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Representation of the CCSD Amplitude Equations

The leading term of H is just the electronic Hamiltonian itself. For its contribution to the Tj amplitude equation, we must evaluate the matrix elements, (Of l(/]sj + as before. Since these elements contain the reference [Pg.88]

For the contribution of to the T2 amplitude equation, we must evaluate the matrix element, (Of- l( N + Tn)I o)5 which contains the reference deter- [Pg.88]

The contribution of the second term of Eq. [122] to the amplitude equation is only slightly more complicated. This term involves the matrix element, and, as before, we will consider only the con- [Pg.89]

However, the first two of these fragments can connect to the T diagram in only one index—via either a single hole line or particle line—thus leaving an additional line extending below the Tj interaction line in the final diagram, for example, [Pg.89]

Because such diagrams cannot represent matrix elements that have the reference wavefunction on the right, only the third diagram above can contribute to [Pg.89]


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