Triangle singularity in $Ï^- \to ν_ÏÏ^- f_0(980)$ ($a_0(980)$) decays
arXiv:1809.11007 · doi:10.1103/PhysRevD.99.016021
Abstract
We study the triangle mechanism for the decay $Ï^- \to ν_ÏÏ^- f_0(980)$, with the $f_0(980)$ decaying into $Ï^+ Ï^- $. This process is initiated by $Ï^- \to ν_ÏK^{*0} K^-$ followed by the $K^{*0}$ decay into $Ï^- K^+$, then the $K^- K^+$ produce the $f_0(980)$ through a triangle loop containing $ K^* K^+ K^-$ which develops a singularity around $1420$~MeV in the $Ïf_0(980)$ invariant mass. We find a narrow peak in the $Ï^+ Ï^-$ invariant mass distribution, which originates from the $f_0(980)$ amplitude. Similarly, we also study the triangle mechanism for the decay $Ï\to νÏ^- a_0(980)$, with the $a_0(980)$ decaying into $Ï^0 η$. The final branching ratios for $Ï^- f_0(980)$ and $Ï^- a_0(980)$ are of the order of $4 \times 10^{-4}$ and $7 \times 10^{-5}$, respectively, which are within present measurable range. Experimental verification of these predictions will shed light on the nature of the scalar mesons and on the origin for the "$a_1(1420)$" peak observed in other reactions.
7 figures, 20 pages