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Nuclear non-perturbative excitations

Conference ·
OSTI ID:6580666
We investigate consequences of a description of nuclear physics in terms of a relativistic field theory. The model Lagrangian contained baryons, sigma-mesons and omega-mesons, and was subsequently extended to include also ..pi..-mesons and rho-mesons. The most important successes of this approach are discussed. In addition to the description of known nuclear structure the field theoretical approach may reveal entirely new nuclear phenomena, based on the explicit treatment of mesonic degrees of freedom. A phenomenological nuclear Lagrangian can be constructed, where the isovector Lorentz-vector rho-meson is described by a non-Abelian gauge field, that acquires its mass spontaneously due to the non-vanishing vacuum expectation value of a Higgs field. The gauge sector solition solution is discussed. For the SU(2) gauge field theory with the Higgs field in the fundamental representation no non-trival topological conservation laws hold. This indicates that the soliton is unstable. Fermions cannot stabilize the soliton solution energetically, because only zero-binding-energy solutions for the fermions exist. Fermions in the presence of the soliton are discussed. Also, it is attempted to achieve stability of the soliton solution by coupling it to the ..pi..-field. Describing the ..pi..-field by the nonlinear sigma-model yields a conserved topological quantum number. In the linear sigma-model the soliton can only be stabilized energetically. 32 references. (WHK)
Research Organization:
Lawrence Berkeley Lab., CA (USA); Los Alamos National Lab., NM (USA)
DOE Contract Number:
W-7405-ENG-36
OSTI ID:
6580666
Report Number(s):
LA-UR-84-2364; CONF-8406178-2; ON: DE84015525
Country of Publication:
United States
Language:
English