Speaker
Description
KLOE and KLOE-2 data (almost $8~fb^{-1}$) constitute a unique sample, rich in physics, and the largest dataset ever collected at an electron-positron collider operating at the $\phi$ peak resonance.
In total it corresponds to the production of about 24 billion $\phi$ mesons, whose decays include about 8 billion pairs of neutral $K$ mesons and about 300 million $\eta$ mesons.
A wide hadron physic program, investigating rare meson decays, $\gamma\gamma$ interaction, and dark forces, is thus carried out by the KLOE-2 Collaboration.
The $\eta\to \pi^0\gamma\gamma$ decay is a test bench for various models and effective theories like VMD (Vector Meson Dominance) or ChPT (Chiral Perturbation Theory) which predict BR far from the experimental value. KLOE-2, with its highly pure $\eta$ sample produced
in $\phi\to \eta\gamma$ process, can give a more refined measurement of this branching ratio.
KLOE-2 continues also its tradition on dark searches testing an opposite model to the U boson or "dark photon", where the dark force mediator is a hypothetical leptophobic B boson that could show up in the $\phi\to \eta_B \to \eta \pi^0\gamma$, $\eta\to \gamma\gamma$ channel. The upper limit on the $\alpha_B$ coupling constant will be shown.
A KLOE-2 distinctive feature is also the the possibility to investigate $\pi^0$ production from $\gamma\gamma$ scattering by tagging final-state leptons from $e^+ e^- \to \gamma^{(*)}\gamma^{(*)} e^+ e^- \to \pi^0 e^+ e^-$ in coincidence with the $\pi^0$ in the barrel calorimeter. The preliminary measurement of the $\gamma^*\gamma \to \pi^0$ cross section performed with single-tagged events will be reported.
Moreover, the search for the double suppressed $\phi\to \eta \pi^+ \pi^-$ and the conversion $\phi\to \eta \mu^+ \mu^-$ decays are being performed at KLOE-2 with both $\eta\to \gamma\gamma$ and $\eta\to 3\pi^0$. Clear signals are seen for the first time.
Finally, preliminary and promising results on the $\omega$ cross-section measurement in the $e^+ e^-\to \pi^+\pi^- \pi^0 \gamma_{\rm ISR}$ channel using the Initial State Radiation (ISR) method will be also presented.
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