f_{2}(1270),$ $a_{1}(1260)$ and $f_{0}(1370)$ as dynamically reconstructed quark-antiquark states

Details f_{2}(1270),$ $a_{1}(1260)$ and $f_{0}(1370)$ as dynamically reconstructed quark-antiquark states f_{2}(1270),$ $a_{1}(1260)$ and $f_{0}(1370)$ as dynamically reconstructed quark-antiquark states

2010-10-05

arxiv.org/abs/1010.1021v1

AIP Conf.Proc.1322:223-231,2010

Physics

High Energy Physics

High Energy Physics - Phenomenology

8 pages, 2 figures. Based on the contribution given at the Chiral10 Workshop, Valencia (Spain), June 21-24, 2010

Scientific paper

10.1063/1.3541985

It is explained why the interpretation of the resonances $f_{2}(1270),$
$a_{1}(1260)$ and $f_{0}(1370)$ as quark-antiquark states is legitimate. The
result of the quark model and of recently performed Bethe-Salpeter studies are
not (necessarily) in conflict and can be understood as two different approaches
toward the description of the same quark-antiquark resonances.

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