Quark loop model of radiative meson decays

1979 ◽  
Vol 2 (1) ◽  
pp. 23-28 ◽  
Author(s):  
Norma M. Chase ◽  
Michael T. Vaughn

1976 ◽  
Vol 61 (2) ◽  
pp. 175-177 ◽  
Author(s):  
N. Chase ◽  
M.T. Vaughn


1973 ◽  
Vol 8 (11) ◽  
pp. 3875-3881 ◽  
Author(s):  
Steven B. Berger ◽  
Bernard T. Feld


1989 ◽  
Author(s):  
Milton Dean Slaughter ◽  
S. Oneda


2001 ◽  
Author(s):  
Aldo Deandrea
Keyword(s):  


1971 ◽  
Vol 1 (1) ◽  
pp. 30-32 ◽  
Author(s):  
A. Esteve ◽  
J. León ◽  
A. Tiemblo


1999 ◽  
Vol 14 (27) ◽  
pp. 4331-4345 ◽  
Author(s):  
R. DELBOURGO ◽  
DONGSHENG LIU ◽  
M. D. SCADRON

We show that all abnormal parity three-body meson interactions can be adequately described by quark loops, evaluated at zero external momentum, with couplings determined by U(Nf) symmetry. We focus primarily on radiative meson decays which involve one pseudoscalar. The agreement with experiment for nonrare decays is surprisingly good and requires very few parameters, namely the coupling constants gπqq and gρqq and some mixing angles. This agreement extends to some three-body decays that are dominated by pion pairs in a P-wave state.



1968 ◽  
Vol 39 (3) ◽  
pp. 696-701 ◽  
Author(s):  
Akira Kanazawa ◽  
Tetsuro Sakuma


1970 ◽  
Vol 68 (3) ◽  
pp. 459-468 ◽  
Author(s):  
D. F. Greenberg


1971 ◽  
Vol 1 (4) ◽  
pp. 174-174
Author(s):  
A. Esteve ◽  
J. León ◽  
A. Tiemblo


1976 ◽  
Vol 54 (2) ◽  
pp. 158-163 ◽  
Author(s):  
L. Resnick ◽  
J. H. Kim

The weak decay of pions into leptons and into leptons plus photon is examined in a simple model at the one loop level. A basic assumption made is that there is more than one pair of quarks to which the pion couples and the masses and coupling constants are such that all amplitudes are finite. The amplitudes are defined by means of dimensional regularization and gauge invariance is rigorously maintained throughout. The experimental lifetimes for charged and neutral pion decay give one constraint among the quark masses and the parameter γ, the ratio of structure dependent axial to vector form factor, gives a second. Quark masses can be found to satisfy either condition, but no solution exists for both constraints simultaneously.



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