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lei0736
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paopaomeng(½ð±Ò+1,VIP+0):лл½»Á÷ 7-8 22:44
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paopaomeng(½ð±Ò+1,VIP+0):лл½»Á÷ 7-8 22:44
zhangyy427(½ð±Ò+13,VIP+0):·Ç³£¸Ðл°¡ Ã÷°×ÁË ÎÒÔÙÉÏÍø²é²éÖÐÎÄ ºÇºÇ 7-9 08:40
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2Â¥2009-07-08 22:19:24
tianlangxingaa
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paopaomeng(½ð±Ò+1,VIP+0):лл½»Á÷ 7-8 22:44
paopaomeng(½ð±Ò+1,VIP+0):лл½»Á÷ 7-8 22:44
|
The Car¨CParrinello method is a type of ab initio (first principles) molecular dynamics, usually employing periodic boundary conditions, planewave basis sets, and density functional theory. In contrast to Born¨COppenheimer molecular dynamics wherein the nuclear (ions) degree of freedom are propagated using ionic forces which are calculated at each iteration by approximately solving the electronic problem with conventional matrix diagonalization methods, the Car¨CParrinello method explicitly introduces the electronic degrees of freedom as (fictitious) dynamical variables, writing an extended Lagrangian for the system which leads to a system of coupled equations of motion for both ions and electrons. In this way an explicit electronic minimization at each iteration is not needed: after an initial standard electronic minimization, the fictitious dynamics of the electrons keep them on the electronic ground state corresponding to each new ionic configuration visited along the dynamics, thus yielding accurate ionic forces. In order to maintain this adiabaticity condition, it is necessary that the fictitious mass of the electrons is chosen small enough to avoid a significant energy transfer from the ionic to the electronic degrees of freedom. This small fictitious mass in turn requires that the equations of motion are integrated using a smaller time step than the ones (1¨C10 fs) commonly used in Born¨COppenheimer molecular dynamics, but it is possible to extend the Car¨CParrinello formalism in order to overcome this limitation. |
3Â¥2009-07-08 22:35:04













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