Erratum: Low-energy technicolor Lagrangian with vector mesons

1991 ◽  
Vol 44 (1) ◽  
pp. 302-302
Author(s):  
Robert Johnson ◽  
Bing-Lin Young ◽  
Douglas W. McKay
Keyword(s):  
1990 ◽  
Vol 42 (11) ◽  
pp. 3855-3865 ◽  
Author(s):  
Robert Johnson ◽  
Bing Lin Young ◽  
Douglas W. McKay
Keyword(s):  

1962 ◽  
Vol 25 (5) ◽  
pp. 1008-1016
Author(s):  
E. Kazes
Keyword(s):  

1972 ◽  
Vol 5 (3) ◽  
pp. 276-280
Author(s):  
G. Fiorenrini

2009 ◽  
Vol 18 (02) ◽  
pp. 253-260
Author(s):  
◽  
K. SCHÖNNING ◽  
H. CALÉN ◽  
K. FRANSSON ◽  
B. HÖISTAD ◽  
...  

The tensor polarization of ω mesons produced in the pd → 3 He ω reaction has been measured at two energies near threshold. The 3 He nuclei were detected in coincidence with the π0π+π- or π0γ decay products of the ω. The ω mesons are found to be unpolarised, which is in complete contrast to the case of ϕ-meson production from the corresponding reaction pd → 3 He ϕ. This brings into question the applicability of the Okubo-Zweig-Iizuka rule when comparing the production of vector mesons in low energy hadronic reactions.


2011 ◽  
Vol 703 (4) ◽  
pp. 504-509 ◽  
Author(s):  
I.V. Danilkin ◽  
L.I.R. Gil ◽  
M.F.M. Lutz

2018 ◽  
Vol 27 (01) ◽  
pp. 1850001 ◽  
Author(s):  
Tochtli Yépez-Martínez ◽  
Osvaldo Civitarese ◽  
Peter Otto Hess

The low-energy sector of the mesonic spectrum exhibits some features which may be understood in terms of the SO(4) symmetry contained in the QCD-Hamiltonian written in the Coulomb Gauge. In our previous work, we have shown that this is indeed the case when the Instantaneous Color-Charge Interaction (ICCI) is treated by means of nonperturbative many-body techniques. Continuing along this line of description, in this work we calculate the width of meson states belonging to the low portion of the spectrum ([Formula: see text] GeV). In spite of the rather simple structure of the Hamiltonian used to calculate the spectra of pseudoscalar and vector mesons, the results for the width of these states follow the pattern of the data.


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