The reactions π-p →ηn and γ'p →ηP are investigated within a dynamical coupledJchannels model of meson production reactions in the nucleon resonance region. The meson-baryon channels included are πN, ηN, π△,...The reactions π-p →ηn and γ'p →ηP are investigated within a dynamical coupledJchannels model of meson production reactions in the nucleon resonance region. The meson-baryon channels included are πN, ηN, π△, σN, and pN. The direct wphotoproduction process is studied within a formalism based on a chiral constituent quark model approach, complemented with a one-gluon-exchange mechanism, to take into account the breakdown of the SU(6)0(3) symmetry. In the models search, the following known nucleon resonances are embodied: Sll (1535), $11(1650), Pll (1440), Pl1(1710), P13(1720), D13(1520), D13(1700), D15(1675), and F15(1680). Data for the π-p →ηnreaction from threshold up to a total center-of-mass energy of W ≈ 2 GeV are satisfactorily reproduced. For the photoproduction channel, two additional higher mass known resonances, P13 (1900) and F15 (2000), are also considered. However, reproducing the data for γ'p →ηP requires, within our approach, two new nucleon resonances, for which we extract mass and width.展开更多
基金Supported by a CPAN CSD 2007-0042 contract, Consolider Ingenio 2010 and by grants No. FIS2008-01661 and 2009SGR-1289
文摘The reactions π-p →ηn and γ'p →ηP are investigated within a dynamical coupledJchannels model of meson production reactions in the nucleon resonance region. The meson-baryon channels included are πN, ηN, π△, σN, and pN. The direct wphotoproduction process is studied within a formalism based on a chiral constituent quark model approach, complemented with a one-gluon-exchange mechanism, to take into account the breakdown of the SU(6)0(3) symmetry. In the models search, the following known nucleon resonances are embodied: Sll (1535), $11(1650), Pll (1440), Pl1(1710), P13(1720), D13(1520), D13(1700), D15(1675), and F15(1680). Data for the π-p →ηnreaction from threshold up to a total center-of-mass energy of W ≈ 2 GeV are satisfactorily reproduced. For the photoproduction channel, two additional higher mass known resonances, P13 (1900) and F15 (2000), are also considered. However, reproducing the data for γ'p →ηP requires, within our approach, two new nucleon resonances, for which we extract mass and width.
基金Supported by U.S. Department of Energy, Office of Nuclear Physics Division(DE-AC02-06CH11357, DE-AC05-06OR23177)under which Jefferson Science Associates operates Jefferson Lab
文摘A summary of the contributions to this workshop is given. The status and future development of N* physics are discussed.