$K^{+}\toπ^{+}π^{0}$ decays at next-to-leading order in the chiral expansion on finite volumes
| dc.creator | Lin, C. -J. D. | |
| dc.creator | Martinelli, G. | |
| dc.creator | Pallante, E. | |
| dc.creator | Sachrajda, C. T. | |
| dc.creator | Villadoro, G. | |
| dc.date | 2002-09-03 | |
| dc.date.accessioned | 2026-07-07T11:08:53Z | |
| dc.date.available | 2026-07-07T11:08:53Z | |
| dc.description | We present the ingredients for determining $K^{+}\toπ^{+}π^{0}$ matrix elements via the combination of lattice QCD and chiral perturbation theory ($χ$PT). By simulating these matrix elements at unphysical kinematics, it is possible to determine all the low-energy constants (LECs) for constructing the physical $K^{+}\toπ^{+}π^{0}$ amplitudes at next-to-leading order (NLO) in the chiral expansion. In this work, the one-loop chiral corrections are calculated for arbitrary meson four-momenta, in both $χ$PT and quenched $χ$PT (q$χ$PT), and the finite-volume effects are studied. | |
| dc.description | Lattice 2002 (matrixel). 3 pages, 2 figures | |
| dc.identifier | https://arxiv.org/abs/hep-lat/0209020 | |
| dc.identifier | http://arxiv.org/abs/hep-lat/0209020 | |
| dc.identifier | Nucl.Phys.Proc.Suppl.119:383-385,2003 | |
| dc.identifier | doi:10.1016/S0920-5632(03)01561-5 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/190287 | |
| dc.subject | High Energy Physics - Lattice | |
| dc.subject | High Energy Physics - Phenomenology | |
| dc.title | $K^{+}\toπ^{+}π^{0}$ decays at next-to-leading order in the chiral expansion on finite volumes | |
| dc.type | text |