Fixed points of the Similarity Renormalization Group and the Nuclear Many-Body Problem
arXiv:1310.8246 · doi:10.1007/s00601-014-0858-7
Abstract
The Similarity Renormalization Group reduces the off-shellness by driving the evolved interaction towards a diagonal band. We analyze the infrared limit and the corresponding on-shell interactions and its consequences for light nuclei. Using a harmonic oscillator shell model we obtain a Tjon line B(4He)= 4B(3H)-3B(2H) which can be understood from a combinatorics counting of nucleon pairs and triplets in the triton and alpha-particle and compares favorably with realistic calculations.
Presented by E.R.A. at the 22th European Conference On Few-Body Problems In Physics: EFB22 9 - 13 Sep 2013, Krakow (Poland), 5 pages, 3 figures (corrections and references added)
References in corpus (10)
- Similarity Renormalization Group for Nucleon-Nucleon Interactions
- Three-body forces: From cold atoms to nuclei
- Evolution of Nuclear Many-Body Forces with the Similarity Renormalization Group
- Evolving Nuclear Many-Body Forces with the Similarity Renormalization Group
- Evolved Chiral NN+3N Hamiltonians for Ab Initio Nuclear Structure Calculations
- Momentum space evolution of chiral three-nucleon forces
- Block Diagonalization using SRG Flow Equations
- Implicit vs Explicit Renormalization and Effective Interactions
- Three-Body Forces Produced by a Similarity Renormalization Group Transformation in a Simple Model
- Nuclear Symmetries of the similarity renormalization group for nuclear forces
Cited by in corpus (7)
- Binding in light nuclei: Statistical NN uncertainties vs Computational accuracy
- The infrared limit of the Similarity Renormalization Group evolution and Levinson's theorem
- Implicit and explicit renormalization: two complementary views of effective interactions
- The BCS pairing gap in the on-shell limit of the Similarity Renormalization Group
- scattering from a similarity renormalization group perspective
- On-shell transition of SRG and nuclear systems
- Fixed points of the SRG evolution and the on-shell limit of the nuclear force