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Physical Review D | 2009

Results from the first science run of the ZEPLIN-III dark matter search experiment

V. N. Lebedenko; H.M. Araújo; E. J. Barnes; A. Bewick; R. Cashmore; V. Chepel; A. Currie; D. Davidge; J. Dawson; T. Durkin; B. Edwards; C. Ghag; M. Horn; A.S. Howard; A. J. Hughes; W.G. Jones; M. Joshi; G. Kalmus; A.G. Kovalenko; A. Lindote; I. Liubarsky; M.I. Lopes; R. Lüscher; P. Majewski; A. St. J. Murphy; F. Neves; J. Pinto da Cunha; R. Preece; J. J. Quenby; P.R. Scovell

The ZEPLIN-III experiment in the Palmer Underground Laboratory at Boulby uses a 12 kg two-phase xenon time-projection chamber to search for the weakly interacting massive particles (WIMPs) that may account for the dark matter of our Galaxy. The detector measures both scintillation and ionization produced by radiation interacting in the liquid to differentiate between the nuclear recoils expected from WIMPs and the electron-recoil background signals down to {approx}10 keV nuclear-recoil energy. An analysis of 847 kg{center_dot}days of data acquired between February 27, 2008, and May 20, 2008, has excluded a WIMP-nucleon elastic scattering spin-independent cross section above 8.1x10{sup -8} pb at 60 GeVc{sup -2} with a 90% confidence limit. It has also demonstrated that the two-phase xenon technique is capable of better discrimination between electron and nuclear recoils at low-energy than previously achieved by other xenon-based experiments.


Astroparticle Physics | 2007

First limits on WIMP nuclear recoil signals in ZEPLIN-II: A two-phase xenon detector for dark matter detection

G. J. Alner; H.M. Araújo; A. Bewick; C. Bungau; B. Camanzi; M.J. Carson; R. Cashmore; H. Chagani; V. Chepel; D. Cline; D. Davidge; J.C. Davies; E. Daw; J. Dawson; T. Durkin; B. Edwards; T. Gamble; J. Gao; C. Ghag; A.S. Howard; W.G. Jones; M. Joshi; E.V. Korolkova; V.A. Kudryavtsev; T.B. Lawson; V. N. Lebedenko; J.D. Lewin; P. K. Lightfoot; A. Lindote; I. Liubarsky

Abstract Results are presented from the first underground data run of ZEPLIN-II, a 31xa0kg two-phase xenon detector developed to observe nuclear recoils from hypothetical weakly interacting massive dark matter particles. Discrimination between nuclear recoils and background electron recoils is afforded by recording both the scintillation and ionisation signals generated within the liquid xenon, with the ratio of these signals being different for the two classes of event. This ratio is calibrated for different incident species using an AmBe neutron source and 60 Co γ-ray sources. From our first 31 live days of running ZEPLIN-II, the total exposure following the application of fiducial and stability cuts was 225xa0kgxa0×xa0days. A background population of radon progeny events was observed in this run, arising from radon emission in the gas purification getters, due to radon daughter ion decays on the surfaces of the walls of the chamber. An acceptance window, defined by the neutron calibration data, of 50% nuclear recoil acceptance between 5xa0keV ee and 20xa0keV ee , had an observed count of 29 events, with a summed expectation of 28.6xa0±xa04.3 γ-ray and radon progeny induced background events. These figures provide a 90% c.l. upper limit to the number of nuclear recoils of 10.4 events in this acceptance window, which converts to a WIMP–nucleon spin-independent cross-section with a minimum of 6.6xa0×xa010 −7 xa0pb following the inclusion of an energy-dependent, calibrated, efficiency. A second run is currently underway in which the radon progeny will be eliminated, thereby removing the background population, with a projected sensitivity of 2xa0×xa010 −7 xa0pb for similar exposures as the first run.


Physics Letters B | 2012

WIMP-nucleon cross-section results from the second science run of ZEPLIN-III

D. Yu. Akimov; H.M. Araújo; E. J. Barnes; V. A. Belov; A. Bewick; A. Burenkov; V. Chepel; A. Currie; L. DeViveiros; B. Edwards; C. Ghag; A. Hollingsworth; M. Horn; W.G. Jones; G. Kalmus; A. S. Kobyakin; A. G. Kovalenko; V. N. Lebedenko; A. Lindote; M.I. Lopes; R. Lüscher; P. Majewski; A. St. J. Murphy; F. Neves; S. M. Paling; J. Pinto da Cunha; R. Preece; J. J. Quenby; L. Reichhart; P.R. Scovell

Abstract We report experimental upper limits on WIMP-nucleon elastic scattering cross sections from the second science run of ZEPLIN-III at the Boulby Underground Laboratory. A raw fiducial exposure of 1344 kg⋅days was accrued over 319 days of continuous operation between June 2010 and May 2011. A total of eight events was observed in the signal acceptance region in the nuclear recoil energy range 7–29 keV, which is compatible with background expectations. This allows the exclusion of the scalar cross-section above 4.8 × 10 − 8 pb near 50 GeV / c 2 WIMP mass with 90% confidence. Combined with data from the first run, this result improves to 3.9 × 10 − 8 pb . The corresponding WIMP-neutron spin-dependent cross-section limit is 8.0 × 10 − 3 pb . The ZEPLIN programme reaches thus its conclusion at Boulby, having deployed and exploited successfully three liquid xenon experiments of increasing reach.


Astroparticle Physics | 2007

The ZEPLIN-III dark matter detector: Instrument design, manufacture and commissioning

D. Yu. Akimov; G. J. Alner; H.M. Araújo; A. Bewick; C. Bungau; A. A. Burenkov; M.J. Carson; H. Chagani; V. Chepel; D. Cline; D. Davidge; E. Daw; J. Dawson; T. Durkin; B. Edwards; T. Gamble; C. Chag; R. Hollingworth; A.S. Howard; W.G. Jones; M. Joshi; K. Mavrokoridis; E.V. Korolkova; A. G. Kovalenko; V.A. Kudryavtsev; I. S. Kuznetsov; T.B. Lawson; V. N. Lebedenko; J.D. Lewin; P. K. Lightfoot

We present details of the technical design, manufacture and testing of the ZEPLIN-III dark matter experiment. ZEPLIN-III is a two-phase xenon detector which measures both the scintillation light and the ionisation charge generated in the liquid by interacting particles and radiation. The instrument design is driven by both the physics requirements and by the technology requirements surrounding the use of liquid xenon. These include considerations of key performance parameters, such as the efficiency of scintillation light collection, restrictions placed on the use of materials to control the inherent radioactivity levels, attainment of high vacuum levels and chemical contamination control. The successful solution has involved a number of novel design and manufacturing features which will be of specific use to future generations of direct dark matter search experiments as they struggle with similar and progressively more demanding requirements.


Physics Letters B | 2005

Limits on WIMP cross-sections from the NAIAD experiment at the Boulby Underground Laboratory

G. J. Alner; H.M. Araújo; G. Arnison; J. C. Barton; A. Bewick; C. Bungau; B. Camanzi; M.J. Carson; D. Davidge; Gavin Davies; J.C. Davies; E. Daw; J. Dawson; Christopher D. P. Duffy; T. Durkin; T. Gamble; S.P. Hart; R. Hollingworth; G.J. Homer; A.S. Howard; I. Ivaniouchenkov; W.G. Jones; M. Joshi; J. Kirkpatrick; V.A. Kudryavtsev; T.B. Lawson; V. N. Lebedenko; M J Lehner; J.D. Lewin; P. K. Lightfoot

The NAIAD experiment (NaI Advanced Detector) for WIMP dark matter searches at the Boulby Underground Laboratory (North Yorkshire, UK) ran from 2000 until 2003. A total of 44.9 kg x years of data collected with 2 encapsulated and 4 unencapsulated NaI(Tl) crystals with high light yield were included in the analysis. We present final results of this analysis carried out using pulse shape discrimination. No signal associated with nuclear recoils from WIMP interactions was observed in any run with any crystal. This allowed us to set upper limits on the WIMP-nucleon spin-independent and WIMP-proton spin-dependent cross-sections. The NAIAD experiment has so far imposed the most stringent constraints on the spin-dependent WIMP-proton cross-section.


Astroparticle Physics | 2003

The NAIAD experiment for WIMP searches at Boulby mine and recent results

B. Ahmed; G. J. Alner; H.M. Araújo; J. C. Barton; A. Bewick; M.J. Carson; D. Davidge; J. Dawson; T. Gamble; S.P. Hart; R. Hollingworth; A.S. Howard; W.G. Jones; M. Joshi; V.A. Kudryavtsev; T.B Lawson; V. N. Lebedenko; M.J Lehner; J.D. Lewin; P. K. Lightfoot; I. Liubarsky; R. Lüscher; J.E. McMillan; B. Morgan; G. Nicklin; S. M. Paling; R. Preece; J. J. Quenby; J.W. Roberts; M. Robinson

Abstract The NAIAD experiment (NaI Advanced Detector) for weakly interacting massive particle (WIMP) dark matter searches at Boulby mine (UK) is described. The detector consists of an array of encapsulated and unencapsulated NaI(Tl) crystals with high light yield. Six crystals are collecting data at present. Data accumulated by four of them (10.6 kgxa0×xa0year exposure) have been used to set upper limits on the WIMP–nucleon spin-independent and WIMP–proton spin-dependent cross-sections. Pulse shape analysis has been applied to discriminate between nuclear recoils, as may be caused by WIMP interactions, and electron recoils due to gamma background. Various calibrations of crystals are presented.


Physical Review Letters | 2009

Limits on the Spin-Dependent WIMP-Nucleon Cross Sections from the First Science Run of the ZEPLIN-III Experiment

V. N. Lebedenko; H.M. Araújo; E. J. Barnes; A. Bewick; R. Cashmore; V. Chepel; A. Currie; D. Davidge; J. Dawson; T. Durkin; B. Edwards; C. Ghag; M. Horn; A.S. Howard; A. J. Hughes; W.G. Jones; M. Joshi; G. Kalmus; A.G. Kovalenko; A. Lindote; I. Liubarsky; M.I. Lopes; R. Lüscher; K. Lyons; P. Majewski; A. St. J. Murphy; F. Neves; J. Pinto da Cunha; R. Preece; J. J. Quenby

We present new experimental constraints on the WIMP-nucleon spin-dependent elastic cross sections using data from the first science run of ZEPLIN-III, a two-phase xenon experiment searching for galactic dark matter weakly interacting massive particles based at the Boulby mine. Analysis of approximately 450 kg x days fiducial exposure allow us to place a 90%-confidence upper limit on the pure WIMP-neutron cross section of sigma(n)=1.9x10(-2) pb at 55 GeV/c(2) WIMP mass. Recent calculations of the nuclear spin structure based on the Bonn charge-dependent nucleon-nucleon potential were used for the odd-neutron isotopes 129Xe and 131Xe. These indicate that the sensitivity of xenon targets to the spin-dependent WIMP-proton interaction could be much lower than implied by previous calculations, whereas the WIMP-neutron sensitivity is impaired only by a factor of approximately 2.


Physics Letters B | 2010

Limits on inelastic dark matter from ZEPLIN-III

D. Yu. Akimov; H.M. Araújo; E. J. Barnes; V. A. Belov; A. Bewick; A. Burenkov; R. Cashmore; V. Chepel; A. Currie; D. Davidge; J. Dawson; T. Durkin; B. Edwards; C. Ghag; A. Hollingsworth; M. Horn; A.S. Howard; A.J. Hughes; W.G. Jones; G. Kalmus; A. S. Kobyakin; A.G. Kovalenko; V. N. Lebedenko; A. Lindote; I. Liubarsky; M.I. Lopes; R. Lüscher; K. Lyons; P. Majewski; A. St. J. Murphy

Abstract We present limits on the WIMP–nucleon cross section for inelastic dark matter from a reanalysis of the 2008 run of ZEPLIN-III. Cuts, notably on scintillation pulse shape and scintillation-to-ionisation ratio, give a net exposure of 63 kg day in the range 20– 80 keV nuclear recoil energy, in which 6 events are observed. Upper limits on signal rate are derived from the maximum empty patch in the data. Under standard halo assumptions a small region of parameter space consistent, at 99% CL, with causing the 1.17 ton yr DAMA modulation signal is allowed at 90% CL: it is in the mass range 45– 60 GeV c − 2 with a minimum CL of 87%, again derived from the maximum patch. This is the tightest constraint yet presented using xenon, a target nucleus whose similarity to iodine mitigiates systematic error from the assumed halo.


Astroparticle Physics | 2006

The ZEPLIN-III dark matter detector: Performance study using an end-to-end simulation tool

H.M. Araújo; D. Yu. Akimov; G. J. Alner; A. Bewick; C. Bungau; B. Camanzi; M.J. Carson; V. Chepel; H. Chagani; D. Davidge; J.C. Davies; E. Daw; J. Dawson; T. Durkin; B. Edwards; T. Gamble; C. Ghag; R. Hollingworth; A.S. Howard; W.G. Jones; M. Joshi; J. Kirkpatrick; A. G. Kovalenko; V.A. Kudryavtsev; V. N. Lebedenko; T.B. Lawson; J.D. Lewin; P. K. Lightfoot; A. Lindote; I. Liubarsky

We present results from a GEANT4-based Monte Carlo tool for end-to-end simulations of the ZEPLIN-III dark matter experiment. ZEPLIN-III is a two-phase detector which measures both the scintillation light and the ionisation charge generated in liquid xenon by interacting particles and radiation. The software models the instrument response to radioactive backgrounds and calibration sources, including the generation, ray-tracing and detection of the primary and secondary scintillations in liquid and gaseous xenon, and subsequent processing by data acquisition electronics. A flexible user interface allows easy modification of detector parameters at run time. Realistic datasets can be produced to help with data analysis, an example of which is the position reconstruction algorithm developed from simulated data. We present a range of simulation results confirming the original design sensitivity of a few times 10−8 pb to the WIMP-nucleon cross-section.


Physics Letters B | 2007

Limits on spin-dependent WIMP-nucleon cross-sections from the first ZEPLIN-II data

G. J. Alner; H.M. Araújo; A. Bewick; C. Bungau; B. Camanzi; M.J. Carson; R. Cashmore; H. Chagani; V. Chepel; D. Cline; D. Davidge; J.C. Davies; E. Daw; J. Dawson; T. Durkin; B. Edwards; T. Gamble; J. Gao; C. Ghag; A.S. Howard; W.G. Jones; M. Joshi; E.V. Korolkova; V.A. Kudryavtsev; T.B. Lawson; V. N. Lebedenko; J.D. Lewin; P. K. Lightfoot; A. Lindote; I. Liubarsky

The first underground data run of the ZEPLIN-II experiment has set a limit on the nuclear recoil rate in the two-phase xenon detector for direct dark matter searches. In this Letter the results from this run are converted into the limits on spin-dependent WIMP-proton and WIMP-neutron cross-sections. The minimum of the curve for WIMP-neutron cross-section corresponds to 7 × 10−2 pb at a WIMP mass of around 65 GeV.

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A. Bewick

Imperial College London

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J. Dawson

Imperial College London

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A.S. Howard

Imperial College London

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D. Davidge

Imperial College London

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M. Joshi

Imperial College London

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H.M. Araújo

Imperial College London

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I. Liubarsky

Imperial College London

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G. J. Alner

Rutherford Appleton Laboratory

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J. J. Quenby

Imperial College London

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