sup 4 He binding energy calculation including full tensor-force effects

Journal Article · Fri Sep 01 00:00:00 EDT 1989 · Physical Review (Section) C: Nuclear Physics; (USA)

DOI:https://doi.org/10.1103/PhysRevC.40.1390· OSTI ID:5552844

Fonseca, A C ^[1]

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1. Centro de Fisica Nuclear, Universidade de Lisbon, 1699 Lisbon, Portugal (PT)

The four-body equations of Alt, Grassberger, and Sandhas are solved in the version where the (2)+(2) subamplitudes are treated exactly by convolution, using one-term separable Yamaguchy nucleon-nucleon potentials in the {sup 1}S{sub 0} and {sup 3}S{sub 1}-{sup 3}D{sub 1} channels. The resulting {ital j}{sup {ital p}}=1/2{sup +} and 3/2{sup +} three-body subamplitudes are represented in a separable form using the energy-dependent pole expansion. Converged bound-state results are calculated for the first time using the full interaction, and are compared with those obtained from a simplified treatment of the tensor force. The Tjon line that correlates three-nucleon and four-nucleon binding energies is shown using different nucleon-nucleon potentials. In all calculations the Coulomb force has been neglected.

• OSTI ID: 5552844
• Journal Information: Physical Review (Section) C: Nuclear Physics; (USA), Vol. 40:3; ISSN 0556-2813
• Country of Publication: United States
• Language: English

Related Subjects

73 NUCLEAR PHYSICS AND RADIATION PHYSICS
HELIUM 4
BINDING ENERGY
ANGULAR MOMENTUM
BOUND STATE
COULOMB FIELD
ENERGY DEPENDENCE
FOUR-BODY PROBLEM
NUCLEON-NUCLEON POTENTIAL
S WAVES
TENSOR FORCES
WAVE FUNCTIONS
ELECTRIC FIELDS
ENERGY
EVEN-EVEN NUCLEI
FUNCTIONS
HELIUM ISOTOPES
ISOTOPES
LIGHT NUCLEI
MANY-BODY PROBLEM
NUCLEI
PARTIAL WAVES
POTENTIALS
STABLE ISOTOPES
653001* - Nuclear Theory- Nuclear Structure
Moments
Spin
& Models