Few-nucleon forces from chiral Lagrangians
Journal Article
·
· Physical Review, C (Nuclear Physics); (United States)
- Department of Physics, FM-15, University of Washington, Seattle, Washington 98195 (United States)
Few-nucleon forces are considered from the point of view of effective chiral Lagrangians. It is argued that such forces naturally arise at the same order in chiral perturbation theory as some important features of the two-nucleon force. In particular, the leading few-nucleon forces cancel against the leading recoil correction in the iteration of the two-body potential. The remaining three-body potential is presented in momentum and coordinate spaces. It is dominated by contributions of the delta isobar of (i) two-pion range, which are not new, and (ii) shorter range, which involve an undetermined parameter.
- OSTI ID:
- 7050430
- Journal Information:
- Physical Review, C (Nuclear Physics); (United States), Journal Name: Physical Review, C (Nuclear Physics); (United States) Vol. 49:6; ISSN 0556-2813; ISSN PRVCAN
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
662240 -- Models for Strong Interactions-- (1992-)
663110* -- General & Average Properties of Nuclei & Nuclear Energy Levels-- (1992-)
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
BINDING ENERGY
BOSONS
CHIRAL SYMMETRY
ELEMENTARY PARTICLES
ENERGY
FIELD THEORIES
HADRONS
LAGRANGIAN FIELD THEORY
MANY-BODY PROBLEM
MESONS
NUCLEAR FORCES
NUCLEON-NUCLEON POTENTIAL
PIONS
POTENTIALS
PSEUDOSCALAR MESONS
QUANTUM CHROMODYNAMICS
QUANTUM FIELD THEORY
SYMMETRY
THREE-BODY PROBLEM
663110* -- General & Average Properties of Nuclei & Nuclear Energy Levels-- (1992-)
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS
73 NUCLEAR PHYSICS AND RADIATION PHYSICS
BINDING ENERGY
BOSONS
CHIRAL SYMMETRY
ELEMENTARY PARTICLES
ENERGY
FIELD THEORIES
HADRONS
LAGRANGIAN FIELD THEORY
MANY-BODY PROBLEM
MESONS
NUCLEAR FORCES
NUCLEON-NUCLEON POTENTIAL
PIONS
POTENTIALS
PSEUDOSCALAR MESONS
QUANTUM CHROMODYNAMICS
QUANTUM FIELD THEORY
SYMMETRY
THREE-BODY PROBLEM