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Sadlej relation

Sadlej Relation—Electric Field Variant Orbitals... [Pg.747]

Fig. 12.7. Sadlej relation. The electric field mainly causes a shift of the electronic charge distribution toward the anode (a). A GTO represents the eigenfunction of a harmonic oscillator. Suppose that an electron oscillates in a parabolic potential energy well (with the force constant I ). In this situation, a homogeneous electric field corresponds to the perturbation x, that conserres the hannonicity with unchanged force constant k (b). Fig. 12.7. Sadlej relation. The electric field mainly causes a shift of the electronic charge distribution toward the anode (a). A GTO represents the eigenfunction of a harmonic oscillator. Suppose that an electron oscillates in a parabolic potential energy well (with the force constant I ). In this situation, a homogeneous electric field corresponds to the perturbation x, that conserres the hannonicity with unchanged force constant k (b).
The nife field method, e.g., a variational approach in which the interaction with a weak homogeneous electric field is included in the Hamiltonian. The components of the polarizability are computed as the second derivatives of the energy with respect to the corresponding field components (the derivatives are calculated at the zero field). In practical calculations within the LCAO MO approximation, we often use the Sadlej relation that connects the shift of a Gaussian atomic orbital with its exponent and the electric field intensity. [Pg.788]

Sadlej relation (p. 640) second/third harmonic generation (p. 646) nuclear magnetic dipole (p. 648) spin magnetic moment (p. 648) g5Tomagnetic factor (p. 648)... [Pg.677]

X2C ( eXact 2-Component ) is an umbrella acronym [56] for a variety of methods that arrive at an exactly decoupled two-component Hamiltonian, with X2C referring to one-step approaches [65]. Related methods to arrive at formally exact two-component relativistic operators are, for example, infinite-order methods by Barysz and coworkers (BSS = Barysz Sadlej Snijders, lOTC = infinite-order two-component) [66-69] and normalized elimination of the small component (NESC) methods [70-77]. We discuss here an X2C approach as it has been implemented in a full two-component form with spin-orbit (SO) coupling and transformation of electric property operators to account for picture-change (PC) corrections [14],... [Pg.312]


See other pages where Sadlej relation is mentioned: [Pg.749]    [Pg.750]    [Pg.789]    [Pg.1036]    [Pg.640]    [Pg.642]    [Pg.643]    [Pg.675]    [Pg.750]    [Pg.789]    [Pg.1036]    [Pg.749]    [Pg.750]    [Pg.789]    [Pg.1036]    [Pg.640]    [Pg.642]    [Pg.643]    [Pg.675]    [Pg.750]    [Pg.789]    [Pg.1036]    [Pg.200]    [Pg.110]    [Pg.184]    [Pg.71]    [Pg.99]    [Pg.266]    [Pg.138]    [Pg.153]    [Pg.749]    [Pg.27]    [Pg.120]    [Pg.322]    [Pg.179]   
See also in sourсe #XX -- [ Pg.640 ]




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