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Science | 2009

Dark matter search results from the CDMS II experiment.

J. Cooley; Z. Ahmed; D. S. Akerib; S. Arrenberg; C. N. Bailey; D. Balakishiyeva; L. Baudis; D. A. Bauer; P. L. Brink; T. Bruch; R. Bunker; B. Cabrera; David O. Caldwell; P. Cushman; M. Daal; F. DeJongh; M. R. Dragowsky; L. Duong; S. Fallows; E. Figueroa-Feliciano; J. Filippini; M. Fritts; S. R. Golwala; D. R. Grant; J. Hall; R. Hennings-Yeomans; S. A. Hertel; D. Holmgren; L. Hsu; M. E. Huber

News from the Dark Side? Dark matter is thought to represent 85% of all matter in the universe and to have been responsible for the formation of structure in the early universe, but its nature is still a mystery. Ahmed et al. (p. 1619, published online 11 February; see the Perspective by Lang) describe the results from the completed Cryogenic Dark Matter Search (CDMS II) experiment, which searched for dark matter in the form of weakly interacting massive particles (WIMP). Two candidate signals were observed, whereas only one background event was expected. The probability of having two or more events from the background would have been 23%. The results of this analysis cannot be interpreted with confidence as evidence for WIMP interactions, but, at the same time, neither event can be ruled out as representing signal. Details of possible, but unlikely, detection events produced by dark matter are reported. Astrophysical observations indicate that dark matter constitutes most of the mass in our universe, but its nature remains unknown. Over the past decade, the Cryogenic Dark Matter Search (CDMS II) experiment has provided world-leading sensitivity for the direct detection of weakly interacting massive particle (WIMP) dark matter. The final exposure of our low-temperature germanium particle detectors at the Soudan Underground Laboratory yielded two candidate events, with an expected background of 0.9 ± 0.2 events. This is not statistically significant evidence for a WIMP signal. The combined CDMS II data place the strongest constraints on the WIMP-nucleon spin-independent scattering cross section for a wide range of WIMP masses and exclude new parameter space in inelastic dark matter models.Z. Ahmed, D.S. Akerib, S. Arrenberg, C.N. Bailey, D. Balakishiyeva, L. Baudis, D.A. Bauer, P.L. Brink, T. Bruch, R. Bunker, B. Cabrera, D.O. Caldwell, J. Cooley, P. Cushman, M. Daal, F. DeJongh, M.R. Dragowsky, L. Duong, S. Fallows, E. Figueroa-Feliciano, J. Filippini, M. Fritts, S.R. Golwala, D.R. Grant, J. Hall, R. Hennings-Yeomans, S.A. Hertel, D. Holmgren, L. Hsu, M.E. Huber, O. Kamaev, M. Kiveni, M. Kos, S.W. Leman, R. Mahapatra, V. Mandic, K.A. McCarthy, N. Mirabolfathi, D. Moore, H. Nelson, R.W. Ogburn, A. Phipps, M. Pyle, X. Qiu, E. Ramberg, W. Rau, A. Reisetter, 7 T. Saab, B. Sadoulet, 13 J. Sander, R.W. Schnee, D.N. Seitz, B. Serfass, K.M. Sundqvist, M. Tarka, P. Wikus, S. Yellin, 14 J. Yoo, B.A. Young, and J. Zhang (CDMS Collaboration) Division of Physics, Mathematics & Astronomy, California Institute of Technology, Pasadena, CA 91125, USA Department of Physics, Case Western Reserve University, Cleveland, OH 44106, USA Fermi National Accelerator Laboratory, Batavia, IL 60510, USA Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA Department of Physics, Massachusetts Institute of Technology, Cambridge, MA 02139, USA Department of Physics, Queen’s University, Kingston, ON, Canada, K7L 3N6 Department of Physics, St. Olaf College, Northfield, MN 55057 USA Department of Physics, Santa Clara University, Santa Clara, CA 95053, USA Department of Physics, Southern Methodist University, Dallas, TX 75275, USA Department of Physics, Stanford University, Stanford, CA 94305, USA Department of Physics, Syracuse University, Syracuse, NY 13244, USA Department of Physics, Texas A & M University, College Station, TX 77843, USA Department of Physics, University of California, Berkeley, CA 94720, USA Department of Physics, University of California, Santa Barbara, CA 93106, USA Departments of Phys. & Elec. Engr., University of Colorado Denver, Denver, CO 80217, USA Department of Physics, University of Florida, Gainesville, FL 32611, USA School of Physics & Astronomy, University of Minnesota, Minneapolis, MN 55455, USA Physics Institute, University of Zürich, Winterthurerstr. 190, CH-8057, Switzerland Division of Physics, Mathematics, and Astronomy, California Institute of Technology, Pasadena, CA 91125, USA


Physical Review Letters | 2011

Results from a Low-Energy Analysis of the CDMS II Germanium Data

Z. Ahmed; D. S. Akerib; S. Arrenberg; C. N. Bailey; D. Balakishiyeva; L. Baudis; D. A. Bauer; P. L. Brink; T. Bruch; R. Bunker; B. Cabrera; David O. Caldwell; J. Cooley; E. Do Couto E Silva; P. Cushman; M. Daal; F. DeJongh; P. Di Stefano; M. R. Dragowsky; L. Duong; S. Fallows; E. Figueroa-Feliciano; J. Filippini; J. Fox; M. Fritts; S. R. Golwala; J. Hall; R. Hennings-Yeomans; S. A. Hertel; D. Holmgren

We report results from a reanalysis of data from the Cryogenic Dark Matter Search (CDMS II) experiment at the Soudan Underground Laboratory. Data taken between October 2006 and September 2008 using eight germanium detectors are reanalyzed with a lowered, 2 keV recoil-energy threshold, to give increased sensitivity to interactions from weakly interacting massive particles (WIMPs) with masses below ∼10  GeV/c(2). This analysis provides stronger constraints than previous CDMS II results for WIMP masses below 9  GeV/c(2) and excludes parameter space associated with possible low-mass WIMP signals from the DAMA/LIBRA and CoGeNT experiments.


Applied Physics Letters | 2010

Titanium nitride films for ultrasensitive microresonator detectors

H. G. LeDuc; Bruce Bumble; P. K. Day; Byeong Ho Eom; Jiansong Gao; S. R. Golwala; Benjamin A. Mazin; Sean McHugh; Andrew Merrill; D. Moore; A. D. Turner; Jonas Zmuidzinas

Titanium nitride (TiNx) films are ideal for use in superconducting microresonator detectors for the following reasons: (a) the critical temperature varies with composition (0 107) and have noise properties similar to resonators made using other materials, while the quasiparticle lifetimes are reasonably long, 10–200 μs. TiN microresonators should therefore reach sensitivities well below 10−19 W Hz−1/2.


Physical Review D | 2010

Low-threshold analysis of CDMS shallow-site data

D. S. Akerib; M. J. Attisha; L. Baudis; D. A. Bauer; A. I. Bolozdynya; P. L. Brink; R. Bunker; B. Cabrera; David O. Caldwell; C. L. Chang; R. M. Clarke; J. Cooley; M. B. Crisler; P. Cushman; F. DeJongh; R. Dixon; D. D. Driscoll; J. P. Filippini; S. Funkhouser; R.J. Gaitskell; S. R. Golwala; D. Holmgren; L. Hsu; M. E. Huber; S. Kamat; R. Mahapatra; V. Mandic; P. Meunier; N. Mirabolfathi; D. Moore

Data taken during the final shallow-site run of the first tower of the Cryogenic Dark Matter Search (CDMS II) detectors have been reanalyzed with improved sensitivity to small energy depositions. Four {approx}224 g germanium and two {approx}105 g silicon detectors were operated at the Stanford Underground Facility (SUF) between December 2001 and June 2002, yielding 118 live days of raw exposure. Three of the germanium and both silicon detectors were analyzed with a new low-threshold technique, making it possible to lower the germanium and silicon analysis thresholds down to the actual trigger thresholds of {approx}1 and {approx}2 keV, respectively. Limits on the spin-independent cross section for weakly interacting massive particles (WIMPs) to elastically scatter from nuclei based on these data exclude interesting parameter space for WIMPs with masses below 9 GeV/c{sup 2}. Under standard halo assumptions, these data partially exclude parameter space favored by interpretations of the DAMA/LIBRA and CoGeNT experiments data as WIMP signals, and exclude new parameter space for WIMP masses between 3 and 4 GeV/c{sup 2}.


Physical Review D | 2013

Silicon detector results from the first five-tower run of CDMS II

R. Agnese; Z. Ahmed; A. J. Anderson; S. Arrenberg; D. Balakishiyeva; R. Basu Thakur; D. A. Bauer; A. W. Borgland; D. Brandt; P. L. Brink; T. Bruch; R. Bunker; B. Cabrera; David O. Caldwell; D. G. Cerdeno; H. Chagani; J. Cooley; B. Cornell; C. H. Crewdson; P. Cushman; M. Daal; F. DeJongh; P. Di Stefano; E. Do Couto E Silva; T. Doughty; L. Esteban; S. Fallows; E. Figueroa-Feliciano; J. Filippini; J. Fox

We report results of a search for weakly interacting massive particles (WIMPs) with the Si detectors of the CDMS II experiment. This report describes a blind analysis of the first data taken with CDMS II’s full complement of detectors in 2006–2007; results from this exposure using the Ge detectors have already been presented. We observed no candidate WIMP-scattering events in an exposure of 55.9 kg-days before analysis cuts, with an expected background of ∼1.1 events. The exposure of this analysis is equivalent to 10.3 kg-days over a recoil energy range of 7–100 keV for an ideal Si detector and a WIMP mass of 10  GeV/c^2. These data set an upper limit of 1.7×10^(-41)  cm^2 on the WIMP-nucleon spin-independent cross section of a 10  GeV/c^2 WIMP. These data exclude parameter space for spin-independent WIMP-nucleon elastic scattering that is relevant to recent searches for low-mass WIMPs.


Applied Physics Letters | 2012

Position and energy-resolved particle detection using phonon-mediated microwave kinetic inductance detectors

D. Moore; S. R. Golwala; Bruce Bumble; B.D. Cornell; P. K. Day; H. G. LeDuc; Jonas Zmuidzinas

We demonstrate position and energy-resolved phonon-mediated detection of particle interactions in a silicon substrate instrumented with an array of microwave kinetic inductance detectors (MKIDs). The relative magnitude and delay of the signal received in each sensor allows the location of the interaction to be determined with < 1 mm precision at 30 keV. Using this position information, variations in the detector response with position can be removed, and an energy resolution of \sigma_E = 0.55 keV at 30 keV was measured. Since MKIDs can be fabricated from a single deposited film and are naturally multiplexed in the frequency domain, this technology can be extended to provide highly-pixelized athermal phonon sensors for ~1 kg scale detector elements. Such high-resolution, massive particle detectors would be applicable to next-generation rare-event searches such as the direct detection of dark matter, neutrinoless double-beta decay, or coherent neutrino-nucleus scattering.


Physical Review D | 2010

Analysis of the low-energy electron-recoil spectrum of the CDMS experiment

Z. Ahmed; D. S. Akerib; S. Arrenberg; C. N. Bailey; D. Balakishiyeva; L. Baudis; D. A. Bauer; J. Beaty; P. L. Brink; T. Bruch; R. Bunker; B. Cabrera; David O. Caldwell; J. Cooley; P. Cushman; F. DeJongh; M. R. Dragowsky; L. Duong; E. Figueroa-Feliciano; J. Filippini; M. Fritts; S. R. Golwala; D. R. Grant; J. Hall; R. Hennings-Yeomans; S. A. Hertel; D. Holmgren; L. Hsu; M. E. Huber; O. Kamaev

We report on the analysis of the low-energy electron-recoil spectrum from the CDMS II experiment using data with an exposure of 443.2 kg-days. The analysis provides details on the observed counting rate and possible background sources in the energy range of 2–8.5 keV. We find no significant excess of a peaked contribution to the total counting rate above the background model, and compare this observation to the recent DAMA results. In the framework of a conversion of a dark matter particle into electromagnetic energy, our 90% confidence level upper limit of 0.246  events/kg/day at 3.15 keV is lower than the total rate above background observed by DAMA. In absence of any specific particle physics model to provide the scaling in cross section between NaI and Ge, we assume a Z2 scaling. With this assumption the observed rate in DAMA remains higher than the upper limit in CDMS. Under the conservative assumption that the modulation amplitude is 6% of the total rate we obtain upper limits on the modulation amplitude a factor of ~2 lower than observed by DAMA, constraining some possible interpretations of this modulation.


Applied Physics Letters | 2013

Demonstration of surface electron rejection with interleaved germanium detectors for dark matter searches

R. Agnese; A. J. Anderson; D. Balakishiyeva; R. Basu Thakur; D. A. Bauer; A. W. Borgland; D. Brandt; P. L. Brink; R. Bunker; B. Cabrera; David O. Caldwell; D. G. Cerdeno; H. Chagani; M. Cherry; J. Cooley; B. Cornell; C. H. Crewdson; P. Cushman; M. Daal; P. Di Stefano; E. Do Couto E Silva; T. Doughty; L. Esteban; S. Fallows; E. Figueroa-Feliciano; J. Fox; M. Fritts; G. Godfrey; S. R. Golwala; J. Hall

The SuperCDMS experiment in the Soudan Underground Laboratory searches for dark matter with a 9-kg array of cryogenic germanium detectors. Symmetric sensors on opposite sides measure both charge and phonons from each particle interaction, providing excellent discrimination between electron and nuclear recoils, and between surface and interior events. Surface event rejection capabilities were tested with two ^(210)Pb sources producing ∼130 beta decays/hr. In ∼800 live hours, no events leaked into the 8–115 keV signal region, giving upper limit leakage fraction 1.7 × 10^(−5) at 90% C.L., corresponding to < 0.6 surface event background in the future 200-kg SuperCDMS SNOLAB experiment.


Physical Review D | 2011

Search for inelastic dark matter with the CDMS II experiment

Z. Ahmed; D. S. Akerib; S. Arrenberg; C. N. Bailey; D. Balakishiyeva; L. Baudis; D. A. Bauer; P. L. Brink; T. Bruch; R. Bunker; B. Cabrera; David O. Caldwell; J. Cooley; E. Do Couto E Silva; P. Cushman; M. Daal; F. DeJongh; P. Di Stefano; M. R. Dragowsky; L. Duong; S. Fallows; E. Figueroa-Feliciano; J. Filippini; J. Fox; M. Fritts; S. R. Golwala; J. Hall; R. Hennings-Yeomans; S. A. Hertel; D. Holmgren

Results are presented from a reanalysis of the entire five-tower data set acquired with the Cryogenic Dark Matter Search (CDMS II) experiment at the Soudan Underground Laboratory, with an exposure of 969 kg-days. The analysis window was extended to a recoil energy of 150 keV, and an improved surface-event background-rejection cut was defined to increase the sensitivity of the experiment to the inelastic dark matter (iDM) model. Three dark matter candidates were found between 25 keV and 150 keV. The probability to observe three or more background events in this energy range is 11%. Because of the occurrence of these events, the constraints on the iDM parameter space are slightly less stringent than those from our previous analysis, which used an energy window of 10–100 keV.


Applied Physics Letters | 2010

Thin film dielectric microstrip kinetic inductance detectors

Benjamin A. Mazin; D. Sank; Sean McHugh; Erik Lucero; Andrew Merrill; Jiansong Gao; David P. Pappas; D. Moore; Jonas Zmuidzinas

Microwave kinetic inductance detectors, or MKIDs, are a type of low temperature detector that exhibit intrinsic frequency domain multiplexing at microwave frequencies. We present the first theory and measurements on a MKID based on a microstrip transmission line resonator. A complete characterization of the dielectric loss and noise properties of these resonators is performed, and agrees well with the derived theory. A competitive noise equivalent power of 5×10^(−17) W Hz^(−1/2) at 10 Hz has been demonstrated. The resonators exhibit the highest quality factors known in a microstrip resonator with a deposited thin film dielectric.

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S. R. Golwala

California Institute of Technology

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J. Cooley

Southern Methodist University

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R. Bunker

University of California

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P. L. Brink

SLAC National Accelerator Laboratory

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P. Cushman

University of Minnesota

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