Publications [#381223] of Seog Oh

Papers Published

1. Byrum, K; Corrodi, S; Oksuzian, Y; Winter, P; Xia, L; Wagner, R; Carey, RM; Edmonds, A; Israel, S; Miller, JP; Mott, J; Barnes, E; Palladino, A; Jorjadze, V; Khalatian, V; Quirk, J; Roberts, BL; Song, H; Tran, N; Wang, Y; Marciano, WJ; Ding, D; Herman, A; Hirsh, S; Kolomensky, YG; Singh, V; Varier, D; Harrig, K; Nguyen, MT; Prebys, EJ; Molzon, W; Borrel, L; Cheng, CH; Echenard, B; Flood, K; Hitlin, DG; Kim, JH; Li, Y; Lin, D; Middleton, S; Miyashita, T; Oyang, J; Porter, F; Roehrken, M; Trevor, J; Zhu, RY; Casler, H; Minh, TN; Lynch, KR; Popp., JL; Artikov, A; Atanov, N; Baranov, V; Budagov, I; Chokheli, D; Davydov, Y; Glagolev, V; Suslov, I; Oh, S; Wang, C; Adentunji, J; Alber, R; Allen, D; Allspach, D; Ambrosio, G; Andreev, N; Arnold, D; Badgley, K; Ball, M; Barker, J; Bartoszek, L; Bernstein, RH; Bianchi, I; Biery, K; Boi, S; Bono, J; Bossert, R; Bowden, M; Brandt, J; Brown, G; Brown, H; Buelher, M; Campbell, M; Casey, B; Cheban, S; Chen, M; Coghill, J; Coleman, RN; Crowley, C; Culbertson, R; Deshpande, A; Dey, J; Dhanraj, J; Dinnon, M; Dixon, S; Drake, G; Drendel, B; Duerling, G; Eddy, N; Evans, R, Mu2e Run I Sensitivity Projections for the Neutrinoless Conversion Search in Aluminum, Universe, vol. 9 no. 1 (January, 2023) [doi]
   (last updated on 2026/01/20)

   Abstract:
   The Mu2e experiment at Fermilab will search for the neutrinoless (Formula presented.) conversion in the field of an aluminum nucleus. The Mu2e data-taking plan assumes two running periods, Run I and Run II, separated by an approximately two-year-long shutdown. This paper presents an estimate of the expected Mu2e Run I search sensitivity and includes a detailed discussion of the background sources, uncertainties of their prediction, analysis procedures, and the optimization of the experimental sensitivity. The expected Run I (Formula presented.) discovery sensitivity is (Formula presented.), with a total expected background of (Formula presented.) events. In the absence of a signal, the expected upper limit is (Formula presented.) at 90% CL. This represents a three order of magnitude improvement over the current experimental limit of (Formula presented.) at 90% CL set by the SINDRUM II experiment.