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See, for example, Proceedings of the 6th International Workshop on Disordered Systems, Andalo [Philos. Mag B 77 (1998)];.Proceedings of the 3rd International Discussion Meeting on Relaxation in Complex Systems, Vigo [J. Non-Cryst. Solids 235-237, (1998)]
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R. Schilling in Disorder Effects on Relaxational Processes, edited by R. Richert and A. Blumen (Springer, Berlin, 1994)
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R. Schilling in Disorder Effects on Relaxational Processes, edited by R. Richert and A. Blumen (Springer, Berlin, 1994).
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Non Equilibrium Phenomena in Supercooled Fluids, Glasses and Amorphous Materials
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and references therein
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Dynamics of Disordered Materials, Vol. 37 of Proceedings in Physics, edited by D. Richter, A. J. Dianoux, W. Petry, and J. Teixera, (Springer, Berlin, 1989).
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85036192429
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Relaxation Kinetics in Supercooled Liquids—Mode Coupling Theory and its Experimental Tests, edited by S. Yip, special issue of Transp. Theory Stat. Phys. 24, (1995).
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85036134986
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edited by J. P. Hansen D. Levesque , and J. Zinn-Justin North-Holland, Amsterdam
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85036147678
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The ionic glass former CKN could be considered as an exception, although it contains molecular units like (Formula presented) ions
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The ionic glass former CKN could be considered as an exception, although it contains molecular units like (Formula presented) ions.
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35
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0031270585
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C. Theis, Diploma thesis, Johannes Gutenberg-Universität Mainz, 1997
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C. Theis, Diploma thesis, Johannes Gutenberg-Universität Mainz, 1997.
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85036412833
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A. Winkler, Diploma thesis, Johannes Gutenberg-Universität Mainz, 1998
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A. Winkler, Diploma thesis, Johannes Gutenberg-Universität Mainz, 1998.
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45
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85036266480
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The validity of the factorization in (i) is guaranteed when the largest eigenvalue (Formula presented) of the stability matrix (see, e.g., 18 for simple liquids) at the critical temperature related to the nonlinear equation for the nonergodicity parameter is not degenerate. In the case that the vertices of the memory kernel that enters the MCT equations are positive, this is automatically fulfilled. Since the vertices occurring in MMCT are neither real nor positive this nondegeneracy does not hold necessarily. Nevertheless, we expect that (Formula presented) in the generic case is nondegenerate. An investigation of (Formula presented) for a system of diatomic molecules confirms this statement 28. The second scaling law is easily proved by showing that the Laplace transformed MMCT equations for (Formula presented) are invariant under the rescaling (Formula presented) for any real number y, provided the microscopic frequencies are neglected
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The validity of the factorization in (i) is guaranteed when the largest eigenvalue (Formula presented) of the stability matrix (see, e.g., 18 for simple liquids) at the critical temperature related to the nonlinear equation for the nonergodicity parameter is not degenerate. In the case that the vertices of the memory kernel that enters the MCT equations are positive, this is automatically fulfilled. Since the vertices occurring in MMCT are neither real nor positive this nondegeneracy does not hold necessarily. Nevertheless, we expect that (Formula presented) in the generic case is nondegenerate. An investigation of (Formula presented) for a system of diatomic molecules confirms this statement 28. The second scaling law is easily proved by showing that the Laplace transformed MMCT equations for (Formula presented) are invariant under the rescaling (Formula presented) for any real number y, provided the microscopic frequencies are neglected.
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85036422407
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The orientational order in simulated liquid water has recently been studied in real space via the introduction of ad hoc angular correlations. See
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The orientational order in simulated liquid water has recently been studied in real space via the introduction of ad hoc angular correlations.
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85036398431
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Properties of the molecular correlators under rotations for the case of linear molecules have been discussed in 2223 and for arbitrary molecules in 24
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Properties of the molecular correlators under rotations for the case of linear molecules have been discussed in 2223 and for arbitrary molecules in 24.
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67
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85036243507
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The minimum seen in all correlators around 0.5 ps is a finite-size effect connected to the low frequency cutoff of the density of states imposed by the boundary conditions and/or by the undamped propagation of the sound waves through the boundary conditions. Enhanced oscillations in the picosecond region have been observed in several molecular dynamics studies of supercooled liquids, especially close to the ideal-glass transitions, and finite-size-effect studies have shown that these oscillations are spurious. In network-forming liquids there is evi-dence that the finite-size effects may be superimposed on a much weaker oscillation associated with the time domain manifestation of the boson peak
-
The minimum seen in all correlators around 0.5 ps is a finite-size effect connected to the low frequency cutoff of the density of states imposed by the boundary conditions and/or by the undamped propagation of the sound waves through the boundary conditions. Enhanced oscillations in the picosecond region have been observed in several molecular dynamics studies of supercooled liquids, especially close to the ideal-glass transitions, and finite-size-effect studies have shown that these oscillations are spurious. In network-forming liquids there is evi-dence that the finite-size effects may be superimposed on a much weaker oscillation associated with the time domain manifestation of the boson peak.
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0001191340
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T. Franosch, M. Fuchs, W. Götze, M. R. Mayr, and A. P. Singh, Phys. Rev. E 55, 7153 (1997)
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Singh, A.P.5
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