Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement?
Abstract We have re-analysed the lattice QCD calculations of the 3-quark potentials by: (i) Sakumichi and Suganuma (Phys Rev D 92(3), 034511, 2015); and (ii) Koma and Koma (Phys Rev D 95(9), 094513, 2017) using hyperspherical variables. We find that: (1) the two sets of lattice results have only two...
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doaj-e739a8cca3474d3e918a0f6102b7df502021-01-24T12:41:01ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522021-01-018111910.1140/epjc/s10052-021-08873-8Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement?James Leech0Milovan Šuvakov1V. Dmitrašinović2University of St. Andrews, The Old Burgh SchoolInstitute of Physics Belgrade, University of BelgradeInstitute of Physics Belgrade, University of BelgradeAbstract We have re-analysed the lattice QCD calculations of the 3-quark potentials by: (i) Sakumichi and Suganuma (Phys Rev D 92(3), 034511, 2015); and (ii) Koma and Koma (Phys Rev D 95(9), 094513, 2017) using hyperspherical variables. We find that: (1) the two sets of lattice results have only two common sets of 3-quark geometries: (a) the isosceles, and (b) the right-angled triangles; (2) both sets of results are subject to unaccounted for deviations from smooth curves that are largest near the equilateral triangle geometry and are function of the hyperradius – the deviations being much larger and extending further in the triangle shape space in Sakumichi and Suganuma’s than in Koma and Koma’s data; (3) the variation of Sakumichi and Suganuma’s results brackets, from above and below, the Koma and Koma’s ones; the latter will be used as the benchmark; (4) this benchmark result generally passes between the Y- and the $$\Delta $$ Δ -string predictions, thus excluding both; (5) three pieces of elastic strings joined at a skewed junction, which lies on the Euler line, reproduce such a potential, within the region where the data sets agree, in qualitative agreement with the calculations of colour flux density by Bissey et al. (Phys Rev D 76, 114512, 2007).https://doi.org/10.1140/epjc/s10052-021-08873-8 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
James Leech Milovan Šuvakov V. Dmitrašinović |
spellingShingle |
James Leech Milovan Šuvakov V. Dmitrašinović Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement? European Physical Journal C: Particles and Fields |
author_facet |
James Leech Milovan Šuvakov V. Dmitrašinović |
author_sort |
James Leech |
title |
Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement? |
title_short |
Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement? |
title_full |
Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement? |
title_fullStr |
Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement? |
title_full_unstemmed |
Hyperspherical variables analysis of lattice QCD three-quark potentials: skewed Y-string as the mechanism of confinement? |
title_sort |
hyperspherical variables analysis of lattice qcd three-quark potentials: skewed y-string as the mechanism of confinement? |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2021-01-01 |
description |
Abstract We have re-analysed the lattice QCD calculations of the 3-quark potentials by: (i) Sakumichi and Suganuma (Phys Rev D 92(3), 034511, 2015); and (ii) Koma and Koma (Phys Rev D 95(9), 094513, 2017) using hyperspherical variables. We find that: (1) the two sets of lattice results have only two common sets of 3-quark geometries: (a) the isosceles, and (b) the right-angled triangles; (2) both sets of results are subject to unaccounted for deviations from smooth curves that are largest near the equilateral triangle geometry and are function of the hyperradius – the deviations being much larger and extending further in the triangle shape space in Sakumichi and Suganuma’s than in Koma and Koma’s data; (3) the variation of Sakumichi and Suganuma’s results brackets, from above and below, the Koma and Koma’s ones; the latter will be used as the benchmark; (4) this benchmark result generally passes between the Y- and the $$\Delta $$ Δ -string predictions, thus excluding both; (5) three pieces of elastic strings joined at a skewed junction, which lies on the Euler line, reproduce such a potential, within the region where the data sets agree, in qualitative agreement with the calculations of colour flux density by Bissey et al. (Phys Rev D 76, 114512, 2007). |
url |
https://doi.org/10.1140/epjc/s10052-021-08873-8 |
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