2001
DOI: 10.1103/physrevd.64.036009
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Relativistic unitary description ofππscattering

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Cited by 9 publications
(7 citation statements)
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“…The coefficient a is chosen to reproduce the scattering length, which is small due to constraints from chiral symmetry [34,39]. The remainder of the denominator is chosen to provide crude agreement with measured phase shifts up to invariant masses of 1 GeV.…”
Section: Interdomain Correlationsmentioning
confidence: 99%
“…The coefficient a is chosen to reproduce the scattering length, which is small due to constraints from chiral symmetry [34,39]. The remainder of the denominator is chosen to provide crude agreement with measured phase shifts up to invariant masses of 1 GeV.…”
Section: Interdomain Correlationsmentioning
confidence: 99%
“…The I=0 channel is particularly important as it corresponds to the mythical meson. Although phase shift analyses do not reveal a sharp peak as in a resonance [30][31][32][33][34], the phase shifts are considerable, rising steadily from zero at threshold to Ϸ90°at M =2M K ϳ1 GeV, where the kaon channel opens. At the two-kaon threshold, the behavior of the phase shifts becomes complicated and an inelastic treatment becomes warranted.…”
Section: ͑10͒mentioning
confidence: 99%
“…Accordingly, π-π scattering has attracted considerable interest even though the cross section is not directly measurable. In particular, a variety of theories have been utilized to make scattering predictions: at low energies, current algebra/PCAC [1], chiral perturbation theory [2,3,4,5] and bosonization models with pion fields [6]; Quantum Hadrodynamic [QHD] meson exchange models and unitarized relativistic coupled channels [7] for intermediate energies; Regge theory at moderately higher energies; perturbative QCD at very high energies. These in turn have been confronted by experimental phase shift analyses [8,9,10,11] yielding reasonable agreement.…”
Section: Introductionmentioning
confidence: 99%