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Quasi-energy ansatz

The last equation is a variation principle for the coupled cluster quasi-energy and wavefunction within oscillating harmonic external fields. If one inserts a perturbation and Fourier expansion as ansatz for the cluster amplitudes... [Pg.57]

The self-energy of the right electrode is similarly defined. How to define the lesser (greater) self-energy, which represents the scatter-in (out) function ofelectrons provided by electrodes, is the central issue. Practical applications of the NEGF will be possible if the (generalized) Kadanoff-Baym ansatz is applicable [67-69, 77]. In the E-M-E system under constant bias Vb, electrodes are the electron reservoirs by means of the Landauer picture thus they can be approximated as a non-interacting quasi-equilibrium system,... [Pg.85]

This implies that when the ZORA ansatz is employed, the small components approach zero at the nuclei. The singular behaviour encountered in quasi-relativistic approaches based on kinetic-energy balance condition is therefore avoided. The ZORA method will be discussed in more detail in the next Section, and now we just note that the ZORA ansatz has a couple of desirable properties that shall be taken into consideration when the general ansatz function is constructed. [Pg.762]


See other pages where Quasi-energy ansatz is mentioned: [Pg.151]    [Pg.22]    [Pg.151]    [Pg.22]    [Pg.57]    [Pg.76]    [Pg.43]    [Pg.758]    [Pg.131]    [Pg.582]    [Pg.585]    [Pg.1063]    [Pg.136]    [Pg.201]    [Pg.388]    [Pg.626]    [Pg.2]   
See also in sourсe #XX -- [ Pg.151 ]




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