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arXiv:2004.01706·v2·High Energy Physics — Phenomenology

Nuclear matter as a liquid phase of spontaneously broken semi-classical chiral perturbation theory: Static chiral nucleon liquids

Bryan W. Lynn🇺🇸 · Brian J. Coffey🇺🇸 · Kellen E. McGee🇺🇸 · Glenn D. Starkman🇺🇸

Abstract

We study effective field theories (EFT) of nuclear structure based on spontaneously broken global chiral symmetry of QCD with two massless quarks, i.e. . For ground-state nuclei, this EFT enables expansion and truncation in inverse powers of , with analytic operators renormalized to all loop orders. We derive the EFT Lagrangian to order . We show that of protons, neutrons and pions admits a semi-classical "Static Chiral Nucleon Liquid" (StaticNL) phase and that "Pion-less" emerges in this liquid: far-infrared pions decouple from StaticNL, vastly simplifying the derivation of saturated nuclear matter (the infinite liquid phase) and of finite microscopic liquid drops (ground-state nuclides). StaticNL are made entirely of nucleons with even parity, total spin zero, and even and ; local expectation values for spin and momenta vanish. They explain the power of pion-less to capture experimental ground-state properties of certain nuclides, this explanation following directly from the global symmetries of QCD with two massless quarks. Mean-field StaticNL non-topological solitons are true solutions of 's semi-classical symmetries: they obey all CVC and PCAC conservation laws and they have zero internal and external pressure. The nuclear liquid-drop model and the semi-empirical mass formula emerge -- with correct nuclear density and saturation and asymmetry energies -- in an explicit Thomas-Fermi construction. We relate our work to compatible and complementary work in pionless and in halo/ cluster EFTs, also composed entirely of nucleons and applied to light () nuclei, which might provide important (<12.5%) corrections to Static.

Comments: 68 pages, 4 figures, subbmitted to Phys. Rev. C. arXiv admin note: substantial text overlap with arXiv:1811.10784

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