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The external linearly polarized electronic field is given as the time derivative of the vector potential [see Eqs. (3.45) and (3.46)], [Pg.45]

One convenient form for the envelope function is a Gaussian function. [Pg.45]

Chemical Theory Beyond the Born-Oppenheimer Paradigm [Pg.46]

See other pages where The external fields introduced is mentioned: [Pg.6] [Pg.17] [Pg.45] [Pg.200]