Abstract

We propose to search the monophoton events at the BESIII detector and future Super Tau Charm Factory to probe the sub-GeV dark photon decay into lighter dark matter. We compute the cross section due to the dark photon associated a standard model photon production, and study the corresponding standard model irreducible/reducible backgrounds. By using the data about 17 fb$^{-1}$ collected at the BESIII detector since 2011, we derive new leading limits of the mixing strength $\varepsilon$, $\varepsilon\lesssim(1.1-1.6)\times 10^{-4}$, in the mass range of 0.04 GeV $\lesssim m_{A^\prime} \lesssim$ 3 GeV. With 30 ab$^{-1}$ data, STCF running at $\sqrt{s} = 2$ GeV, can probe $\varepsilon$ down to 5.1$\times 10^{-6}$ when $m_{A^\prime}=1$ GeV. For models of scalar and fermionic light thermal dark matter production via dark photon, we present the constrains on the dimensionless dark matter parameter $y=\varepsilon^2\alpha_D(m_\chi/m_{A^\prime})^4$ as function of the DM mass $m_{\chi}$ at BESIII and future STCF, conventionally assuming the dark coupling constant $\alpha_D=0.5$ and $m_{A^\prime}=3 m_{\chi}$. We find that BESIII can exclude model of scalar, Majorana, and pseudo-Dirac (with a small splitting) DM for the mass region 0.03$\sim$1 GeV, 0.04$\sim$1 GeV and 0.4$\sim$1 GeV respectively. For values $\alpha_D\lesssim 0.005$, combining the results from 2 GeV STCF with 30 ab$^{-1}$ data and BaBar, one can exclude the above three DM models in the mass region 0.001 GeV $\lesssim m_{\chi} \lesssim$ 1 GeV.

Highlights

  • To investigate the nature of dark matter (DM) particle is one of the most pressing issues in modern physics

  • We propose probing the invisible decay of dark photon via the monophoton signature at the BESIII detector and future Super Tau Charm Factory (STCF)

  • The dark photon mixes with the SM photon and decays dominantly invisible into light DM particles A0 → χχ

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Summary

INTRODUCTION

To investigate the nature of dark matter (DM) particle is one of the most pressing issues in modern physics. Since there are no firm predictions for the dark photon, various experiments have been searched for it over a wide range of its mass and decay modes [9,10,11]. We focus on the search for the invisible decay of the dark photon at the BESIII detector and future Super Tau. Charm Factory (STCF). The cleanest collider signature of such particles is the process eþe− → γA0, followed by invisible decay of the A0, which is monochromatic single photon production accompanied by significant missing energy and momentum. We use the monophoton signature to probe invisible decay of dark photon at the BESIII detector and STCF.

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