2016
DOI: 10.1103/physreva.94.062512
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Coupled-cluster Green's function: Analysis of properties originating in the exponential parametrization of the ground-state wave function

Abstract: In this paper we derive basic properties of the Green's function matrix elements stemming from the exponential coupled cluster (CC) parametrization of the ground-state wave function. We demonstrate that all intermediates used to express retarded (or equivalently, ionized) part of the Green's function in the ω-representation can be expressed through connected diagrams only. Similar properties are also shared by the first order ω-derivative of the retarded part of the CC Green's function. Moreover, first order ω… Show more

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Cited by 29 publications
(50 citation statements)
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References 78 publications
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“…The earliest are from Nooijen and coworkers 22,23 while the most recent ones can be found in Ref. 13,[24][25][26]. These solve for the Green's function using linear equations on the real axis.…”
Section: Introductionmentioning
confidence: 99%
“…The earliest are from Nooijen and coworkers 22,23 while the most recent ones can be found in Ref. 13,[24][25][26]. These solve for the Green's function using linear equations on the real axis.…”
Section: Introductionmentioning
confidence: 99%
“…This representation can be used to prove/derive basic properties of GFCC including connected character of Green's function matrix elements and their arbitraryorder ω-derivatives. [48,49] The possibility of calculating GFCC matrix and their ω-derivatives, through the Dyson equations, extends in a natural way to the corresponding self-energies. These properties enable one to calculate spectral functions, pole strengths, and other properties using GFCC method.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper we further extend the analysis carried out in the previous papers. [ [46][47][48][49][50] In particular, motivated by the accuracy attainable by the GFCC model with singles, doubles, and triples (GFCCSDT) [47] we explore the possibilities of further improving accuracies of calculated pole locations by only increasing excitation level in the auxiliary inner operators X p (ω) and Y q (ω). To this end we discuss the general class of GFCC-i(n, m) approximations, where n is the rank of excitations included in the T and Λ operators, while m designates the excitation level used to define X p (ω) and Y q (ω) operators.…”
Section: Introductionmentioning
confidence: 99%
“…As discusseded in our previous work on this subject [51,[62][63][64][65][66], the practical calculation of GFCCSD matrix employing the above method involves the solution of the conventional To address this issue, in the context of high performance computing, one can divide the full computational task posed by the GFCC method into several smaller tasks according to the number of orbitals and frequencies desired. In so doing, one can distribute these smaller tasks over the available processors to execute them concurrently.…”
Section: Methodsmentioning
confidence: 99%
“…Alternatively, the CC Green's function matrix may be obtained directly in its analytic form [25][26][27] through the evaluation of a shifted set of linear systems involving the IP/EA-EOM-CC Hamiltonian at a frequency of interest [51,[62][63][64][65][66]. In the treatment of the GFCC method as a linear system, one is able to bypass the need for the evaluation of the eigenstates of the IP/EA-EOM-CC Hamiltonian explicitly, and in principle efficiently resolve the entire spectrum of the IP/EA-EOM-CC Hamiltonian.…”
Section: Introductionmentioning
confidence: 99%