The DarkLight Experiment: A Precision Search for New Physics at Low Energies
J. Balewski, J. Bernauer, J. Bessuille, R. Corliss, R. Cowan, C. Epstein, P. Fisher, D. Hasell, E. Ihloff, Y. Kahn, J. Kelsey, R. Milner, S. Steadman, J. Thaler, C. Tschalaer, C. Vidal, S. Benson, J. Boyce, D. Douglas, P. Evtushenko, C. Hernandez-Garcia, C. Keith, C. Tennant, S. Zhang, R. Alarcon, D. Blyth, R. Dipert, L. Ice, G. Randall, B. Dongwi, N. Kalantarians, M. Kohl, A. Liyanage, J. Nazeer, M. Garcon, R. Cervantes, K. Dehmelt, A. Deshpande, N. Feege, B. Surrow
TL;DR
This paper outlines the motivation for a dark photon search at low energies, presents the DarkLight experimental concept for precision $ep$ scattering with full final-state reconstruction, and details a staged path to realization (Phase-I and Phase-II) using existing infrastructure and new detector technologies. It describes leveraging a 100 MeV energy-recovery linac beam on a windowless H$_2$ target inside a 0.5 T solenoidal magnet to achieve high luminosity and ~1 MeV/$c^2$ $e^+e^-$ invariant-mass resolution, enabling sensitivity to $A'$ decays to $e^+e^-$ and invisible final states. The paper covers the motivation, conceptual design, current status, and a phased plan for realization, including detector technologies and a triggerless data-acquisition approach, arguing that the approach can explore previously unconstrained regions of $\\epsilon^2$ vs $m_{A'}$ space. Overall, DarkLight seeks to advance low-$Q^2$ electron scattering and provide a complementary, high-sensitivity search for new light gauge bosons.
Abstract
We describe the current status of the DarkLight experiment at Jefferson Laboratory. DarkLight is motivated by the possibility that a dark photon in the mass range 10 to 100 MeV/c$^2$ could couple the dark sector to the Standard Model. DarkLight will precisely measure electron proton scattering using the 100 MeV electron beam of intensity 5 mA at the Jefferson Laboratory energy recovering linac incident on a windowless gas target of molecular hydrogen. The complete final state including scattered electron, recoil proton, and e+e- pair will be detected. A phase-I experiment has been funded and is expected to take data in the next eighteen months. The complete phase-II experiment is under final design and could run within two years after phase-I is completed. The DarkLight experiment drives development of new technology for beam, target, and detector and provides a new means to carry out electron scattering experiments at low momentum transfers.
