Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Computer Physics Reports

Computational methods for the one-particle green's function

Wolfgang von Niessen, J. Schirmer, Lorenz S. Cederbaum

Published Apr 1, 1984• 1,127 citations
Publisher
DOI
10.1016/0167-7977(84)90002-9

Related papers

One-particle Green's functions from the quantum equation of motion algorithm

Jacopo Rizzo, Francesco Libbi, Francesco Tacchino +3 more

Many-body Green's functions encode all the properties and excitations of interacting electrons. While these are challenging to be evaluated accurately on a classical computer, recent efforts have been directed toward finding quantum algorithms that may provide a quantum advantage for this task, exploiting architectures that will become available in the near future. In this work we introduce a novel near-term quantum algorithm for computing one-particle Green's functions via their Lehmann representation. The method is based on a generalization of the quantum equation of motion algorithm that gives access to the charged excitations of the system. We demonstrate the validity of the present proposal by computing the Green's function of a two-site Fermi-Hubbard model on a IBM quantum processor.

arXiv:2201.01826•Physical Review Research•Oct 7, 2022•23 citations

Determination of the one-particle Green's function: freedom and constraints

Pina Romaniello, Giovanna Lani, Lucia Reining

Bulletin of the American Physical Society•Mar 4, 2014•0 citations

Evaluation of two-particle properties within finite-temperature self-consistent one-particle Green’s function methods: Theory and application to GW and GF2

Pavel Pokhilko, Sergei Iskakov, Chia-Nan Yeh +1 more

One-particle Green’s function methods can model molecular and solid spectra at zero or non-zero temperatures. One-particle Green’s functions directly provide electronic energies and one-particle properties, such as dipole moment. However, the evaluation of two-particle properties, such as ⟨S2⟩ and ⟨N2⟩, can be challenging because they require a solution of the computationally expensive Bethe–Salpeter equation to find two-particle Green’s functions. We demonstrate that the solution of the Bethe–Salpeter equation can be completely avoided. Applying the thermodynamic Hellmann–Feynman theorem to self-consistent one-particle Green’s function methods, we derive expressions for two-particle density matrices in a general case and provide explicit expressions for GF2 and GW methods. Such density matrices can be decomposed into an antisymmetrized product of correlated one-electron density matrices and the two-particle electronic cumulant of the density matrix. Cumulant expressions reveal a deviation from ensemble representability for GW, explaining its known deficiencies. We analyze the temperature dependence of ⟨S2⟩ and ⟨N2⟩ for a set of small closed-shell systems. Interestingly, both GF2 and GW show a non-zero spin contamination and a non-zero fluctuation of the number of particles for closed-shell systems at the zero-temperature limit.

arXiv:2104.10308•The Journal of Chemical Physics•Jul 13, 2021•27 citations

The single-particle Green’s function

Lecture notes in physics. M, Monographs•Dec 15, 2008•1 citation

Analytical properties of one-particle Green's functions

Institute of Physics eBooks•Nov 26, 2004•0 citations

- Nonlocal Operators

Girish S. Setlur

The description of many-particle quantum mechanics given till now does not give us much insight into how one may go about computing the Green function of quantum systems with infinitely many coupled degrees of freedom. Apart from the free particle case and perhaps the harmonic oscillator, there are precious few exact computations of Green functions of many-particle systems. Even the approximate methods are found wanting since we have already alluded to the ‘uncontrolled’ nature of most of the approximations that have been proposed to date. There is one method that offers some hope in this regard. This method is (wrongly) called ‘bosonization’. This method will be the main focus of much of this and the next chapter. The main mathematical tool used is the introduction of operators that are ‘non-local’ in a sense to be made precise later, which enables the exact computation of the asymptotic properties of the Green function (G(x− x′, t− t ′) in the regime |x− x′| → ∞ and/or |t − t ′| → ∞) under some further restrictive assumptions. We wish to ease into this subject through the study of quantum vortices in charged bosons where the notion of nonlocality makes its presence felt in a relatively more familiar setting.

CRC Press eBooks•Dec 5, 2013•0 citations
Many-body Green's functions encode all the properties and excitations of interacting electrons. While these are challenging to be evaluated accurately on a classical computer, recent efforts have been directed toward finding quantum algorithms that may provide a quantum advantage for this task, exploiting architectures that will become available in the near future. In this work we introduce a novel near-term quantum algorithm for computing one-particle Green's functions via their Lehmann representation. The method is based on a generalization of the quantum equation of motion algorithm that gives access to the charged excitations of the system. We demonstrate the validity of the present proposal by computing the Green's function of a two-site Fermi-Hubbard model on a IBM quantum processor.
One-particle Green’s function methods can model molecular and solid spectra at zero or non-zero temperatures. One-particle Green’s functions directly provide electronic energies and one-particle properties, such as dipole moment. However, the evaluation of two-particle properties, such as ⟨S2⟩ and ⟨N2⟩, can be challenging because they require a solution of the computationally expensive Bethe–Salpeter equation to find two-particle Green’s functions. We demonstrate that the solution of the Bethe–Salpeter equation can be completely avoided. Applying the thermodynamic Hellmann–Feynman theorem to self-consistent one-particle Green’s function methods, we derive expressions for two-particle density matrices in a general case and provide explicit expressions for GF2 and GW methods. Such density matrices can be decomposed into an antisymmetrized product of correlated one-electron density matrices and the two-particle electronic cumulant of the density matrix. Cumulant expressions reveal a deviation from ensemble representability for GW, explaining its known deficiencies. We analyze the temperature dependence of ⟨S2⟩ and ⟨N2⟩ for a set of small closed-shell systems. Interestingly, both GF2 and GW show a non-zero spin contamination and a non-zero fluctuation of the number of particles for closed-shell systems at the zero-temperature limit.
The description of many-particle quantum mechanics given till now does not give us much insight into how one may go about computing the Green function of quantum systems with infinitely many coupled degrees of freedom. Apart from the free particle case and perhaps the harmonic oscillator, there are precious few exact computations of Green functions of many-particle systems. Even the approximate methods are found wanting since we have already alluded to the ‘uncontrolled’ nature of most of the approximations that have been proposed to date. There is one method that offers some hope in this regard. This method is (wrongly) called ‘bosonization’. This method will be the main focus of much of this and the next chapter. The main mathematical tool used is the introduction of operators that are ‘non-local’ in a sense to be made precise later, which enables the exact computation of the asymptotic properties of the Green function (G(x− x′, t− t ′) in the regime |x− x′| → ∞ and/or |t − t ′| → ∞) under some further restrictive assumptions. We wish to ease into this subject through the study of quantum vortices in charged bosons where the notion of nonlocality makes its presence felt in a relatively more familiar setting.