Pion-pion scattering amplitude. II. Improved analysis above K̅K threshold

dc.contributor.authorKamiński, R
dc.contributor.authorPeláez Sagredo, José Ramón
dc.contributor.authorYnduráin, F. J.
dc.date.accessioned2023-06-20T11:06:55Z
dc.date.available2023-06-20T11:06:55Z
dc.date.issued2006-07
dc.description©2006 The American Physical Society. The work of F. J. Y. was supported in part by the Spanish DGI of the MEC under Contract No. FPA2003-04597. The research of J. R. P. is partially funded by Spanish CICYT Contracts No. FPA2005-02327 and BFM2003-00856, as well as Banco Santander/Complutense Contract No. PR27/ 05-13955-BSCH, and is part of the EU integrated infrastructure initiative HADRONPHYSICS PROJECT, under Contract No. RII3-CT-2004-506078. Finally, R. Kaminski thanks the Complutense University of Madrid for a grant under the Foreign Doctor Visit Program and the Departamento de Física Teórica II, where most of his research was carried out.
dc.description.abstractWe improve, in the energy region between the K̅K threshold and ~ 1.4 GeV, the energy-dependent phase shift analysis of π π scattering presented in a previous paper. For the S0 wave, we have included more data above the K̅K threshold and we have taken into account systematically the elasticity data on the reaction π π →K̅K. We here made a coupled channel fit. For the D0 wave, we have considered information on low energy parameters, and imposed a better fit to the f_2 resonance. For both waves the expressions we now find are substantially more precise than the previous ones. We also provide slightly improved D2 and P waves, including the estimated inelasticity for the first, and a more flexible parametrization between 1 and 1.42 GeV for the second. The accuracy of our amplitudes is now such that it requires a refinement of the Regge analysis, for^(1/2) ≥ 1.42 GeV, which we also carry out. We show that this more realistic input produces π π scattering amplitudes that satisfy better forward dispersion relations, particularly for π^0 π^0 scattering.
dc.description.departmentDepto. de Física Teórica
dc.description.facultyFac. de Ciencias Físicas
dc.description.refereedTRUE
dc.description.sponsorshipSpanish DGI of the MEC
dc.description.sponsorshipSpanish CICYT
dc.description.sponsorshipBanco Santander/Complutense
dc.description.sponsorshipEU Integrated Infrastructure Initiative HADRONPHYSICS PROJECT
dc.description.statuspub
dc.eprint.idhttps://eprints.ucm.es/id/eprint/35370
dc.identifier.doi10.1103/PhysRevD.74.014001
dc.identifier.issn1550-7998
dc.identifier.officialurlhttp://dx.doi.org/10.1103/PhysRevD.74.014001
dc.identifier.relatedurlhttp://journals.aps.org
dc.identifier.urihttps://hdl.handle.net/20.500.14352/51727
dc.issue.number1
dc.journal.titlePhysical review D
dc.language.isoeng
dc.publisherAmer Physical Soc
dc.relation.projectIDFPA2003-04597
dc.relation.projectIDFPA2005-02327
dc.relation.projectIDBFM2003-00856
dc.relation.projectIDPR27/ 05-13955-BSCH,
dc.relation.projectIDRII3-CT-2004-506078
dc.rights.accessRightsopen access
dc.subject.cdu51-73
dc.subject.keywordPhase-shift analysis
dc.subject.keywordGev-c
dc.subject.keywordπ-P->π π&N
dc.subject.ucmFísica-Modelos matemáticos
dc.subject.ucmFísica matemática
dc.titlePion-pion scattering amplitude. II. Improved analysis above K̅K threshold
dc.typejournal article
dc.volume.number74
dcterms.references[1] J. R. Peláez and F. J. Ynduráin, Phys. Rev. D 71, 074016 (2005). [2] B. Hyams et al., Nucl. Phys. B64, 134 (1973); see also the analysis of the same experimental data in P. Estabrooks and A. D. Martín, Nucl. Phys. B79, 301 (1974). [3] G. Grayer et al., Nucl. Phys. B75, 189 (1974). [4] S. D. Protopopescu et al., Phys. Rev. D 7, 1279 (1973). [5] R. Kamiński, L. Lesniak, and K. Rybicki, Z. Phys. C 74, 79 (1997); Eur. Phys. J. direct C 4, 4 (2002). [6] B. Hyams et al., Nucl. Phys. B100, 205 (1975). [7] π π →K̅K scattering: W. Wetzel et al., Nucl. Phys. B115, 208 (1976); D. Cohen et al., Phys. Rev. D 22, 2595 (1980); E. Etkin et al., Phys. Rev. D 25, 1786 (1982). [8] PDT: S. Eidelman et al., Phys. Lett. B 592, 1 (2004). [9] F. Q. Wu et al., Nucl. Phys. A B735, 111 (2004). [10] J. F. de Troco´niz and F. J. Ynduráin, Phys. Rev. D 65, 093001 (2002); 71, 073008 (2005). [11] J. R. Peláez and F. J. Ynduráin, Phys. Rev. D 69, 114001 (2004). [12] K. Adel, F. Barreiro, and F. J. Ynduráin, Nucl. Phys. B495, 221 (1997). [13] W. Rarita et al., Phys. Rev. 165, 1615 (1968). [14] J. R. Cudell et al., Phys. Lett. B 587, 78 (2004); J. R. Peláez, Proceedings of the 11th Conference on Elastic and Diffractive Scattering, Blois, France, May, 2005 (hep-ph/ 0510005). Note, however, that the first reference fits data for π N and NN, but not for π π, and only for energies above ~ 4 GeV; while the last article contains only preliminary results and, indeed, the parameters for exchange of isospin zero are not well determined. [15] J. R. Peláez and F. J. Ynduráin, Phys. Rev. D 68, 074005 (2003); J. R. Pelaáez and F. J. Ynduráin, AIP Conf. Proc. 756, 48 (2005); J. R. Peláez and F. J. Ynduráin, in Proceedings of the 2005 Montpelier Conference (hep-ph/ 0510216, to be published). [16] H. Pilkuhn, The Interaction of Hadrons (North- Holland, Amsterdam, 1967). [17] F. J. Ynduráin, hep-ph/0212282; see also F. J. Ynduráin, Phys. Lett. B 612, 245 (2005).
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relation.isAuthorOfPublication70900239-cb8b-49f3-931f-9dc6a8b7d8d5
relation.isAuthorOfPublication.latestForDiscovery70900239-cb8b-49f3-931f-9dc6a8b7d8d5

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