期刊
PHYSICAL REVIEW LETTERS
卷 127, 期 24, 页码 -出版社
AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.127.242002
关键词
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资金
- Office of Science of the U.S. Department of Energy [DE-AC02-05CH11231]
- Oak Ridge Leadership Computing Facility, DOE Office of Science User Facility [DE-AC05-00OR22725, LGT107]
- Institutional Computing at Los Alamos National Laboratory
- U.S. Department of Energy, Office of Science, Office of High Energy Physics [DE-AC52-06NA25396]
- LANL LDRD program
- Center for Nonlinear Studies
- Swiss National Science Foundation [PCEFP2_181117]
- Office of Science of the U.S. Department of Energy
In this study, analysis of the pion-nucleon sigma-term using lattice data was conducted to remove excited-state contamination, with results consistent with phenomenological values. Further calculations on additional physical mass ensembles are needed to confirm the results and resolve the tension between lattice QCD and phenomenology.
We present an analysis of the pion-nucleon sigma-term sigma(pi N) using six ensembles with 2 + 1 + 1-flavor highly improved staggered quark action generated by the MILC Collaboration. The most serious systematic effect in lattice calculations of nucleon correlation functions is the contribution of excited states. We estimate these using chiral perturbation theory ('PT) and show that the leading contribution to the isoscalar scalar charge comes from N pi and N pi pi states. Therefore, we carry out two analyses of lattice data to remove excited-state contamination, the standard one and a new one including N-pi and N-pi pi states. We find that the standard analysis gives sigma(pi N) = 41.9(4.9) MeV, consistent with previous lattice calculations, while our preferred chi PT-motivated analysis gives alpha N-pi = 59.6(7.4) MeV, which is consistent with phenomenological values obtained using pi N scattering data. Our data on one physical pion mass ensemble were crucial for exposing this difference, therefore, calculations on additional physical mass ensembles are needed to confirm our result and resolve the tension between lattice QCD and phenomenology.
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