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Title: Joint description of the e{sup +}e{sup -} annihilation into both four-pion channels

Abstract

The e{sup +}e{sup -}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0}{pi}{sup 0} reaction cross section as a function of the incident energy is calculated using a model that is an extension of our recently published model of the e{sup +}e{sup -} annihilation into four charged pions. The latter considered the intermediate states with the {pi}, {rho}, and a{sub 1} mesons and fixed the mixing angle of the a{sub 1}{rho}{pi} Lagrangian and other parameters by fitting the cross section data. Here we supplement the original intermediate states with those containing {omega}(782) and h{sub 1}(1170), but keep unchanged the values of those parameters that enter both charged and mixed channel calculations. The inclusion of {omega} is vital for obtaining a good fit to the cross section data, while the intermediate states with h{sub 1} further improve it. Finally, we merge our models of the e{sup +}e{sup -}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0}{pi}{sup 0} and e{sup +}e{sup -}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup +}{pi}{sup -} reactions and obtain a simultaneous good fit.

Authors:
 [1];  [1]
  1. Institute of Physics, Silesian University in Opava, Bezrucovo namesti 13, 746 01 Opava (Czech Republic)
Publication Date:
OSTI Identifier:
21250288
Resource Type:
Journal Article
Journal Name:
Physical Review. D, Particles Fields
Additional Journal Information:
Journal Volume: 78; Journal Issue: 1; Other Information: DOI: 10.1103/PhysRevD.78.017501; (c) 2008 The American Physical Society; Country of input: International Atomic Energy Agency (IAEA); Journal ID: ISSN 0556-2821
Country of Publication:
United States
Language:
English
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS; ANNIHILATION; CHARGED-PARTICLE REACTIONS; COMPUTERIZED SIMULATION; CROSS SECTIONS; H1-1170 MESONS; INTERMEDIATE STATE; LAGRANGIAN FUNCTION; OMEGA-782 MESONS; PARTICLE DECAY; PIONS MINUS; PIONS NEUTRAL; PIONS PLUS; WEINBERG ANGLE

Citation Formats

Juran, Josef, Lichard, Peter, and Institute of Experimental and Applied Physics, Czech Technical University, Horska 3/a, 120 00 Prague. Joint description of the e{sup +}e{sup -} annihilation into both four-pion channels. United States: N. p., 2008. Web. doi:10.1103/PHYSREVD.78.017501.
Juran, Josef, Lichard, Peter, & Institute of Experimental and Applied Physics, Czech Technical University, Horska 3/a, 120 00 Prague. Joint description of the e{sup +}e{sup -} annihilation into both four-pion channels. United States. https://doi.org/10.1103/PHYSREVD.78.017501
Juran, Josef, Lichard, Peter, and Institute of Experimental and Applied Physics, Czech Technical University, Horska 3/a, 120 00 Prague. 2008. "Joint description of the e{sup +}e{sup -} annihilation into both four-pion channels". United States. https://doi.org/10.1103/PHYSREVD.78.017501.
@article{osti_21250288,
title = {Joint description of the e{sup +}e{sup -} annihilation into both four-pion channels},
author = {Juran, Josef and Lichard, Peter and Institute of Experimental and Applied Physics, Czech Technical University, Horska 3/a, 120 00 Prague},
abstractNote = {The e{sup +}e{sup -}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0}{pi}{sup 0} reaction cross section as a function of the incident energy is calculated using a model that is an extension of our recently published model of the e{sup +}e{sup -} annihilation into four charged pions. The latter considered the intermediate states with the {pi}, {rho}, and a{sub 1} mesons and fixed the mixing angle of the a{sub 1}{rho}{pi} Lagrangian and other parameters by fitting the cross section data. Here we supplement the original intermediate states with those containing {omega}(782) and h{sub 1}(1170), but keep unchanged the values of those parameters that enter both charged and mixed channel calculations. The inclusion of {omega} is vital for obtaining a good fit to the cross section data, while the intermediate states with h{sub 1} further improve it. Finally, we merge our models of the e{sup +}e{sup -}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup 0}{pi}{sup 0} and e{sup +}e{sup -}{yields}{pi}{sup +}{pi}{sup -}{pi}{sup +}{pi}{sup -} reactions and obtain a simultaneous good fit.},
doi = {10.1103/PHYSREVD.78.017501},
url = {https://www.osti.gov/biblio/21250288}, journal = {Physical Review. D, Particles Fields},
issn = {0556-2821},
number = 1,
volume = 78,
place = {United States},
year = {Tue Jul 01 00:00:00 EDT 2008},
month = {Tue Jul 01 00:00:00 EDT 2008}
}