High-energy positron annihilation is a viable mechanism to produce dark photons (A′). This reaction plays a significant role in beam-dump experiments using multi-GeV electron beams on thick targets by enhancing the sensitivity to A′ production. The positrons produced by the electromagnetic shower can produce an A′ via nonresonant (e++e-→γ+A′) and resonant (e++e-→A′) annihilation on atomic electrons. For visible decays, the contribution of resonant annihilation results in a larger sensitivity with respect to limits derived by the commonly used A′-strahlung in certain kinematic regions. When included in the evaluation of the E137 beam-dump experiment reach, positron annihilation pushes the current limit on μ downwards by a factor of 2 in the range 33 MeV/c2<120 MeV/c2.
Dark photon production through positron annihilation in beam-dump experiments / Marsicano, L.; Battaglieri, M.; Bondi, M.; Carvajal, C. D. R.; Celentano, A.; De Napoli, M.; De Vita, R.; Nardi, E.; Raggi, M.; Valente, P.. - In: PHYSICAL REVIEW D. - ISSN 2470-0010. - 98:1(2018). [10.1103/PhysRevD.98.015031]
Dark photon production through positron annihilation in beam-dump experiments
Raggi M.;Valente P.
2018
Abstract
High-energy positron annihilation is a viable mechanism to produce dark photons (A′). This reaction plays a significant role in beam-dump experiments using multi-GeV electron beams on thick targets by enhancing the sensitivity to A′ production. The positrons produced by the electromagnetic shower can produce an A′ via nonresonant (e++e-→γ+A′) and resonant (e++e-→A′) annihilation on atomic electrons. For visible decays, the contribution of resonant annihilation results in a larger sensitivity with respect to limits derived by the commonly used A′-strahlung in certain kinematic regions. When included in the evaluation of the E137 beam-dump experiment reach, positron annihilation pushes the current limit on μ downwards by a factor of 2 in the range 33 MeV/c2<120 MeV/c2.File | Dimensione | Formato | |
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