Cluster perturbation theory. III. Perturbation series for coupled cluster singles and doubles excitation energies

被引:17
|
作者
Baudin, Pablo [1 ,2 ]
Pawlowski, Filip [2 ,3 ]
Bykov, Dmytro [2 ,4 ]
Liakh, Dmitry [4 ]
Kristensen, Kasper [2 ,5 ]
Olsen, Jeppe [2 ]
Jorgensen, Poul [2 ]
机构
[1] Ecole Polytech Fed Lausanne, Inst Chem Sci & Engn, Lab Computat Chem & Biochem, CH-1015 Lausanne, Switzerland
[2] Aarhus Univ, Dept Chem, Langelandsgade 140, DK-8000 Aarhus C, Denmark
[3] Auburn Univ, Dept Chem & Biochem, Auburn, AL 36849 USA
[4] Oak Ridge Natl Lab, 1 Bethel Valley Rd, Oak Ridge, TN 37831 USA
[5] Aarhus Univ, Sch Engn, Inge Lehmanns Gade 10, DK-8000 Aarhus C, Denmark
来源
JOURNAL OF CHEMICAL PHYSICS | 2019年 / 150卷 / 13期
基金
欧洲研究理事会;
关键词
CONFIGURATION-INTERACTION SINGLES; POLARIZATION PROPAGATOR; TRANSITION-PROBABILITIES; ELECTRONIC-STRUCTURE; RESPONSE FUNCTIONS; EXCITED-STATES; WAVE-FUNCTION; BASIS-SETS; 3RD-ORDER; MODEL;
D O I
10.1063/1.5046935
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The cluster perturbation series, CPS(D), for coupled cluster singles and doubles excitation energies is considered. It is demonstrated that the second-order model CPS(D-2) is identical to the configuration interaction singles with perturbative doubles, CIS(D) model. The third-order model, CPS(D-3), provides excitation energies of coupled cluster singles and doubles (CCSD) quality in the sense that the difference between CPS(D-3) and CCSD excitation energies is of the same size or smaller than the effect of adding triples corrections to CCSD excitation energies. We further show that the third-order corrections can be efficiently implemented, in particular, when the resolution of the identity approximation is used for integrals. We also show that the CPS(D-3) excitation energies can be determined for system sizes that are far beyond what can be considered in conventional CCSD excitation energy calculations. Published under license by AIP Publishing.
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页数:22
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