Ionization yield measurement in a germanium CDMSlite detector using photo-neutron sources
Creators: name: SuperCDMS Collaboration
name: Albakry, M. F.
name: Alkhatib, I.
name: Amaral, D. W. P.
name: Aralis, T.
name: Aramaki, T.
name: Arnquist, I. J.
name: Langroudy, I. Ataee
name: Azadbakht, E.
name: Banik, S.
name: Bathurst, C.
name: Bauer, D. A.
name: Bezerra, L. V. S.
name: Bhattacharyya, R.
name: Bowles, M. A.
name: Brink, P. L.
name: Bunker, R.
name: Cabrera, B.
name: Calkins, R.
name: Cameron, R. A.
name: Cartaro, C.
name: Cerdeño, D. G.
name: Chang, Y. -Y.
name: Chaudhuri, M.
name: Chen, R.
name: Chott, N.
name: Cooley, J.
name: Coombes, H.
name: Corbett, J.
name: Cushman, P.
name: De Brienne, F.
name: di Vacri, M. L.
name: Diamond, M. D.
name: Fascione, E.
name: Figueroa-Feliciano, E.
name: Fink, C. W.
name: Fouts, K.
name: Fritts, M.
name: Gerbier, G.
name: Germond, R.
name: Ghaith, M.
name: Golwala, S. R.
name: Hall, J.
name: Hines, B. A.
name: Hollister, M. I.
name: Hong, Z.
name: Hoppe, E. W.
name: Hsu, L.
name: Huber, M. E.
name: Iyer, V.
name: Jastram, A.
name: Kashyap, V. K. S.
name: Kelsey, M. H.
name: Kubik, A.
name: Kurinsky, N. A.
name: Lawrence, R. E.
name: Lee, M.
name: Li, A.
name: Liu, J.
name: Liu, Y.
name: Loer, B.
name: Lukens, P.
name: MacDonell, D.
name: MacFarlane, D. B.
name: Mahapatra, R.
name: Mandic, V.
name: Mast, N.
name: Mayer, A. J.
name: Theenhausen, H. Meyer zu
name: Michaud, É.
name: Michielin, E.
name: Mirabolfathi, N.
name: Mohanty, B.
name: Mendoza, J. D. Morales
name: Nagorny, S.
name: Nelson, J.
name: Neog, H.
name: Novati, V.
name: Orrell, J. L.
name: Osborne, M. D.
name: Oser, S. M.
name: Page, W. A.
name: Partridge, R.
name: Pedreros, D. S.
name: Podviianiuk, R.
name: Ponce, F.
name: Poudel, S.
name: Pradeep, A.
name: Pyle, M.
name: Rau, W.
name: Reid, E.
name: Ren, R.
name: Reynolds, T.
name: Roberts, A.
name: Robinson, A. E.
name: Saab, T.
name: Sadoulet, B.
name: Saikia, I.
name: Sander, J.
name: Sattari, A.
name: Scarff, A.
name: Schmidt, B.
name: Schnee, R. W.
name: Scorza, S.
name: Serfass, B.
name: Sincavage, D. J.
name: Stanford, C.
name: Street, J.
name: Thasrawala, F. K.
name: Toback, D.
name: Underwood, R.
name: Verma, S.
name: Villano, A. N.
name: von Krosigk, B.
name: Watkins, S. L.
name: Wen, O.
name: Williams, Z.
name: Wilson, M. J.
name: Winchell, J.
name: Wykoff, K.
name: Yellin, S.
name: Young, B. A.
name: Yu, T. C.
name: Zatschler, B.
name: Zatschler, S.
name: Zaytsev, A.
name: Zhang, E.
name: Zheng, L.
name: Zuber, S.
Publisher: name: arXiv
Year: 2022
Subjects: subject: Instrumentation and Detectors (physics.ins-det)
subject: FOS: Physical sciences
subject: FOS: Physical sciences

description: Two photo-neutron sources, $^{88}$Y$^{9}$Be and $^{124}$Sb$^{9}$Be, have been used to investigate the ionization yield of nuclear recoils in the CDMSlite germanium detectors by the SuperCDMS collaboration. This work evaluates the yield for nuclear recoil energies between 1 keV and 7 keV at a temperature of $\sim$ 50 mK. We use a Geant4 simulation to model the neutron spectrum assuming a charge yield model that is a generalization of the standard Lindhard model and consists of two energy dependent parameters. We perform a likelihood analysis using the simulated neutron spectrum, modeled background, and experimental data to obtain the best fit values of the yield model. The ionization yield between recoil energies of 1 keV and 7 keV is shown to be significantly lower than predicted by the standard Lindhard model for germanium. There is a general lack of agreement among different experiments using a variety of techniques studying the low-energy range of the nuclear recoil yield, which is most critical for interpretation of direct dark matter searches. This suggests complexity in the physical process that many direct detection experiments use to model their primary signal detection mechanism and highlights the need for further studies to clarify underlying systematic effects that have not been well understood up to this point.