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E. Leutheusser: Phys. Rev. A 29 (1984) 2765; U. Bengtzelius, W. Götze and A. Sjölander: J. Phys. C 17 (1984) 5915.
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Leutheusser, E.1
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0000978126
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ed. J. P. Hansen, D. Levesque and J. Zinn-Justin North-Holland, Amsterdam
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See, for example, W. Götze: Liquids, Freezing and the Glass Transition, ed. J. P. Hansen, D. Levesque and J. Zinn-Justin (North-Holland, Amsterdam, 1992) p. 287.
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Liquids, Freezing and the Glass Transition
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Götze, W.1
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5
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0000763001
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W. Götze and L. Sjögren: Z. Phys. B 65 (1987) 415; W. Götze and L. Sjögren: J. Phys. C 21 (1988) 3407; L. Sjögren: Z. Phys. B 79 (1990) 5; M. Fuchs et al.: J. Phys.: Condens. Matter 4 (1992) 7709.
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Z. Phys. B
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Götze, W.1
Sjögren, L.2
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6
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0001140794
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W. Götze and L. Sjögren: Z. Phys. B 65 (1987) 415; W. Götze and L. Sjögren: J. Phys. C 21 (1988) 3407; L. Sjögren: Z. Phys. B 79 (1990) 5; M. Fuchs et al.: J. Phys.: Condens. Matter 4 (1992) 7709.
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J. Phys. C
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Götze, W.1
Sjögren, L.2
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7
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0039648212
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W. Götze and L. Sjögren: Z. Phys. B 65 (1987) 415; W. Götze and L. Sjögren: J. Phys. C 21 (1988) 3407; L. Sjögren: Z. Phys. B 79 (1990) 5; M. Fuchs et al.: J. Phys.: Condens. Matter 4 (1992) 7709.
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Z. Phys. B
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Sjögren, L.1
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8
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0347030576
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W. Götze and L. Sjögren: Z. Phys. B 65 (1987) 415; W. Götze and L. Sjögren: J. Phys. C 21 (1988) 3407; L. Sjögren: Z. Phys. B 79 (1990) 5; M. Fuchs et al.: J. Phys.: Condens. Matter 4 (1992) 7709.
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J. Phys.: Condens. Matter
, vol.4
, pp. 7709
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Fuchs, M.1
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H. Z. Cummins et al.: Phys. Rev. E 47 (1993) 4223; Prog. Theor. Phys. Suppl. 126 (1997) 21.
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Phys. Rev. E
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Cummins, H.Z.1
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0642338813
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H. Z. Cummins et al.: Phys. Rev. E 47 (1993) 4223; Prog. Theor. Phys. Suppl. 126 (1997) 21.
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Prog. Theor. Phys. Suppl.
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15
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0002789286
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to be published
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K. Kawasaki: Physica A 208 (1994) 35; to be published.
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Physica A
, vol.208
, pp. 35
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Kawasaki, K.1
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17
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4243227441
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4,7) see also R. Schmitz, J. W. Dufty and P. De: Phys. Rev. Lett. 71 (1993) 2066. At this time it is still unclear how our DDFT can shed light on this issue, which is now under investigation.
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Phys. Rev. Lett.
, vol.71
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Schmitz, R.1
Dufty, J.W.2
De, P.3
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21
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0000782086
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N. Y.
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see J. S. Langer: Ann. Phys. (N. Y.) 54 (1969) 258, in which, however, the second-rank kinetic tensor should be modified; see K. Kitahara and M. Imada: Prog. Theor. Phys. Suppl. 64 (1978) 165.
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Ann. Phys.
, vol.54
, pp. 258
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Langer, J.S.1
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22
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0000782086
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see J. S. Langer: Ann. Phys. (N. Y.) 54 (1969) 258, in which, however, the second-rank kinetic tensor should be modified; see K. Kitahara and M. Imada: Prog. Theor. Phys. Suppl. 64 (1978) 165.
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(1978)
Prog. Theor. Phys. Suppl.
, vol.64
, pp. 165
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Kitahara, K.1
Imada, M.2
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23
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0000319550
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Although the approximation becomes better as longer coarsening lengths are chosen, a proper choice of the coarse-graining scale as described in the text is indeed a key to correctly reproduce the β-relaxation as well as the α-relaxation. If a longer coarsening scale is employed to capture the latter process as was done by C. Dasgupta and O. T. Valls: Phys. Rev. E 53 (1996) 2603, the nonlinear feedback mechanism of density fluctuations giving rise to the former process is completely lost.
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Phys. Rev. E
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Dasgupta, C.1
Valls, O.T.2
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24
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0012083898
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The same equation has been derived but in different contexts; see T. Munakata: J. Phys. Soc. Jpn. 43 (1977) 1723; B. Bagchi: Physica A 145 (1987) 273.
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(1977)
J. Phys. Soc. Jpn.
, vol.43
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Munakata, T.1
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25
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0012050380
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The same equation has been derived but in different contexts; see T. Munakata: J. Phys. Soc. Jpn. 43 (1977) 1723; B. Bagchi: Physica A 145 (1987) 273.
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(1987)
Physica A
, vol.145
, pp. 273
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Bagchi, B.1
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31
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85034463448
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note
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For L̃ = 15 and σ = 3.3h, qσ ≃ 18 at the R point of the zone boundary. No lattice pinning was detected even in the lowest packing fraction studied.
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