angular distribution of the phonons from the heater is quite broad, approximately (cosn π+cosm θ)/2 with n ≈ 0.65 and m ≈ 3.4. However, the receiver response has a broad component with n ≈ 2.2 and an extraordinarily narrow one with m ≈ 106. In agreement with the theory in I, the reflection appears to be specular within the accuracy of the experiment. The reflection coefficient is unity within the experimental error; the weighted mean value is 1.001±0.025. During the experiment, the free surface became contaminated with ∼ 0.034 of a monolayer of3He, but no effect from the3He impurity was observed.
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 104 (1996), S. 295-316 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The scattering of a low energy phonon at the free surface of liquid4He at finite temperature is discussed in relation to the reflection measurements in the accompanying paper (II). If not specularly reflected, the phonon may be inelastically scattered, with the emission or absorption of a single ripplon, or it may be absorbed with the emission of two ripplons. The inelastic scattering produces deviations from ideal specular reflection that depend logarithmically on the angular sensitivity of the measurement. For the experiment described in II, the predicted deviations due to scattering and absorption are roughly equal and too small (∼5×10−4) to be measured. In addition, there should be a small broadening (less than 1 ° in angle) of the reflected image of the phonon source due to phonon decay in the bulk liquid. This was calculated from the curvature of the phonon spectrum measured by Rugar and Foster. Phonon decay also determines the distribution of the incident phonon beam with respect to energy. From the known decay rate, the average incident phonon energy in our experiment is calculated to be ∼0.5 K. We also discuss the attenuation of surface second sound due to the inelastic scattering and absorption of thermal phonons at the surface. We find that two ripplon absorption is the dominant effect. Below ∼0.7 K, the attenuation due to phonons is probably just small enough for pure ripplon surface sound to exist in a narrow range of low frequencies. To show this, we have recalculated the ripplon lifetime using the 3-ripplon interaction as recently revised by Rocheet al. The results for the ripplon lifetime are displayed in a simple scaling format.
    Type of Medium: Electronic Resource
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  • 7
    Publication Date: 1995-02-06
    Print ISSN: 0031-9007
    Electronic ISSN: 1079-7114
    Topics: Physics
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  • 8
    Publication Date: 1997-05-01
    Print ISSN: 1063-777X
    Electronic ISSN: 1090-6517
    Topics: Physics
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  • 9
    Publication Date: 1998-04-13
    Print ISSN: 0031-9007
    Electronic ISSN: 1079-7114
    Topics: Physics
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