Light hadron spectroscopy on the lattice with the non-perturbatively improved Wilson action
| dc.creator | Becirevic, D. | |
| dc.creator | Boucaud, Ph. | |
| dc.creator | Giusti, L. | |
| dc.creator | Leroy, J. P. | |
| dc.creator | Lubicz, V. | |
| dc.creator | Martinelli, G. | |
| dc.creator | Mescia, F. | |
| dc.creator | Rapuano, F. | |
| dc.date | 1998-09-16 | |
| dc.date.accessioned | 2026-07-07T03:40:08Z | |
| dc.date.available | 2026-07-07T03:40:08Z | |
| dc.description | We present results for the light meson masses and decay constants as obtained from calculations with the non-perturbatively improved (`Alpha') action and operators on a 24^3 \times 64 lattice at beta = 6.2, in the quenched approximation. The analysis was performed in a way consistent with O(a) improvement. We obtained: reasonable agreement with experiment for the hyperfine splitting; f_K=156(17) MeV, f_pi =139(22) MeV, f_K/f_pi = 1.13(4) ; f_{K*}=219(7) MeV, f_rho =199(15) MeV, f_phi =235(4) MeV; f_{K*}^{T}(2 GeV) = 178(10) MeV, f_rho^{T}(2 GeV) =165(11) MeV, where f_V^{T} is the coupling of the tensor current to the vector mesons; the chiral condensate <\bar{q}q>^\bar{MS} (2 GeV)= - (253 +/- 25 MeV)^3. Our results are compared to those obtained with the unimproved Wilson action. We also verified that the free-boson lattice dispersion relation describes our results very accurately for a large range of momenta. | |
| dc.description | 29 pages (LaTeX), 14 Postscript figures | |
| dc.identifier | https://arxiv.org/abs/hep-lat/9809129 | |
| dc.identifier | http://arxiv.org/abs/hep-lat/9809129 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/39165 | |
| dc.subject | High Energy Physics - Lattice | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | Light hadron spectroscopy on the lattice with the non-perturbatively improved Wilson action | |
| dc.type | text |