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Green-function formalism

Cerda J, van Hove MA (1997) Efficient method for the simulation of STM images. I. Generalized green-function formalism. Phys Rev B 56 15885... [Pg.263]

In this section, we describe our model, and give a brief, self-contained account on the equations of the non-equilibrium Green function formalism. This is closely related to the electron and particle-hole propagators, which have been at the heart of Jens electronic structure research [7,8]. For more detailed and more general analysis, see some of the many excellent references [9-15]. We restrict ourselves to the study of stationary transport, and work in energy representation. We assume the existence of a well-defined self-energy. The aim is to solve the Dyson and the Keldysh equations for the electronic Green functions ... [Pg.25]

Structure of the molecular device [84-87, 129] with the well-established Green function formalism, to compute the transport characteristics. In such a way, it would be possible to distinguish self-consistently in the calculations different mechanisms, and their relative importance in experimental settings. [Pg.223]

Two different procedures were used for the removal of the reference state singularities and the derivation of RSC. As it was shown in [12], the Coulomb-Coulomb contribution to RSC is absent. The RSC were first introduced in QED in [13] in the frames of the Green function formalism in the Feynman gauge [13,14]. The expressions for RSC are much simplified in the equal energies case (Ea = Eb), i.e. for the ground state of the two-electron ion. The explicit expression for the equal energies correction was derived in [15]... [Pg.394]

There is clear now that the Green function formalism do not automatically solve the initial Schrodinger problem, but replaces it with a more general one when also the causality of events counts. The passage from the retarded to advanced Green function equation can be easily made though the previously stipulated recipe. [Pg.267]

As example of the use of exciton theory, the visible optical spectrum of two typical polydiacetylene crystals calculated by S. Suhai (PTS with an acetylene-like structure and TCDU with a butatriene-like structure) are presented using a first principle Greenes function formalism of charge transfer exciton theory. [Pg.57]


See other pages where Green-function formalism is mentioned: [Pg.98]    [Pg.263]    [Pg.25]    [Pg.763]    [Pg.62]    [Pg.763]    [Pg.179]    [Pg.196]    [Pg.57]    [Pg.1301]    [Pg.34]    [Pg.78]    [Pg.123]    [Pg.4]    [Pg.6]    [Pg.342]   
See also in sourсe #XX -- [ Pg.78 ]




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