A new direct detection electron scattering experiment to search for the X17 particle

D. Dutta, H. Gao,A. Gasparian,T. J. Hague,N. Liyanage,R. Paremuzyan,C. Peng, W. Xiong,P. Achenbach,A. Ahmidouch,S. Ali,H. Avakian, C. Ayerbe-Gayoso,X. Bai,M. Battaglieri,H. Bhatt, A. Bianconi, J. Boyd, D. Byer,P. L. Cole, G. Costantini, S. Davis,M. De Napoli,R. De Vita,B. Devkota, B. Dharmasena, J. Dunne,L. El Fassi, V. Gamage, L. Gan,K. Gnanvo, G. Gosta,D. Higinbotham, C. Howell, S. Jeffas,S. Jian,A. Karki,B. Karki, V. Khachatryan, M. Khandaker,V. Kubarovsky, I. Larin,M. Leali,V. Mascagna, G. Matousek,S. Migliorati,R. Miskimen,P. Mohanmurthy, H. Nguyen,E. Pasyuk, A. Rathnayake,J. Rittenhouse West,A. Shahinyan, A. Smith,S. Stepanyan, E. van Nieuwenhuizen,L. Venturelli, B. Yu,Z. Zhao,J. Zhou

arxiv(2023)

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摘要
A new electron scattering experiment (E12-21-003) to verify and understand the nature of hidden sector particles, with particular emphasis on the so-called X17 particle, has been approved at Jefferson Lab. The search for these particles is motivated by new hidden sector models introduced to account for a variety of experimental and observational puzzles: excess in $e^+e^-$ pairs observed in multiple nuclear transitions, the 4.2$\sigma$ disagreement between experiments and the standard model prediction for the muon anomalous magnetic moment, and the small-scale structure puzzle in cosmological simulations. The aforementioned X17 particle has been hypothesized to account for the excess in $e^+e^-$ pairs observed from the $^8$Be M1, $^4$He M0, and, most recently, $^{12}$C E1 nuclear transitions to their ground states observed by the ATOMKI group. This experiment will use a high resolution electromagnetic calorimeter to search for or set new limits on the production rate of the X17 and other hidden sector particles in the $3 - 60$ MeV mass range via their $e^+e^-$ decay (or $\gamma\gamma$ decay with limited tracking). In these models, the $1 - 100$ MeV mass range is particularly well-motivated and the lower part of this range still remains unexplored. Our proposed direct detection experiment will use a magnetic-spectrometer-free setup (the PRad apparatus) to detect all three final state particles in the visible decay of a hidden sector particle for an effective control of the background and will cover the proposed mass range in a single setting. The use of the well-demonstrated PRad setup allows for an essentially ready-to-run and uniquely cost-effective search for hidden sector particles in the $3 - 60$ MeV mass range with a sensitivity of 8.9$\times$10$^{-8}$ - 5.8$\times$10$^{-9}$ to $\epsilon^2$, the square of the kinetic mixing interaction constant between hidden and visible sectors.
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new direct detection electron,particle
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