Vector meson mass in the chiral symmetry restored vacuum
arXiv:2012.06463 · doi:10.1103/PhysRevD.103.L051501
Abstract
We calculate the mass of the vector meson in the chiral symmetry restored vacuum. This is accomplished by separating the four quark operators appearing in the vector and axial vector meson sum rules into chiral symmetric and symmetry breaking parts depending on the contribution of the fermion zero modes. We then identify each part from the fit to the vector and axial vector meson masses. By taking the chiral symmetry breaking part to be zero while keeping the symmetric operator to the vacuum value, we find that the chiral symmetric part of the vector and axial vector meson mass to be between 550 and 600 MeV. This demonstrates that chiral symmetry breaking, while responsible for the mass difference between chiral partner, accounts only for a small fraction of the symmetric part of the mass.
arXiv comment5 pages, 3 figures
References in corpus (13)
- Current correlation functions, QCD sum rules and vector mesons in baryonic matter
- Hadron properties in the nuclear medium
- On meson resonances and chiral symmetry
- Evidence for the Role of Instantons in Hadron Structure from Lattice QCD
- Hadrons in strongly interacting matter
- Meson-nucleus potentials and the search for meson-nucleus bound states
- The High Temperature Phase of QCD and {\boldmath } Symmetry
- Origins of Mass
- Hadron Physics at J-PARC
- QCD Sum Rule for Open Strange Meson in Nuclear Matter
- On light vector mesons and chiral SU(3) extrapolations
- Trigger Merging Module for the J-PARC E16 Experiment
- Theory on Hadrons in Nuclear Medium
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- mesons moving in nuclear matter
- Chiral, parity-doublet, effective-Lagrangian mean-field theories for nuclear and astrophysical phenomenology