Renormalization group analysis of nuclear current operators
arXiv:nucl-th/0606026 · doi:10.1103/PhysRevC.74.034004 10.1103/PhysRevC.76.069902
Abstract
A Wilsonian renormalization group (WRG) equation for nuclear current operators in two-nucleon systems is derived. Nuclear current operators relevant to low-energy Gamow-Teller transitions are analyzed using the WRG equation. We employ the axial two-body current operators from phenomenological models and heavy-baryon chiral perturbation theory, which are quite different from one another in describing small scale physics. After reducing the model space of the operators using the WRG equation, we find that there still remains a significant model dependence at Λ= 200 MeV, where Λis the sharp cutoff specifying the size of the model space. A model independent effective current operator is found at a rather small cutoff value, Λ= 70 MeV. By simulating the effective current operator at Λ=70 MeV, we obtain a current operator based on a pionless theory, thereby arguing an equivalence relation between nuclear current operators of phenomenological models and those of effective field theories.
26 pages, 11 figures
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Cited by in corpus (9)
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- Proposal of a gauge-invariant treatment of l=0,1-mode perturbations on Schwarzschild Background Spacetime
- Gauge invariance in the presence of a cutoff
- On the Wilsonian renormalization group equation for nuclear current operators
- Renormalisation-group analysis of electromagnetic couplings in the pionless effective field theory
- Consistency between renormalization group running of chiral operator and counting rule -- Case of chiral pion production operator --