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.
引用
收藏
页数:22
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