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An Analysis of -Scattering Phase Shift and Existence of (555) Particle
Author(s) -
S. Ishida,
M. Ishida,
H. Takahashi,
Takashi Ishida,
K. Takamatsu,
T. Tsuru
Publication year - 1996
Publication title -
progress of theoretical physics
Language(s) - English
Resource type - Journals
eISSN - 1347-4081
pISSN - 0033-068X
DOI - 10.1143/ptp.95.745
Subject(s) - physics , unitarity , amplitude , phase (matter) , goldstone boson , scalar (mathematics) , boson , particle physics , quantum electrodynamics , quantum mechanics , geometry , mathematics
In most of the Nambu:Jona-Lasinio(NJL)-type models, realizing the hiddenchiral symmetry, the existence of a scalar particle \sigma is needed with amass m_\sigma=2 m_q, as a partner of the Nambu-Goldstone boson \pi. However,the results of many analyses on \pi\pi phase-shift thus far made have beennegative for its existence. In this paper we re-analyze the phase-shift,applying a new method, the interfering amplitude method, which treats theT-matrix directly and describes multi-resonances in conformity with theunitarity. As a result, the existence of \sigma has been strongly suggestedfrom the behavior of the \pi\pi-->\pi\pi phase shift between the \pi\pi- andthe KK- thresholds, with mass = 553.3 +- 0.5_{st} MeV and width= 242.6 +-1.2_{st} MeV. The most crucial point in our analysis is the introduction of anegative background phase, possibly reflecting a ``repulsive core" in \pi\piinteractions. The properties of f_0(980) are also investigated from dataincluding those over the KK threshold. Its mass is obtained as 993.2 +-6.5_{st} +- 6.9_{sys} MeV. Its width is about a hundred MeV, although thisdepends largely on the treatment of the elasticity and the \pi\pi-->KK phaseshift, both of which may have large experimental uncertainties.Comment: 22 pages, Latex with Prog. Theor. Phys. format PTPTEX.sty, 4 EPS figure

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