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- W2000964733 abstract "In the Landau theory of second-order phase transitions one usually considers the position that the characteristic parameter of the phase transition transforms according to an irreducible representation, with wave vectors terminating at special points of the Brillouin zone. The period of the structure which arises at such transitions is a multiple of the lattice constant of the initial phase (i.e. 1, 2, 3, or 4 times)1. Such transitions are possible only if a special condition (Lifschitz condition) on the transformation properties of the characteristic parameter is fulfilled. Namely, gradient invariants such as ηδζ/δz - ζδη/δz, where q,E are the components of the characteristic parameter (transforming according to an irreducible representation with wave vector qo) must be absent.1 If the Lifschitz condition is not fulfilled, then a second-order phase transition corresponding to the irreducible representation under consideration is impossible. The transition is realized according to the representation with ..." @default.
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- W2000964733 date "1976-01-01" @default.
- W2000964733 modified "2023-09-25" @default.
- W2000964733 title "Phase transitions into inhomogeneous states" @default.
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- W2000964733 doi "https://doi.org/10.1080/00150197608236689" @default.
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