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Data-Driven Modeling of Electron Recoil Nucleation in PICO C$_3$F$_8$ Bubble Chambers

Authors :
Amole, C.
Ardid, M.
Arnquist, I. J.
Asner, D. M.
Baxter, D.
Behnke, E.
Bressler, M.
Broerman, B.
Cao, G.
Chen, C. J.
Chen, S.
Chowdhury, U.
Clark, K.
Collar, J. I.
Cooper, P. S.
Coutu, C. B.
Cowles, C.
Crisler, M.
Crowder, G.
Cruz-Venegas, N. A.
Dahl, C. E.
Das, M.
Fallows, S.
Farine, J.
Filgas, R.
Fuentes, J.
Girard, F.
Giroux, G.
Hackett, B.
Hagen, A.
Hall, J.
Hardy, C.
Harris, O.
Hillier, T.
Hoppe, E. W.
Jackson, C. M.
Jin, M.
Klopfenstein, L.
Kozynets, T.
Krauss, C. B.
Laurin, M.
Lawson, I.
Leblanc, A.
Levine, I.
Licciardi, C.
Lippincott, W. H.
Loer, B.
Mamedov, F.
Mitra, P.
Moore, C.
Nania, T.
Neilson, R.
Noble, A. J.
Oedekerk, P.
Ortega, A.
Pal, S.
Piro, M. -C.
Plante, A.
Priya, S.
Robinson, A. E.
Sahoo, S.
Scallon, O.
Seth, S.
Sonnenschein, A.
Starinski, N.
��tekl, I.
Sullivan, T.
Tardif, F.
Tiwari, D.
V��zquez-J��uregui, E.
Wagner, J. M.
Walkowski, N.
Weima, E.
Wichoski, U.
Wierman, K.
Woodley, W.
Yan, Y.
Zacek, V.
Zhang, J.
Publication Year :
2019

Abstract

The primary advantage of moderately superheated bubble chamber detectors is their simultaneous sensitivity to nuclear recoils from WIMP dark matter and insensitivity to electron recoil backgrounds. A comprehensive analysis of PICO gamma calibration data demonstrates for the first time that electron recoils in C$_3$F$_8$ scale in accordance with a new nucleation mechanism, rather than one driven by a hot-spike as previously supposed. Using this semi-empirical model, bubble chamber nucleation thresholds may be tuned to be sensitive to lower energy nuclear recoils while maintaining excellent electron recoil rejection. The PICO-40L detector will exploit this model to achieve thermodynamic thresholds as low as 2.8 keV while being dominated by single-scatter events from coherent elastic neutrino-nucleus scattering of solar neutrinos. In one year of operation, PICO-40L can improve existing leading limits from PICO on spin-dependent WIMP-proton coupling by nearly an order of magnitude for WIMP masses greater than 3 GeV c$^{-2}$ and will have the ability to surpass all existing non-xenon bounds on spin-independent WIMP-nucleon coupling for WIMP masses from 3 to 40 GeV c$^{-2}$.<br />18 pages, 12 figures

Details

Language :
English
Database :
OpenAIRE
Accession number :
edsair.doi.dedup.....4768fb2dcec543c0fd598ba36e14b4dc