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Related papers: Extraction of P11 resonances from pi N data

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We study the stability of resonance poles in pi-N P_11 partial wave, particularly the Roper resonance, by varying parameters significantly within the EBAC dynamical coupled-channels model, keeping a good fit to the empirical amplitude. We…

Nuclear Theory · Physics 2015-05-28 S. X. Nakamura

We address a question about how much resonance poles and residues extracted from data depend on a model used for the extraction, and on the precision of data. We focus on the P11 pi-N scattering and use the dynamical coupled-channel (DCC)…

Nuclear Theory · Physics 2015-05-20 S. X. Nakamura

An important question about resonance extraction is how much resonance poles and residues extracted from data depend on a model used for the extraction, and on the precision of data. We address this question with the dynamical…

Nuclear Theory · Physics 2011-09-30 S. X. Nakamura , H. Kamano , T. -S. H. Lee , T. Sato

We extract pole positions for the N(1535) and N(1650) resonances using two different models. The positions are determined from fits to different subsets of the existing $\pi N\to\pi N$, $\pi N\to\eta N$ and $\gamma p\to\eta p$ data and…

Nuclear Theory · Physics 2008-11-26 R. A. Arndt , A. M. Green , R. L. Workman , S. Wycech

We present a pedagogical study of the commonly employed Speed-Plot (SP) and Time-delay (TD) methods for extracting the resonance parameters from the data of two particle coupled-channels reactions. Within several exactly solvable models, it…

Nuclear Theory · Physics 2009-03-04 N. Suzuki , T. Sato , T. -S. H. Lee

Low-energy partial-wave $\pi N$ scattering data is reexamined with the help of the production representation of partial-wave $S$ matrix, where branch cuts and poles are thoroughly under consideration. The left-hand cut contribution to the…

High Energy Physics - Phenomenology · Physics 2019-01-01 Yu-Fei Wang , De-Liang Yao , Han-Qing Zheng

The partial wave T-matrices for the pi N, eta N and pi2 N channels have been obtained within the framework of the coupled channel model using the pi N elastic and pi N --> eta N data base as input. It has been shown that for the P11 partial…

Nuclear Theory · Physics 2017-08-23 S. Ceci , A. Svarc , B. Zauner

Within the previously developed Dubna-Mainz-Taipei meson-exchange model, the singularity structure of the pi N scattering amplitudes has been investigated. For all partial waves up to F waves and c.m. energies up to W = 2 GeV, the T-matrix…

Nuclear Theory · Physics 2010-12-02 L. Tiator , S. S. Kamalov , S. Ceci , G. Y. Chen , D. Drechsel , A. Svarc , S. N. Yang

The phase shift of pion nucleon elastic scattering D33, corresponding to isospin I=3/2 and angular momentum J=3/2, has been parameterized over the range 1100 < W < 1375 MeV, using the single channel p Pi+ data from CNS-DAC. By employing our…

Nuclear Theory · Physics 2007-05-23 Mohamed E. Kelabi

We show that two almost degenerate poles near the $\pi\Delta$ threshold and the next higher mass pole in the $P_{11}$ partial wave of $\pi N$ scattering evolve from a single bare state through its coupling with $\pi N$, $\eta N$ and $\pi\pi…

Nuclear Theory · Physics 2010-04-06 N. Suzuki , B. Julia-Diaz , H. Kamano , T. -S. H. Lee , A. Matsuyama , T. Sato

A unitary multi-channel approach, first developed by the Carnegie-Mellon- Berkeley group, is applied to extract the pole positions, masses, and partial decay widths of nucleon resonances. Input used are the partial wave amplitudes for the…

Nuclear Theory · Physics 2008-11-26 T. P. Vrana , S. A. Dytman , T. -S. H. Lee

The nucleon resonances are investigated within a dynamical coupled-channels model of pi N and gamma N reactions up to the invariant mass W = 2 GeV. The meson-baryon (MB) channels included in the calculations are MB = pi N, eta N, K Lambda,…

Nuclear Theory · Physics 2013-09-30 H. Kamano , S. X. Nakamura , T. -S. H. Lee , T. Sato

A new partial wave analysis of pion photoproduction has been obtained in the framework of fixed-t dispersion relations valid form threshold up to 500 MeV. It is based on new Mainz data for \pi^{0} and \pi^{+} production off the proton and…

Nuclear Theory · Physics 2011-04-15 L. Tiator

Data on the reaction $\gamma p\to K^+\Lambda$ from the CLAS experiments are used to derive the leading multipoles, $E_{0+}$, $M_{1-}$, $E_{1+}$, and $M_{1+}$, from the production threshold to 2180\,MeV in 24 slices of the invariant mass.…

Properties of the Roper resonance, the first scalar excitation of the nucleon, are determined. Pole positions and residues of the $P_{11}$ partial wave are studied in a combined analysis of pion- and photo-induced reactions. We find the…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. V. Sarantsev

We have performed a dynamical coupled-channels analysis of available p(e,e'pi)N data in the region of W < 1.6 GeV and Q^2 < 1.45 (GeV/c)^2. The channels included are gamma^* N, pi N, eta N, and pi pi N which has pi Delta, rho N, and sigma N…

Nuclear Theory · Physics 2009-09-01 B. Julia-Diaz , H. Kamano , T. -S. H. Lee , A. Matsuyama , T. Sato , N. Suzuki

Properties of scalar--isoscalar mesons in a mass range from pi-pi threshold up to 1800 MeV are analysed using an unitary model with separable interactions in three decay channels: pi-pi, K-anti K and an effective 2pi-2pi. Different…

High Energy Physics - Phenomenology · Physics 2007-05-23 R. Kamiński , L. Leśniak , B. Loiseau

We report our recent effort for the extraction of resonance parameters (complex pole mass and residues etc.) associated with Lambda* and Sigma* hyperons. This was accomplished via a comprehensive partial-wave analysis of the data for K^- p…

Nuclear Theory · Physics 2017-08-02 Hiroyuki Kamano

We present results on the electroexcitation of the low mass resonances Delta(1232)P33, N(1440)P11, N(1520)D13, and N(1535)S11 in a wide range of Q2. The results were obtained in the comprehensive analysis of JLab-CLAS data on differential…

Nuclear Experiment · Physics 2010-04-06 I. G. Aznauryan , V. D. Burkert , the CLAS Collaboration

We analyze Pion Nucleon Scattering up to 700 MeV using a simple, relativistic, unitary model\cite{1}. The kernel of the integral equation includes nucleon, roper, delta, D_13 as well as S_11 poles with their corresponding crossed pole terms…

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