Hyperon-nucleon potentials from lattice QCD
| dc.creator | Nemura, H. | |
| dc.creator | Ishii, N. | |
| dc.creator | Aoki, S. | |
| dc.creator | Hatsuda, T. | |
| dc.date | 2007-10-19 | |
| dc.date.accessioned | 2026-07-07T11:53:41Z | |
| dc.date.available | 2026-07-07T11:53:41Z | |
| dc.description | We calculate $pΞ^0$ potentials from the equal-time Bethe-Salpeter amplitude measured in the quenched QCD simulation with the spatial lattice volume, (4.4 fm)$^3$. The standard Wilson gauge action with the gauge coupling $β=5.7$ on $32^4$ lattice together with the standard Wilson quark action are used. The hopping parameter $κ_{ud}=0.1678$ is chosen for $u$ and $d$ quarks, which corresponds to $m_π\simeq 0.37$ GeV. The physical strange quark mass is used by taking the parameter $κ_s=0.1643$ which is deduced from the physical $K$ meson mass. The lattice spacing $a=0.1420$ fm is determined by the physical $ρ$ meson mass. We find that the $pΞ^0$ potential has strong spin dependence. Strong repulsive core is found in $^1S_0$ channel while the effective central potential in the $^3S_1$ channel has relatively weak repulsive core. The potentials also have weak attractive parts in the medium to long distance region (0.6 fm $\lsim r \lsim 1.2$ fm) in both of the $^1S_0$ and $^3S_1$ channels. | |
| dc.description | UTCCS-P-38, UT-554, TKYNT-07-16, 7pages, talk presented at the XXV International Symposium on Lattice Field Theory (Lattice 2007), 30 Jul - 4 Aug 2007, Regensburg, Germany | |
| dc.identifier | https://arxiv.org/abs/0710.3622 | |
| dc.identifier | http://arxiv.org/abs/0710.3622 | |
| dc.identifier | PoSLAT2007:156,2007 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/204628 | |
| dc.subject | High Energy Physics - Lattice | |
| dc.title | Hyperon-nucleon potentials from lattice QCD | |
| dc.type | text |