η(1295)→3πη(1295)\to3π decays

preprint2021arXivOpen access

Abstract

The radially excited pseudoscalar state η(1295)η(1295) is still poorly understood [as well as its SU(3)SU(3) partners π(1300)π(1300) and K(1460)K(1460 )] and we want to attract attention experimenters to its comprehensive study. As for the main three-body decay η(1295)→ηππη(1295)\to ηππ, here the main interest is the measurements of the shapes of the ηπηπ and ππππ mass spectra in which the contributions from the a0(980)a_0(980) resonance and the large ππππ SS wave (σσ) should manifest themselves. To describe these mass spectra, we propose to use a simple isobar model with a single fitting parameter characterizing the relative intensity of the a0(980)a_0 (980) and σσ state production. Our main goal is to discuss the dynamics of the isospin-breaking decays η(1295)→π+π−π0η(1295)\toπ^+ π^-π^0 and η(1295)→3π0η(1295)\to3π^0, whose experimental studies could continue the impressive story of isospin violations in the decays of light isoscalar mesons ω→2πω\to2π, η→3πη\to3 π, η′→3πη'\to3π, η(1405)→3πη(1405)\to3π, and f1(1285)→3πf_1(1285)\to3π. We estimate the widths of the isospin-breaking decays η(1295)→3πη(1295)\to 3π produced via the mixing of the π0−ηπ^0-η and a00(980)−f0(980)a^0_0(980) -f_0(980) states and also due to the π0(1300)−η(1295)π^0(1300)-η(1295) mixing. Processes that have the potential for detecting η(1295)→3πη(1295) \to3π decays are discussed.

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