Study of Dalitz-Plot Distributions of the Decays η→π+π−π0 and η→π+π−γ
J. G. Layter, J. A. Appel, A. Kotlewski, W. Lee, Stephen J. Stein, J. J. Thaler
Abstract
J. G. Layter, J. A. Appel, A. Kotlewski, W. Lee, Stephen J. Stein, J. J. Thaler
Abstract
Based on 80 884 events, we obtained the matrix element squared for the decay $\ensuremath{\eta}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}:{|M(x,y)|}^{2}=1\ensuremath{-}(1.08\ifmmode\pm\else\textpm\fi{}0.014)y+(0.03\ifmmode\pm\else\textpm\fi{}0.03){y}^{2}+(0.05\ifmmode\pm\else\textpm\fi{}0.03){x}^{2}$ where $x$ and $y$ are the usual Dalitz-plot coordinates. The $\ensuremath{\gamma}$-ray energy spectrum was measured for 18 150 $\ensuremath{\eta}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\gamma}$ events. $\ensuremath{\rho}$ dominance of the ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ final state is strongly favored over a simple gauge-invariant matrix element.
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Based on 80 884 events, we obtained the matrix element squared for the decay $\ensuremath{\eta}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{\ensuremath{\pi}}^{0}:{|M(x,y)|}^{2}=1\ensuremath{-}(1.08\ifmmode\pm\else\textpm\fi{}0.014)y+(0.03\ifmmode\pm\else\textpm\fi{}0.03){y}^{2}+(0.05\ifmmode\pm\else\textpm\fi{}0.03){x}^{2}$ where $x$ and $y$ are the usual Dalitz-plot coordinates. The $\ensuremath{\gamma}$-ray energy spectrum was measured for 18 150 $\ensuremath{\eta}\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}\ensuremath{\gamma}$ events. $\ensuremath{\rho}$ dominance of the ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ final state is strongly favored over a simple gauge-invariant matrix element.
Key concepts: Physics, Dalitz plot, Particle physics, Energy (signal processing), Combinatorics, Meson, Quantum mechanics, Mathematics