1997
DOI: 10.1142/s0218301397000299
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Recent Progress in Quantum Hadrodynamics

Abstract: Quantum hadrodynamics (QHD) is a framework for describing the nuclear many-body problem as a relativistic system of baryons and mesons. Motivation is given for the utility of such an approach and for the importance of basing it on a local, Lorentz-invariant lagrangian density. Calculations of nuclear matter and finite nuclei in both renormalizable and nonrenormalizable, effective QHD models are discussed. Connections are made between the effective and renormalizable models, as well as between relativistic mean… Show more

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Cited by 1,001 publications
(1,575 citation statements)
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References 412 publications
(748 reference statements)
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“…Relativistic mean-field models traditionally include an isodoublet nucleon field (ψ) interacting via the exchange of two isoscalar mesons (a scalar φ and a vector V µ ), one vector-isovector meson (b µ ), and the photon (A µ ) [8][9][10]. The non-interacting Lagrangian density for such a model may be written as follows:…”
Section: A Relativistic Mean-field Modelsmentioning
confidence: 99%
“…Relativistic mean-field models traditionally include an isodoublet nucleon field (ψ) interacting via the exchange of two isoscalar mesons (a scalar φ and a vector V µ ), one vector-isovector meson (b µ ), and the photon (A µ ) [8][9][10]. The non-interacting Lagrangian density for such a model may be written as follows:…”
Section: A Relativistic Mean-field Modelsmentioning
confidence: 99%
“…We note that the equation of state calculation of Buchler and Coon [19] is close in strategy to the virial equation of state, but it takes into account Pauli blocking on the phase shifts and thus uses a model NN interaction. Moreover, there are a variety of Skyrme-type [20,21,22] and relativistic mean-field [23,24,25] parametrizations of the nuclear energy functional, which are used to calculate ground-state energies and densities of intermediate-mass and heavy nuclei. However, it is not clear what form to take for the energy functional for a gas of nucleons at low densities, where the system forms clusters and the binding energy per nucleon is density-independent with E/A ≈ −16 MeV.…”
Section: Introductionmentioning
confidence: 99%
“…Here we focus our attention on relativistic heavy ion collisions, that provide a unique terrestrial opportunity to probe the in-medium nuclear interaction in high density and high momentum regions. An effective Lagrangian approach to the hadron interacting system is extended to the isospin degree of freedom: within the same frame equilibrium properties (EoS, [ 3]) and transport dynamics [ 4,5] can be consistently derived.…”
Section: Introductionmentioning
confidence: 99%