TY - JOUR
T1 - Narrow or wide resonance?
AU - Mart, Terry
N1 - Publisher Copyright:
© Copyright owned by the author(s) under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike Licence.
PY - 2013
Y1 - 2013
N2 - We have investigated the existence of the Jp = 1/2+ (P11) narrow resonance predicted by the chiral soliton model. For this purpose we used an isobar model developed for explaining the kaon photoproduction process. It was found that the most possible narrow resonance has a mass of 1650 MeV and a width of 5 MeV. This finding is, however, different from that obtained in the ηphotoproduction off a neutron, where the extracted mass and width are relatively larger, i.e. 1680 and 30 MeV, respectively. We have revisited the calculation by considering a wider resonance width and using the latest covariant isobar model. The result still indicates the existence of the narrow resonance with the mass of 1650 MeV, but the best agreement between experimental data and model prediction could be achieved by using the resonance mass and width of 1690 and 75 MeV, respectively. However, the possibly small N∗(1710)P11 coupling constant would constrain the mass and width to be . 1680 and . 35 MeV, respectively.
AB - We have investigated the existence of the Jp = 1/2+ (P11) narrow resonance predicted by the chiral soliton model. For this purpose we used an isobar model developed for explaining the kaon photoproduction process. It was found that the most possible narrow resonance has a mass of 1650 MeV and a width of 5 MeV. This finding is, however, different from that obtained in the ηphotoproduction off a neutron, where the extracted mass and width are relatively larger, i.e. 1680 and 30 MeV, respectively. We have revisited the calculation by considering a wider resonance width and using the latest covariant isobar model. The result still indicates the existence of the narrow resonance with the mass of 1650 MeV, but the best agreement between experimental data and model prediction could be achieved by using the resonance mass and width of 1690 and 75 MeV, respectively. However, the possibly small N∗(1710)P11 coupling constant would constrain the mass and width to be . 1680 and . 35 MeV, respectively.
UR - http://www.scopus.com/inward/record.url?scp=85019507237&partnerID=8YFLogxK
M3 - Conference article
AN - SCOPUS:85019507237
SN - 1824-8039
JO - Proceedings of Science
JF - Proceedings of Science
T2 - 15th International Conference on Hadron Spectroscopy, Hadron 2013
Y2 - 4 November 2013 through 8 November 2013
ER -