Role of a triangle singularity in the $\pi \Delta$ decay of the $N(1700)(3/2^{-})$

Abstract

We show the important role played by the $\pi \Delta (1232)$ channel in the build up of the $N(1700)(3/2^{-})$ resonance due to the non-trivial enhancement produced by a singularity of a triangular loop. The $N(1700)$ is one of the dynamically generated resonances produced by the coupled channel vector-baryon interaction. The $\pi \Delta$ channel was neglected in previous works but we show that it has to be incorporated into the coupled channel formalism due to an enhancement produced by a singularity in the triangular loop with $\rho$, nucleon and $\pi$ as internal loop lines and $\pi$ and $\Delta$ as external ones. The enhancement is of non-resonant origin but it contributes to the dynamical generation of the $N(1700)$ resonance due to the non-linear dynamics involved in the coupled channel mechanisms. We obtain an important increase of the total width of the $N(1700)$ resonance when the $\pi \Delta$ channel is included and provide predictions for the partial widths of the $N(1700)$ decays into $VB$ and $\pi \Delta$.

8 pages, 6 figures

References in corpus (8)

• A Discussion on Triangle Singularities in the ${\Lambda }_b\to J/\psi K^{-}p$ Reaction
• Hidden gauge formalism for the radiative decays of axial-vector mesons
• On the nature of $a_1(1420)$
• The "$a_1(1420)$" peak as the $\pi f_0(980)$ decay mode of the $a_1(1260)$
• $f_1(1285)$ decays into $a_0(980){\pi }^0$, $f_0(980){\pi }^0$ and isospin breaking
• Role of a triangle singularity in the $\gamma p\to K^{+}\Lambda (1405)$ reaction
• Revising the $f_1(1420)$ resonance
• $f_2(1810)$ as a triangle singularity

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