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1
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0001633167
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K. Hepp and E. H. Lieb, Helv. Phys. Acta 46, 573 (1973); Dynamical Systems, Theory and Applications, Springer Lecture Notes in Physics 38, edited by J. Moser (Springer, Heidelberg, 1975), pp. 178-208.
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(1973)
Helv. Phys. Acta
, vol.46
, pp. 573
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Hepp, K.1
Lieb, E.H.2
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2
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0000641586
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Dynamical Systems, Theory and Applications
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Springer, Heidelberg
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K. Hepp and E. H. Lieb, Helv. Phys. Acta 46, 573 (1973); Dynamical Systems, Theory and Applications, Springer Lecture Notes in Physics 38, edited by J. Moser (Springer, Heidelberg, 1975), pp. 178-208.
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(1975)
Springer Lecture Notes in Physics
, vol.38
, pp. 178-208
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Moser, J.1
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4
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0002261379
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R. Graham and H. Haken, Z. Phys. 237, 31 (1970): H. Haken, Handbuch der Physik, Bd. XXV/2C (Springer, Heidelberg, 1970).
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(1970)
Z. Phys.
, vol.237
, pp. 31
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Graham, R.1
Haken, H.2
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5
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0002261379
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Springer, Heidelberg
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R. Graham and H. Haken, Z. Phys. 237, 31 (1970): H. Haken, Handbuch der Physik, Bd. XXV/2C (Springer, Heidelberg, 1970).
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(1970)
Handbuch der Physik
, vol.25
, Issue.2 C
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Haken, H.1
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7
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85033921453
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note
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Apart from the difference in their mathematical settings, this model differs from that of HL in the following physical respect. The atoms of HL are pairs of Fermi oscillators, and can thus accommodate 0, 1, or 2 electrons each; whereas those of (I) correspond to two-level atoms, each with precisely one electron.
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12
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33644647258
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Erratum, ibid. 30, 83 (1979)
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P. Vanheuverzwijn, Ann. Inst. Henri Poincaré, Sect. A 29, 123 (1978); Erratum, ibid. 30, 83 (1979); B. de Moen, P. Vanheuverzwijn, and A. Verbeure, Rep. Math. Phys. 15, 27 (1979).
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(1978)
Ann. Inst. Henri Poincaré, Sect. A
, vol.29
, pp. 123
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Vanheuverzwijn, P.1
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13
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0347525418
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P. Vanheuverzwijn, Ann. Inst. Henri Poincaré, Sect. A 29, 123 (1978); Erratum, ibid. 30, 83 (1979); B. de Moen, P. Vanheuverzwijn, and A. Verbeure, Rep. Math. Phys. 15, 27 (1979).
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(1979)
Rep. Math. Phys.
, vol.15
, pp. 27
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De Moen, B.1
Vanheuverzwijn, P.2
Verbeure, A.3
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16
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85033925658
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note
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(N), S, rather than the a's; consequently, the latter do not appear in the local field algebra when one passes to the limit N→∞.
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17
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85033909966
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note
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t, would tend to a constant as t tended to infinity, and consequently that the macroscopic dynamics would not be chaotic.
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20
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85033939741
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note
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A different variational principle, namely, one of minimum entropy production, was established in Ref. 18 for a certain class of systems, in a regime close to thermal equilibrium.
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