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J. P. Hansen, D. Levesque, D. Zinn-Justin, North Holland, Amsterdam
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Liquids, Freezing and the Glass Transition
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Götze, W.1
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2
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85036300870
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For a recent update and references to original work on MC theory, see Ref. 11
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For a recent update and references to original work on MC theory, see Ref. 11.
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10
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0002967101
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U. Schneider, P. Lunkenheimer, R. Brand and A. Loidl, J. Non-Cryst. Solids 235-237, 173 (1998).
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85036312271
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(unpublished)
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J. Wuttke (unpublished).
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Wuttke, J.1
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33
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85036145065
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The cross section for slow neutrons in (Formula presented) is inverse proportional to the speed of the neutron. For economic reasons, the (Formula presented) pressure and detector diameter are chosen such that the detection efficiency is high, but not close to 1. Therefore, the probability of detecting a scattered neutron depends on its energy. This energy dependence is regularly corrected for by standard formulas which in turn depend on very rough approximations for the detector geometry. Improvement will only be possible by direct experimentation on selected detector tubes
-
The cross section for slow neutrons in (Formula presented) is inverse proportional to the speed of the neutron. For economic reasons, the (Formula presented) pressure and detector diameter are chosen such that the detection efficiency is high, but not close to 1. Therefore, the probability of detecting a scattered neutron depends on its energy. This energy dependence is regularly corrected for by standard formulas which in turn depend on very rough approximations for the detector geometry. Improvement will only be possible by direct experimentation on selected detector tubes.
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36
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0001367560
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H.C. Barshilia, G. Li, G.Q. Shen, and H.Z. Cummins, Phys. Rev. E 59, 5625 (1999).
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37
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85036341277
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Using the interpolation (Formula presented)instead of the full series expansion of (Formula presented) 17 that we employ in the present paper. For the interpretation of dielectric data, the small numeric difference between the two expressions has no importance
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Using the interpolation (Formula presented)instead of the full series expansion of (Formula presented) 17 that we employ in the present paper. For the interpretation of dielectric data, the small numeric difference between the two expressions has no importance.
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-
-
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38
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85036204747
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Data from Du et al. 20. On the scale of this figure, slight distortions of light scattering spectra by insufficient band passing are negligible
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Data from Du et al. 20. On the scale of this figure, slight distortions of light scattering spectra by insufficient band passing are negligible.
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40
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0001635648
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T. Franosch, W. Götze, M. Mayr, and A.P. Singh, Phys. Rev. E 55, 3183 (1997).
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85036272935
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Phys. Rev. E (to be published)
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W. Götze and T. Voigtmann, Phys. Rev. E (to be published).
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Götze, W.1
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85036263360
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A. P. Singh, Ph.D. thesis, Technische Universität München, 1999 (unpublished)
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A. P. Singh, Ph.D. thesis, Technische Universität München, 1999 (unpublished).
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47
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85036175637
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P. K. Feyerabend, Wider den Methodenzwang (Suhrkamp, Frankfurt, 1986); see, in particular, pp. 388–389
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P. K. Feyerabend, Wider den Methodenzwang (Suhrkamp, Frankfurt, 1986); see, in particular, pp. 388–389.
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