The current density order based on the Ginzburg-Landau description
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Інститут фізики напівпровідників імені В.Є. Лашкарьова НАН України
Анотація
The goal of this survey is to deduce the grandeurs, or the set of grandeurs,
 from which is derived simultaneously as a linear combination of densities of states,
 current density matrix and the reduced entropy, according to the general fact that the
 logarithm of the distribution is additive first integral. In this perspective, we introduce the
 notations, which gives to the logarithm of the distribution as the
 quaternionic picture of the operatorial transcriptions, this must follow the behaviour of a
 canonical distribution through the interval of the transitions. It seems that the
 nonreproducibility is caused essentially by the fact of absolute separability of dimensions
 between the observed and observer. The reduced entropy will suggest the inner
 displaying of observer, the invariance of unsymmetric order parameter products will be
 an expression of reproducibility. We must have a displaying of such products over inner
 dimensions, allowing to translate a limit of the displaying of stationary levels of
 macroscopic bodies over inner distances. Iˆ is the parity operator and will act under
 respect or violation of products as uncertainties, Jˆ is representing measurement process
 decomposing layers, sublayers and orbitals according to the thresholds logics answering
 how cold will be felt to transgress the conventional univoc filling rules, Kˆ represents
 measurement process realising the centesimal entropy depth penetration. The
 introduction of such notations will be justified by the fact that the ρ -distribution,
 introduced as an unsymmetric product of order parameters, is defined per pavement –
 pavement as defined by J.H. Poincaré.
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The current density order based on the Ginzburg-Landau description / Z. Bousnane, N. Merabtine, M. Benslama, F. Bousaad // Semiconductor Physics Quantum Electronics & Optoelectronics. —  2007. — Т. 10, № 1. — С. 97-100. — Бібліогр.: 2 назв. — англ.