Projected sensitivity of the SuperCDMS SNOLAB experiment

R. Agnese(University of Florida), A. J. Anderson(Massachusetts Institute of Technology), T. Aramaki(SLAC National Accelerator Laboratory), I. J. Arnquist(Pacific Northwest National Laboratory), W. Baker(Texas A&M University), D. Barker(University of Minnesota), R. Basu Thakur(University of Illinois Urbana-Champaign), D. Bauer(Fermi National Accelerator Laboratory), A. W. Borgland(Kavli Institute for Particle Astrophysics and Cosmology), M. A. Bowles(South Dakota School of Mines and Technology), P. L. Brink(SLAC National Accelerator Laboratory), R. Bunker(Pacific Northwest National Laboratory), Blas Cabrera(Stanford University), D. O. Caldwell(University of California, Santa Barbara), R. Calkins(Southern Methodist University), C. Cartaro(SLAC National Accelerator Laboratory), D. G. Cerdeño(Durham University), H. Chagani(University of Minnesota), Y. Chen(Syracuse University), J. Cooley(Southern Methodist University), Bruce Cornell(California Institute of Technology), P. Cushman(University of Minnesota), M. Daal(University of California, Berkeley), P. C. F. Di Stefano(Queen's University), T. Doughty(University of California, Berkeley), Luis Esteban(Universidad Autónoma de Madrid), S. Fallows(University of Minnesota), E. Figueroa‐Feliciano(Northwestern University), M. Fritts(University of Minnesota), G. Gerbier(Queen's University), M. Ghaith(Queen's University), G. L. Godfrey(SLAC National Accelerator Laboratory), S. R. Golwala(California Institute of Technology), J. Hall(Pacific Northwest National Laboratory), H. R. Harris(Texas A&M University), T. Höfer(University of Minnesota), D. Holmgren(Fermi National Accelerator Laboratory), Z. Hong(Northwestern University), E. W. Hoppe(Pacific Northwest National Laboratory), L. Hsu(Fermi National Accelerator Laboratory), M. E. Huber(University of Colorado Denver), V. Iyer(National Institute of Science Education and Research), D. Jardin(Southern Methodist University), A. Jastram(Texas A&M University), M. H. Kelsey(SLAC National Accelerator Laboratory), A. Kennedy(University of Minnesota), A. Kubik(Mitchell Institute), Noah Kurinsky(SLAC National Accelerator Laboratory), A. Leder(Massachusetts Institute of Technology), B. Loer(Pacific Northwest National Laboratory), E. Lopez Asamar(Durham University), P. Lukens(Fermi National Accelerator Laboratory), R. Mahapatra(Mitchell Institute), V. Mandic(University of Minnesota), N. Mast(University of Minnesota), N. Mirabolfathi(Texas A&M University), R. A. Moffatt(Stanford University), J. D. Morales Mendoza(Texas A&M University), J. L. Orrell(Pacific Northwest National Laboratory), S. M. Oser(University of British Columbia), K. Page(Queen's University), W. A. Page(University of British Columbia), R. Partridge(SLAC National Accelerator Laboratory), M. Pepin(University of Minnesota), A. Phipps(University of California, Berkeley), S. S. Poudel(University of South Dakota), M. Pyle(University of California, Berkeley), H. Qiu(Southern Methodist University), W. Rau(Queen's University), P. Redl(Stanford University), A. Reisetter(University of Evansville), A. Roberts(University of South Dakota), Alan Robinson(Fermi National Accelerator Laboratory), H. E. Rogers(University of Minnesota), T. Saab(University of Florida), B. Sadoulet(University of California, Berkeley), J. Sander(University of South Dakota), K. Schneck(SLAC National Accelerator Laboratory), R. W. Schnee(South Dakota School of Mines and Technology), B. Serfass(University of California, Berkeley), D. Speller(University of California, Berkeley), M. Stein(Southern Methodist University), John Street(South Dakota School of Mines and Technology), Hidetaka TANAKA(University of Toronto), D. Toback(Texas A&M University), R. Underwood(Queen's University), A. N. Villano(University of Minnesota), B. von Krosigk(University of British Columbia), B. Welliver(University of Florida), Jennifer Wilson(Texas A&M University), D. H. Wright(Kavli Institute for Particle Astrophysics and Cosmology), S. Yellin(Stanford University), J. J. Yen(Stanford University), B. A. Young(Santa Clara University), X. Zhang(Queen's University), X. Zhao(Texas A&M University)
Physical review. D/Physical review. D.
April 7, 2017
Cited by 290Open Access
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Abstract

SuperCDMS SNOLAB will be a next-generation experiment aimed at directly detecting low-mass particles (with masses $\ensuremath{\le}10\text{ }\text{ }\mathrm{GeV}/{\mathrm{c}}^{2}$) that may constitute dark matter by using cryogenic detectors of two types (HV and iZIP) and two target materials (germanium and silicon). The experiment is being designed with an initial sensitivity to nuclear recoil cross sections $\ensuremath{\sim}1\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}43}\text{ }\text{ }{\mathrm{cm}}^{2}$ for a dark matter particle mass of $1\text{ }\text{ }\mathrm{GeV}/{\mathrm{c}}^{2}$, and with capacity to continue exploration to both smaller masses and better sensitivities. The phonon sensitivity of the HV detectors will be sufficient to detect nuclear recoils from sub-GeV dark matter. A detailed calibration of the detector response to low-energy recoils will be needed to optimize running conditions of the HV detectors and to interpret their data for dark matter searches. Low-activity shielding, and the depth of SNOLAB, will reduce most backgrounds, but cosmogenically produced $^{3}\mathrm{H}$ and naturally occurring $^{32}\mathrm{Si}$ will be present in the detectors at some level. Even if these backgrounds are 10 times higher than expected, the science reach of the HV detectors would be over 3 orders of magnitude beyond current results for a dark matter mass of $1\text{ }\text{ }\mathrm{GeV}/{\mathrm{c}}^{2}$. The iZIP detectors are relatively insensitive to variations in detector response and backgrounds, and will provide better sensitivity for dark matter particles with masses $\ensuremath{\gtrsim}5\text{ }\text{ }\mathrm{GeV}/{\mathrm{c}}^{2}$. The mix of detector types (HV and iZIP), and targets (germanium and silicon), planned for the experiment, as well as flexibility in how the detectors are operated, will allow us to maximize the low-mass reach, and understand the backgrounds that the experiment will encounter. Upgrades to the experiment, perhaps with a variety of ultra-low-background cryogenic detectors, will extend dark matter sensitivity down to the ``neutrino floor,'' where coherent scatters of solar neutrinos become a limiting background.


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