BrokenSU 5 ×SU 5 chiral symmetry and heavy pseudoscalar mesons

1980 ◽  
Vol 29 (7) ◽  
pp. 207-213 ◽  
Author(s):  
S. Fajfer ◽  
Z. Stipčević
1969 ◽  
Vol 183 (5) ◽  
pp. 1463-1468 ◽  
Author(s):  
P. R. Auvil ◽  
N. G. Deshpande

1977 ◽  
Vol 39 (4) ◽  
pp. 554-569 ◽  
Author(s):  
G. J. Gounaris ◽  
S. B. Sarantakos

2001 ◽  
Vol 16 (17) ◽  
pp. 3011-3024 ◽  
Author(s):  
M. NAPSUCIALE ◽  
S. RODRIGUEZ

It is shown that most of the unusual properties of the lowest lying scalar (and pseudoscalar) mesons can be understood, at the qualitative and quantitative level, on the basis of the breakdown of the UA(1) symmetry coupled to the vacuum expectation values of scalars by the spontaneous breaking of chiral symmetry.


1984 ◽  
Vol 62 (5) ◽  
pp. 520-526 ◽  
Author(s):  
M. Hatzis

We consider broken SU(5) × SU(5) chiral symmetry and we assume that the vacuum is SU(5)-symmetric. Using the observed mass spectrum of pseudoscalar mesons, and setting the [Formula: see text] mass in the range 5.2 ± 0.06 GeV, we predict the masses of [Formula: see text], [Formula: see text], and ηb states as well as axial current couplings fi/fπ. SU(5) × SU(5) is found to be consistent with SU(4) × SU(4) breaking. The problem of η − η′ − ηe − ηb mixing is also discussed.


2008 ◽  
Vol 23 (22) ◽  
pp. 3493-3507
Author(s):  
XIAOYA LI ◽  
BIN WANG ◽  
XIAOZHAO CHEN ◽  
XIAOFU LÜ

The chiral effective Lagrangian for pseudoscalar meson nonet including eight Goldstone bosons and a SU (3) singlet η0is constructed with the breaking effect of chiral symmetry in both quark condensate and quark mass differences taken into account. The [Formula: see text] mixing is discussed. By solving the mass equations of pseudoscalar mesons, the quark mass ratios are obtained and the quark condensate ratios are constrained in ranges. The mass split of π0-π±is discussed.


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