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THE RELATIVISTIC MEAN-FIELD EQUATIONS OF THE ATOMIC NUCLEUS

机译:原子核的相对论平均场方程

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In nuclear physics, the relativistic mean-field theory describes the nucleus as a systemnof Dirac nucleons which interact via meson fields. In a static case and without nonlinearnself-coupling of the σ meson, the relativistic mean-field equations become a system ofnDirac equations where the potential is given by the meson and photon fields. The aimnof this work is to prove the existence of solutions of these equations. We consider anminimization problem with constraints that involve negative spectral projectors andnwe apply the concentration-compactness lemma to find a minimizer of this problem. Wenshow that this minimizer is a solution of the relativistic mean-field equations considered
机译:在核物理学中,相对论平均场理论将原子核描述为狄拉克核子的系统,狄拉克核子通过介子场相互作用。在静态情况下,没有σ介子的非线性自耦合,相对论平均场方程成为nDirac方程的系统,势由介子场和光子场给出。这项工作的目的是证明这些方程解的存在性。我们考虑带有负谱投影仪的约束的最小化问题,然后应用浓度-紧凑性引理找到该问题的最小化子。 Wenshow这个最小化器是相对论平均场方程的解决方案

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