2010
DOI: 10.1063/1.3442368
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Communications: Accurate and efficient approximations to explicitly correlated coupled-cluster singles and doubles, CCSD-F12

Abstract: We propose a novel explicitly correlated coupled-cluster singles and doubles method CCSD(F12(*)), which retains the accuracy of CCSD-F12 while the computational costs are only insignificantly larger than those for a conventional CCSD calculation.

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Cited by 288 publications
(313 citation statements)
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“…Explicitly correlated coupled cluster singles and doubles with perturbative triples (CCSD(T)(F12*)) calculations were performed with Turbomole 6.5 [103][104][105][106] using the cc-pVDZ-F12 107 basis set as well as the corresponding auxiliary basis sets. 108 The Hartree-Fock contribution was corrected with the complementary auxiliary basis set (CABS) singles approach of Knizia and Werner.…”
Section: Quantum Chemical Methods and Qce Protocolmentioning
confidence: 99%
“…Explicitly correlated coupled cluster singles and doubles with perturbative triples (CCSD(T)(F12*)) calculations were performed with Turbomole 6.5 [103][104][105][106] using the cc-pVDZ-F12 107 basis set as well as the corresponding auxiliary basis sets. 108 The Hartree-Fock contribution was corrected with the complementary auxiliary basis set (CABS) singles approach of Knizia and Werner.…”
Section: Quantum Chemical Methods and Qce Protocolmentioning
confidence: 99%
“…69 The SP ansatz (also called the fixed amplitude or diagonal orbital invariant ansatz), in conjunction with STG, greatly simplifies the implementation and has been used in various CC models with Lagrangian functionals. [70][71][72][73][74][75] These have also been expanded into F12 adaptations in local correlation pictures, as we will outline later. Note the rational generator is a spin-free operator that does not contain the spin index s. This feature permits the application ofR 12 to open-shell references involving unrestricted HF (UHF), 76,77 restricted open-shell HF (ROHF), 74,78,79 and multi-determinant [80][81][82][83][84][85] wave functions in the manner of spinflipped geminal 73,77 and internally contracted 80 bases.…”
Section: Introductionmentioning
confidence: 99%
“…The level of correlation treatment is unchanged, while the basis set limit for the parameterization of the double excitations is approached more rapidly than for standard methods. The reason that F12 methods achieve near basis set limit accuracy with relatively small basis sets is because the F12 basis functions efficiently describe the sharp features of the wave function in the region of short-range r 12 , that is, the correlation cusp. In this way, the X −3 energy convergence of the orbital expansion is accelerated to X −7 for F12 methods, where X is the cardinal number of the orbital basis set.…”
Section: F12 Basis Functionsmentioning
confidence: 99%
“…Two-body electronelectron interactions are accounted for through double excitations, where a pair of occupied spin orbitals |ij is replaced by a linear combination of pair functions |ab , where a, b are virtual spin orbitals. The essence of F12 theory is to use a basis of pair functions |w xy in addition to the standard pair basis |ab , where |w xy depends explicitly on r 12 , the distance between two electrons. The level of correlation treatment is unchanged, while the basis set limit for the parameterization of the double excitations is approached more rapidly than for standard methods.…”
Section: F12 Basis Functionsmentioning
confidence: 99%
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