Strong Coupling of Pseudoscalar-Meson Octet

1966 ◽  
Vol 17 (1) ◽  
pp. 66-66 ◽  
Author(s):  
C. J. Goebel
1997 ◽  
Vol 50 (1) ◽  
pp. 95 ◽  
Author(s):  
C. J. Burden ◽  
L. Qian ◽  
C. D. Roberts ◽  
P. C. Tandy ◽  
M. J. Thomson

We present details of a model for calculating the mass spectrum of light-quark mesons and decay constants of the pseudoscalar meson octet from a phenomenological model based on Dyson–Schwinger and Bethe–Salpeter equations. In this model the Bethe-Salpeter kernel is approximated by a separable ansatz obtained from input quark propagators.


1942 ◽  
Vol 62 (3-4) ◽  
pp. 85-108 ◽  
Author(s):  
W. Pauli ◽  
S. M. Dancoff

1989 ◽  
Vol 04 (19) ◽  
pp. 1815-1825
Author(s):  
I.V. ANDREEV ◽  
M.M. TSYPIN

The effective Lagrangian for pseudoscalar meson octet including terms up to fourth order in momenta and masses is derived from a linear sigma model with vector and axial mesons. The mass of scalar meson nonet 720±75 MeV ensures a good fit of coefficients in effective Lagrangian with values derived from experiment.


2010 ◽  
Vol 835 (1-4) ◽  
pp. 346-349
Author(s):  
Toru T. Takahashi ◽  
Güray Erkol ◽  
Makoto Oka

2001 ◽  
Vol 51 (S2) ◽  
pp. B135-B144
Author(s):  
T. Fuchs ◽  
B. Pasquini ◽  
C. Unkmeir ◽  
S. Scherer

1990 ◽  
Vol 05 (29) ◽  
pp. 2457-2464 ◽  
Author(s):  
KIM MALTMAN ◽  
DAVID KOTCHAN

We investigate the chiral log corrections to the electromagnetic self-energies of the pseudoscalar meson octet and demonstrate that, for the charged pions and kaons, such corrections, at scales μ ~ 1 GeV , are large. We argue that this indicates that leading order chiral results may be misleading in the electromagnetic sector and discuss information on η → 3π and isospin breaking in Kl3 which support this interpretation.


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