Abstract
Quantum chromodynamics (QCD) claims that the major source of the nucleon invariant mass is not the Higgs mechanism but the trace anomaly in the QCD energy-momentum tensor. Although experimental and theoretical results support such a conclusion, a direct demonstration is still absent. We present the first lattice QCD calculation of the quark and gluon trace anomaly contributions to the hadron masses, using the overlap fermion on the $2+1$-flavor dynamical domain wall quark ensemble at ${m}_{\ensuremath{\pi}}=340\text{ }\text{ }\mathrm{MeV}$ and lattice spacing $a=0.1105\text{ }\text{ }\mathrm{fm}$. The result shows that the gluon trace anomaly contributes to most of the nucleon mass, the contribution in the pion state is smaller than that in others nearly by a factor of $\ensuremath{\sim}10$, and the gluon trace anomaly density in the center of the pion is negative. The gluon trace anomaly coefficient $\ensuremath{\beta}/{g}^{3}=\ensuremath{-}0.056(6)$ we obtained is consistent with its regularization-independent leading-order value $(\ensuremath{-}11+\frac{2{N}_{f}}{3})/(4\ensuremath{\pi}{)}^{2}$ perfectly.
Highlights
The most essential and nontrivial feature of the quantum field theory is the regularization
The central challenge is verifying whether the difference between a hadron mass and its quark mass contribution comes from the trace anomaly effect. Such a calculation is highly nonperturbative and can only be performed by lattice Quantum chromodynamics (QCD), but the chiral symmetry breaking in the quark mass term of the Wilson-like action will mix with the original trace anomaly, since its bare quark mass suffers linear divergence
Based on the energy-momentum tensor (EMT) trace anomaly sum rule in the PS and V meson states with mv 1⁄4 0.479 GeV, we determined the bare anomalous dimensions of the quark mass and gluon coupling constant as γm and β g3
Summary
The most essential and nontrivial feature of the quantum field theory is the regularization. The trace anomaly leads to the most nontrivial feature of QCD: quantum particles like nucleons can have positive masses, even though the light quark mass is small and the gluon is massless. The central challenge is verifying whether the difference between a hadron mass and its quark mass contribution comes from the trace anomaly effect. Such a calculation is highly nonperturbative and can only be performed by lattice QCD, but the chiral symmetry breaking in the quark mass term of the Wilson-like action will mix with the original trace anomaly, since its bare quark mass suffers linear divergence. We find that the gluon trace anomaly density in the pion turns out to be much smaller than that in the other hadrons like nucleons and vector mesons, due to the significant difference in the gluon trace anomaly distribution inside the hadrons
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have
Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.