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The presence of extra P11 resonances in Zagreb analysis since 1995. A. Švarc, S. Ceci and B. Zauner Rudjer Bošković Institute Zagreb. Definition of the Zagreb model. CMU-LBL formalism. Formalism:.
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The presence of extra P11 resonances in Zagreb analysis since 1995 A. Švarc, S. Ceci and B. Zauner Rudjer Bošković Institute Zagreb
Definition of the Zagreb model CMU-LBL formalism
GENERAL AGREEMENT the number of resonances directly corresponds to the number of poles of the Green function in the CMU_LBL formalism PROBLEM: resonance identification
The input for the Zagreb model 1. pion elastic channel : partial T-matrices (KH-80+SM85) 2. eta-production channel:DATA BASE 3. number of Green function poles per partial wave
The criterion of acceptancethe best chi-square fitgeneral acceptability
Number of Green function poles required by the Zagreb PWA(possible solutions) S11: three poles in the Green function (the same as PDG) P11: a. three poles in the Green function b. four poles in the Green function
The model with four polesBatinic et al. Physica Scripta 58 (1998) 15black line The model with three poles Batinic et al. Phys. Rev C51 (1995) 231 red line
The best obtained chi-square/data pointthree poles model: 1.522four poles model: 1.301
0.4 0.8 0.2 0.6 0 0.4 - 0.2 0.2 - 0.4 0 1500 2000 2500 3000 1500 2000 2500 3000
0.6 0.1 0.5 0.05 0.4 0 0.3 - 0.05 0.2 - 0.1 0.1 - 0.15 0 1500 2000 2500 3000 1500 2000 2500 3000
CONCLUSIONS 1. We obtain two solutions, with three and four poles respectively, which to the precision of the input data equally well reproduce and channels 2. The three resonant solution does not give any significan branching ratio to the channel so we prefere a four resonance solution 3. We do not claim that such a three resonant solution does not exist, we simply claim that at the present moment we have no means to find it
The solutionWe are developing the general purposse code(GPC)