As suggested by Vanagas, we choose the microscopic collective states for a system of A nucleons to be those states left invariant by the transformations of the (full) orthogonal group O(n) associated with the n = A-1 Jacobi vectors. For pedagogical convenience, we begin by discussing the case of an
Simulating the dynamics of collective behavior in nonhomogeneous groups
β Scribed by A. A. Vasin
- Publisher
- Springer
- Year
- 1993
- Tongue
- English
- Weight
- 515 KB
- Volume
- 4
- Category
- Article
- ISSN
- 1046-283X
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THE COLLECTIVE BEHAVIOR Varslltlvsky 14) irlucst;lg&d the function L : N -+ N informally defined by: L(H) is tllc m;1ximum length of a configku-ation whiol~ can be grow;.. frotn one ;Uivated automaton in a linear cel1 space of ider2tical finite s?We automata kkng IZ ir2tenr~l st;ltes, Each auton2ato
Using an atomistic shell model we study the temperature dependence of the ferroelectric properties of BaTiO 3 under biaxial compressive strain applicable to growth on perovskites substrate. Molecular dynamics simulations show a ''r ! c ! p'' sequence of phase transitions when temperature is increase