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Gaussian basis functions three-dimensional

In variance with the hydrogen-like and Slater functions the potential employed to formally construct the gaussian basis states has nothing to do with the real potential acting upon an electron in an atom. On the other hand the solutions of this (actually three-dimensional harmonic oscillator problem) form a complete discrete basis in the space of orbitals in contrast to the hydrogen-like orbitals. [Pg.43]

While plane wave basis sets have primarily been used for periodic systems, they can also be used for molecular species by using a supercell approach, where the molecule is placed in a sufficiently large unit cell such that it does not interact with its own image in the neighbouring cells. Placing a relatively small molecule in a large supercell to avoid self-interaction consequently requires many plane wave functions, and such cases are handled more efficiently by localized Gaussian functions. A three-dimensional periodic system, on the other hand, may be better described by a plane wave basis than with nuclear-centred basis functions. [Pg.212]


See other pages where Gaussian basis functions three-dimensional is mentioned: [Pg.79]    [Pg.485]    [Pg.903]    [Pg.184]    [Pg.24]    [Pg.181]    [Pg.198]    [Pg.198]    [Pg.281]    [Pg.24]    [Pg.133]    [Pg.24]    [Pg.170]    [Pg.214]    [Pg.222]    [Pg.118]    [Pg.337]    [Pg.215]   
See also in sourсe #XX -- [ Pg.82 , Pg.83 , Pg.84 , Pg.85 , Pg.86 , Pg.87 , Pg.88 , Pg.89 ]




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