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

APS

Calculation of Few-Body Observables with the SRG Flow Equations

E. R. Anderson, R. J. Furnstahl, Robert J. Perry, S. K. Bogner, Eric Jurgenson

Published Nov 1, 2010• 0 citations
OpenAlex

Related papers

Three-body Momentum Representation SRG Evolution and Operator Factorization

Kyle Wendt

APS•Sep 1, 2014•0 citations

Phase Transition in the SRG Flow of Nuclear Interactions

V. S. Timóteo, E. Ruiz Arriola, S. Szpigel

arXiv:1611.06799•Few-Body Systems•Jan 30, 2017•1 citation

Models and Methods in Few-Body Physics

Ferreira, Lidia S, A. C. Fonseca, Ludwig Streit

Lecture notes in physics•Jan 1, 1987•87 citations

Operator evolution via the similarity renormalization group: The deuteron

E. R. Anderson, S. K. Bogner, R. J. Furnstahl +1 more

Similarity renormalization group (SRG) flow equations can be used to unitarily soften nuclear Hamiltonians by decoupling high-energy intermediate-state contributions to low-energy observables while maintaining the natural hierarchy of many-body forces. Analogous flow equations can be used to consistently evolve operators so that observables are unchanged if no approximations are made. The question in practice is whether the advantages of a softer Hamiltonian and less-correlated wave functions might be offset by complications in approximating and applying other operators. Here we examine the properties of SRG-evolved operators, focusing in this article on applications to the deuteron but leading toward methods for few-body systems. We find the advantageous features generally carry over to other operators with additional simplifications in some cases from factorization of the unitary transformation operator.

arXiv:1008.1569•Physical Review C•Nov 3, 2010•67 citations

Low-momentum interactions for few-body systems

S. K. Bogner

Few-Body Systems•Dec 1, 2008•1 citation

The similarity renormalization group for three-body interactions in one dimension

Oscar Åkerlund, Lindgren, E. J., Johan Bergsten +5 more

We report on recent progress of the implementation of the similarity renormalization group (SRG) for three-body interactions in a one-dimensional, bosonic model system using the plane-wave basis. We discuss our implementation of the flow equations and show results that confirm that results in the three-body sector remain unchanged by the transformation of the Hamiltonian. We also show how the SRG transformation decouples low- from high-momentum nodes in the three-body sector and therefore simplifies the numerical calculation of observables.

•Jan 1, 2011•6 citations
Similarity renormalization group (SRG) flow equations can be used to unitarily soften nuclear Hamiltonians by decoupling high-energy intermediate-state contributions to low-energy observables while maintaining the natural hierarchy of many-body forces. Analogous flow equations can be used to consistently evolve operators so that observables are unchanged if no approximations are made. The question in practice is whether the advantages of a softer Hamiltonian and less-correlated wave functions might be offset by complications in approximating and applying other operators. Here we examine the properties of SRG-evolved operators, focusing in this article on applications to the deuteron but leading toward methods for few-body systems. We find the advantageous features generally carry over to other operators with additional simplifications in some cases from factorization of the unitary transformation operator.
We report on recent progress of the implementation of the similarity renormalization group (SRG) for three-body interactions in a one-dimensional, bosonic model system using the plane-wave basis. We discuss our implementation of the flow equations and show results that confirm that results in the three-body sector remain unchanged by the transformation of the Hamiltonian. We also show how the SRG transformation decouples low- from high-momentum nodes in the three-body sector and therefore simplifies the numerical calculation of observables.