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  • 1
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Physica C: Superconductivity and its applications 235-240 (1994), S. 1623-1624 
    ISSN: 0921-4534
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Physics
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Physica B: Physics of Condensed Matter 194-196 (1994), S. 409-410 
    ISSN: 0921-4526
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Physics
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Physica B: Physics of Condensed Matter 194-196 (1994), S. 521-522 
    ISSN: 0921-4526
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Physics
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Physica B: Physics of Condensed Matter 194-196 (1994), S. 521-522 
    ISSN: 0921-4526
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Physics
    Type of Medium: Electronic Resource
    Location Call Number Expected Availability
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  • 5
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Physica B: Physics of Condensed Matter 194-196 (1994), S. 409-410 
    ISSN: 0921-4526
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Physics
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Copenhagen : International Union of Crystallography (IUCr)
    Applied crystallography online 29 (1996), S. 285-290 
    ISSN: 1600-5767
    Source: Crystallography Journals Online : IUCR Backfile Archive 1948-2001
    Topics: Geosciences , Physics
    Notes: A Monte Carlo algorithm for the analysis of powder diffraction patterns is presented. One aim of this algorithm, which can be used as a supplement to the regular Rietveld refinement, is to provide a self-consistent determination of the thermal displacements of the atoms. This is achieved by modelling the total scattered intensity, comprising both the Bragg peak intensity and the diffuse contribution to the spectrum from the scattering density of an assembly of atoms. This assembly, which is constructed by the reverse Monte Carlo technique so as to yield a best fit with the data, is then used to calculate the average atomic thermal displacements. This allows for a refinement that, in principle, no longer requires angle-dependent background parameters, and that is well suited for dealing with highly anisotropic Debye–Waller factors and split atomic sites.
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  • 7
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 109 (1997), S. 577-623 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We determine the behavior of the phonon excitations in liquid 4He, covering both the normal and superfluid phase, for a range of temperatures T (1 〈 T 〈 4.2 K), wave numbers q (0.1 〈 q 〈 2.2 Å−1) and pressures p (0 〈 p 〈 25 bars), by means of a numerical fitting procedure based on the effective eigenmode description of the density correlation function. We find that the q, p and T dependence of all inelastic neutron scattering data can be well described by using only one adjustable parameter, the damping rate of the momentum fluctuations. We establish that there is a close similarity between classical liquids, normal-fluid 4He and superfluid 4He. We observe, for all q-values, a marked change in the damping rate of the momentum fluctuations as one passes through the superfluid-transition temperature Tλ. For the roton excitations, this results in a heavily damped (overdamped at p = 20 bars) mode in the normal phase, in contrast to the propagating mode observed in the superfluid phase. The change in damping rate is found to occur predominantly in a small temperature region just below Tλ, for all q-values. We do not find any evidence for the sudden appearance of the predicted “renormalized single-particle” excitations as one enters the superfluid phase. We argue that the full dispersion curve of the phonon-maxon-roton excitations can be understood for all temperatures and pressures in terms of the damping rate of the momentum fluctuations, whereas the rapid changes in this damping rate near Tλ can be viewed as a direct consequence of the Bose symmetry requirements on the 4He-wavefunction.
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  • 8
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 109 (1997), S. 577-623 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We determine the behavior of the phonon excitations in liquid4He, covering both the normal and superfluid phase, for a range of temperatures T (1〈T〈4.2 K), wave numbers q (0.1〈q〈2.2 Å−1) and pressures p (0〈p〈25 bars), by means of a numerical fitting procedure based on the effective eigenmode description of the density correlation function. We find that the q, p and T dependence of all inelastic neutron scattering data can be well described by using only one adjustable parameter, the damping rate of the momentum fluctuations. We establish that there is a close similarity between classical liquids, normal-fluid4He and superfluid4He. We observe, for all q-values, a marked change in the damping rate of the momentum fluctuations as one passes through the superfluid-transition temperature Tλ. For the roton excitations, this results in a heavily damped (overdamped at p=20 bars) mode in the normal phase, in contrast to the propagating mode observed in the superfluid phase. The change in damping rate is found to occur predominantly in a small temperature region just below Tλ, for all q-values. We do not find any evidence for the sudden appearance of the predicted “renormalized single-particle” excitations as one enters the superfluid phase. We argue that the full dispersion curve of the phonon-maxonroton excitations can be understood for all temperatures and pressures in terms of the damping rate of the momentum fluctuations, whereas the rapid changes in this damping rate near Tλ can be viewed as a direct consequence of the Bose symmetry requirements on the4He-wavefunction.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 121 (2000), S. 293-302 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We present a unified description of the dynamic response of superfluid 4 He using perturbation theory. We show that the characteristic features of the 4 He inelastic neutron scattering spectra at T∼1 K can be fully described by considering only density fluctuations. We also discuss how the response changes when the temperature is raised through the superfluid phase to the normal-fluid phase, and we argue that these changes principally reflect the behavior expected because of the Bose statistics obeyed by all the 4 He atoms rather than being effects of the depletion of the Bose condensate.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Journal of low temperature physics 89 (1992), S. 437-440 
    ISSN: 1573-7357
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract We correct for the effect of temperature induced frequency shifts on the observed dynamic structure factor S(q,ω) and find that the intrinsic behavior for non-superfluid4He is remarkably similar to that for other noble-gas fluids.
    Type of Medium: Electronic Resource
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