New iterative and non-iterative triple excitation corrections to EOM-CCSD are presented based upon the CCSDT-3 method. This method is recommended formally, since it fully employs the EOM-CCSD Hamiltonian /t = exp[-(T 1 + T2)]H exp(T I + T z) in its development. This permits defining iterative EOM-CC
Open-shell analytical energy gradients for triple excitation many-body, coupled-cluster methods: MBPT(4), CCSD+T(CCSD), CCSD(T),and QCISD(T)
✍ Scribed by John D. Watts; Jürgen Gauss; Rodney J. Bartlett
- Publisher
- Elsevier Science
- Year
- 1992
- Tongue
- English
- Weight
- 540 KB
- Volume
- 200
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
Equations are derived for the derivatives of the contribution of triple excitations to the energy for the fourth-order many-body perturbation theory (MBPT (4) ), quadratic configuration interaction with singles, doubles, and noniterative triples (QCISD(T ) ), and coupled-cluster with singles, doubles, and noniterative triples (CCSD+T(CCSD) and CCSD(T)) methods. Based on these equations, analytical gradients have been efficiently implemented for the four aforementioned methods for unrestricted Hartree-Fock (UHF) reference functions. This is the first implementation of open-shell analytical gradients for the QCISD(T), CCSD+T( CCSD), and CCSD(T) methods. The new analytical gradient techniques have been used to compute the structure and some properties of the ground state of the HO0 radical with extended basis sets.
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