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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 3169-3176 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Direct measurements have been made on the average single-particle kinetic energies, 〈Ek〉, of a series of solid and liquid specimens of heavy noble gases near melting. To do this, the distributions of energy losses of incident eV neutrons, scattered at angles ranging from 87 to 136 deg, were analyzed on the assumptions that atoms in these specimens have a Gaussian momentum distribution n(p) and that for these experimental conditions the atoms scatter independently of one another. It is known that the solids, Ar, Kr, and Xe show considerable differences in such characteristics as (a) their respective ratios of triple point to Debye temperatures, (b) the extent of multibody force contributions to cohesion, and (c) phonon anharmonicity. Regardless, it is found for all three solids near their respective triple points that 〈Ek〉 is equal to the equipartition value (3/2)kT well within the various estimated experimental uncertainties of 3% to 7%. Moreover, liquid Kr near its triple point yields the same result, as does liquid Xe at temperature up to 1.8 times its triple point temperature. Because all these systems are expected to be classical at these temperatures, these results demonstrate applicability of this neutron recoil method to determine 〈Ek〉 even of heavy atoms in suitable cases where a value may not be known in advance.
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 110 (1999), S. 1650-1661 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Neutron Compton profiles were measured of atomic momentum distributions in solid hexafluoroethane (C2F6) at saturated vapor pressure from 20 to 170 K, and of the liquid phase at 180 K. There are conflicting reports in the literature, from different kinds of measurements, about the nature and extent of solid phases of C2F6. Present neutron diffraction and thermal analysis shows that there is a clear crystallographic transformation near 103 K from a higher-temperature body-centered-cubic (bcc) phase which has considerable orientational disorder to a lower-temperature phase of different symmetry, which has relatively little disorder. The C and F atomic momentum profiles are found to have only small dependencies upon temperature and upon condensed phase. They are analyzed in terms of a dominant contribution from intramolecular vibrations plus contributions from translational and rotational motions of molecules. The nature of rotational contributions is of special interest, because of questions about the extent of static versus dynamic disorder in this kind of crystal. Brief comparisons to related solids such as SF6 are made. © 1999 American Institute of Physics.
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  • 3
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: A versatile system, operating at pressures to 300 MPa and temperatures to 4 K, has been designed and used for a variety of elastic and inelastic x-ray scattering studies of single crystals of condensed gases. Sintered Be sample cells of volumes 15–30 mm3 are used. Pressure generation is clean and well controlled. Excellent temperature control allows monitoring of phase transitions associated with solidification and melting. The system has very low background and, combined with the high-intensity of synchrotron radiation, is well suited to studies of low-intensity signals. It has been used for 4He in q-dependent studies of fcc lattice dynamics and diffuse scattering and to study thermal defect properties through lattice parameter measurements. In addition, its application to inelastic scattering studies of hcp 4He at 1.5 eV and 10 meV resolution have yielded results about electronic and phonon excitations, respectively. The system can also be used to study other crystalline compounds; in particular, an application has been made to lattice parameter measurements on C2F6. © 1996 American Institute of Physics.
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  • 4
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Inelastic x-ray scattering spectroscopy measurements on hcp single crystal solid He with q(parallel)c axis and q=0.45, 0.97, and 1.24 a.u. are presented. The crystals were grown in situ under a pressure of 600 bar at 5–7 K within a Be hollow cylinder. By subtracting a measurement on the empty Be cylinder, pure solid He spectra are obtained and discussed in terms both of the hcp He band structure and of excitonic excitation. The existence of an exciton at 21.8 eV above the 1s core level could unambiguously be settled. Clear evidence is found that the bottom of the conduction band is at 27 eV. © 1995 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    Chester : International Union of Crystallography (IUCr)
    Journal of synchrotron radiation 3 (1996), S. 316-317 
    ISSN: 1600-5775
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: Recently, the suitability of inelastic X-ray scattering for the investigation of solid and fluid 4He has been demonstrated. For the test experiments an energy resolution of the order of 10–15 meV was used at the backscattering spectrometer INELAX at the storage ring DORIS of DESY, Hamburg. Lattice excitations were observed for momentum transfers along the c axis of h.c.p. helium crystals which were grown in situ at pressures of 54–63 MPa and at temperatures of 4.2–6.4 K. At 10 K above the melting point, energy-loss signals could also be detected from the liquid helium at equivalent momentum transfers.
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 68 (1987), S. 125-146 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Phase separation temperatures have been determined in bcc3He-4He mixtures as a function of3He concentration and melting pressure from measurements of changes in the X-ray lattice parameter and Bragg peak shape. A new rigid tail dilution refrigerator cryostat was used to study3He-4He crystals with3He concentrations of 0.10, 0.20, 0.30, 0.45, 0.60, and 0.70 and melting pressures between 3.0 and 4.3 MPa. The phase separation temperatures determined are in good agreement with regular solution theory and give little support for an asymmetry in the coexistence curve expected from a Nosanow-type model and reported from previous experiments using other signatures of phase separation. At a given concentration, differences in phase separation temperatures determined from slow cooling and warming data, respectively, are as much as 25 mdeg, but this is less than half the differences reported from previous experiments. A bcc-hcp transformation was seen in a crystal with 10%3He at aboutT=0.3 K for a melting pressure of3.7 MPa.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 67 (1987), S. 353-375 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract X-ray lattice parameters of bcc4He crystals in contact with superfluid4He were measured with 300 ppm accuracy in the temperature range 1.494–1.711 K, corresponding to solid molar volumes between 20.88 and 21.09 cm3. Thermal vacancy concentrations in the solid at melting were estimated from a comparison of these lattice parameters with bulk solid molar volumes from the literature. Independently, temperature-dependent x-ray lattice parameter measurements on a bcc sample, held at constant macroscopic volume from 1.700 to 1.735 K, were referenced to the same solid sample (at 20.90 cm3) in the hcp phase near 0.8 K, where thermal vacancy content is small. The value of the free energy of formation for vacancies in bcc4He obtained from these measurements isf=9±1 K. The relationship between this value and indirect inferences about vacancy formation from ion mobility and NMR experiments is discussed. Comparisons are made between vacancy properties in bcc4He and in the more extensively studied bcc phase of3He. There are many parallels between the two systems. But a puzzling apparent difference between the vacancy relaxation energies in the two solids is pointed out.
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  • 8
    Publication Date: 1958-01-15
    Print ISSN: 0031-899X
    Electronic ISSN: 1536-6065
    Topics: Physics
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  • 9
    Publication Date: 1958-02-15
    Print ISSN: 0031-899X
    Electronic ISSN: 1536-6065
    Topics: Physics
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  • 10
    Publication Date: 1962-02-01
    Print ISSN: 0031-899X
    Electronic ISSN: 1536-6065
    Topics: Physics
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