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McMurchie-Davidson algorithm

Relativistic generalization for G-spinor basis functions of the well-known McMurchie-Davidson algorithm [3] for direct evaluation of interaction integrals. [Pg.200]

The McMurchie-Davidson algorithm [111] is used extensively for the calculation of two electron interaction integrals in nonrelativistic electronic structure calculations. The relativistic generalization [112] can be obtained immediately... [Pg.176]

Electron repulsion integrals may be evaluated by a straightforward generalization of the McMurchie-Davidson algorithm [34], using the definition of the two-spinor charge operator. The Coulomb interaction involves only the Eg-coefficients for q = 0, and results in G-spinor integrals of the form... [Pg.28]

It is here that the simplifications made possible by defining the , -coefficients is most apparent, since integrals over 612 may be be obtained by a simple extension of the McMurchie-Davidson algorithm for electron repulsion integrals. This approach conveys the advantages of simplicity, generality and efficiency when compared with those which exist in the literature [49, 50]. [Pg.29]


See other pages where McMurchie-Davidson algorithm is mentioned: [Pg.205]    [Pg.142]    [Pg.166]    [Pg.77]    [Pg.176]    [Pg.179]    [Pg.23]    [Pg.24]    [Pg.26]    [Pg.11]    [Pg.12]    [Pg.21]    [Pg.405]    [Pg.146]    [Pg.387]   
See also in sourсe #XX -- [ Pg.166 ]




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Davidson algorithm

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