2022
DOI: 10.48550/arxiv.2201.00431
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Instanton effects on chiral symmetry breaking and hadron spectroscopy

Abstract: This project aims to give indications to find monopole and instanton effects in QCD on the observables by experiments. First, we add the monopole and anti-monopole to the QCD vacuum of the quenched SU(3) and calculate the physical observables using the eigenvalues and eigenvectors of the overlap Dirac operator that preserves the exact chiral symmetry. We have found that the additional monopole and anti-monopole make the long monopole loops are closely related to the quark confinement without changing the vacuu… Show more

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Cited by 2 publications
(5 citation statements)
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“…Accordingly, we carry out numerical calculations using the eigenvalues and eigenvectors of the overlap Dirac operator that preserves the exact chiral symmetry in lattice gauge theory [36][37][38][39][40] and quantitatively demonstrate the monopole and instanton effects in QCD on chiral symmetry breaking and hadrons [41][42][43]. The primary purposes of this study are to inspect the influences of the finite lattice volume and discretization on the observables and quantitative relations that we have obtained in our previous research and to derive the interpolated results at the continuum limit.…”
Section: Introductionmentioning
confidence: 90%
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“…Accordingly, we carry out numerical calculations using the eigenvalues and eigenvectors of the overlap Dirac operator that preserves the exact chiral symmetry in lattice gauge theory [36][37][38][39][40] and quantitatively demonstrate the monopole and instanton effects in QCD on chiral symmetry breaking and hadrons [41][42][43]. The primary purposes of this study are to inspect the influences of the finite lattice volume and discretization on the observables and quantitative relations that we have obtained in our previous research and to derive the interpolated results at the continuum limit.…”
Section: Introductionmentioning
confidence: 90%
“…Next, we calculate the intersections a F π P S and am π P S between the curve (42) and the linear functions made using the fitting results of the slope a −1 A P S and intercept a B P S . The normalization factor Z π is determined for each lattice using the intersections of the standard configuration and the experimental outcomes of the pion decay constant (43) or pion mass (44) as follows:…”
Section: Matching the Decay Constant And Mass Of The Pseudoscalar Mes...mentioning
confidence: 99%
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“…We have already presented the preliminary results at the 38th international symposium on lattice field theory [43].…”
Section: Introductionmentioning
confidence: 99%