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Pure two-body correlation matrix

A. The Pure Two-Body Correlation Matrix within the 2-RDM Formalism... [Pg.205]

That is, all the information about the three important matrices 2-RDM, 2-HRDM, and 2-G is contained and available in the pure two-body correlation matrix. Moreover, the spin properties of both the pure two-body correlation matrix and the 2-G matrices play a central role in this purification procedure. [Pg.231]

That is, both the 2-CM and the 2-G matrix have common elements, but a given element occupies different positions in each matrix. In other words, while the labels of the row/column of the 2-CM refer, as in the 2-RDM, to two particlesitwo holes, the labels of the row/column of the 2-G matrix refer to particle-hole/hole-particle. Thus, although both the 2-CM and the 2-G matrices describe similar types of correlation effects, only the 2-CM describes pure two-body correlation effects. This is because the 2-CM natural tensorial contractions vanish, and thus there is no contribution to the natural contraction of the 2-RDM into the one-body space whereas the 2-G natural tensorial contractions are functionals of the 1-RDM. [Pg.234]


See other pages where Pure two-body correlation matrix is mentioned: [Pg.207]    [Pg.230]    [Pg.233]    [Pg.207]    [Pg.230]    [Pg.233]    [Pg.55]    [Pg.55]    [Pg.177]    [Pg.183]    [Pg.519]    [Pg.362]    [Pg.95]   
See also in sourсe #XX -- [ Pg.231 , Pg.232 , Pg.233 , Pg.234 , Pg.235 , Pg.236 ]




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