Abstract
We investigate the isospin breaking in the ${\chi _{c1}} \to {\pi ^0}{\pi ^ + }{\pi ^ - }$ and ${\chi _{c1}} \to {\pi ^0}{\pi ^0}\eta $ decays and its relation to the a0(980) – f0(980) mixing, which was measured by the BESIII Collaboration. The isospin violation is introduced through the use of different masses for the charged and neutral kaons, either in the propagators of pairs of mesons created in the χc1 decay, or in the propagators inside the T matrix. We find that the most important effect in the total amplitude is the isospin breaking inside the T matrix which is essential to get a good agreement with the experimental measurement of the mixing.
Highlights
Since the discoveries of a0(980) and f0(980) mesons several decades ago, explanations of their nature have been a topic of much discussion
We investigate the isospin breaking in the χc1 → π0π+π− and χc1 → π0π0η decays and its relation to the a0(980) − f0(980) mixing, which was measured by the BESIII Collaboration
The isospin violation is introduced through the use of different masses for the charged and neutral kaons, either in the propagators of pairs of mesons created in the χc1 decay, or in the propagators inside the T matrix
Summary
Since the discoveries of a0(980) and f0(980) mesons several decades ago, explanations of their nature have been a topic of much discussion. We investigate the isospin breaking in the χc1 → π0π+π− and χc1 → π0π0η decays and its relation to the a0(980) − f0(980) mixing, which was measured by the BESIII Collaboration.
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