Screening without screening: baryon energy at high baryon density

Abstract

We compute the Coulomb interaction energy of dense sets of static quarks in a compact volume (much smaller than the lattice volume) containing one quark per lattice site. The quark color charges are combined into either a set of three-quark nucleon states, or into a non-factorizable "one big hadron" state. In both cases we find that the energy per quark is roughly constant as the volume of quarks increases. A surprise is that if we construct the nucleon states from sets of three quarks chosen at random in the volume, then the energy per quark remains roughly constant, even as the average distance between quarks in a nucleon state grows as the volume increases. This energy dependence of a nucleon in a dense medium is at odds with the behavior of an isolated nucleon as quark separation increases, and for static quarks it is not easily explicable in terms of some version of Debye screening.

arXiv comment8 pages, 6 figures

References in corpus (6)

• Coulomb Energy, Vortices, and Confinement
• The QCD phase diagram in the limit of heavy quarks using complex Langevin dynamics
• Heavy dense QCD and nuclear matter from an effective lattice theory
• Properties of Color-Coulomb String Tension
• Coulomb string tension, asymptotic string tension, and the gluon chain
• The Coulomb flux tube on the lattice