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Featured researches published by A. Bewick.


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.


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.


Physics Letters B | 2000

NaI dark matter limits and the NAIAD array – a detector with improved sensitivity to WIMPs using unencapsulated NaI

N.J.C. Spooner; V.A. Kudryavtsev; C.D. Peak; P. K. Lightfoot; T.B Lawson; M.J Lehner; J.E. McMillan; J.W. Roberts; D. R. Tovey; N.J.T. Smith; P.F. Smith; J.D. Lewin; G.J. Homer; G. J. Alner; T. J. Sumner; A. Bewick; W. G. Jones; J. J. Quenby; I. Liubarsky; Jerome C. Barton

Re-analysis of published data from the UKDMC NaI Tl dark matter experiment is presented using latest spin factors and comparison is made with the sensitivity predicted for NAIAD, a 100 kg NaI detector concept based on unencapsulated . NaI Tl . We present experimental results and Monte Carlo simulations for NAIAD and show that a factor of 1.5-2 improvement in energy threshold is achievable over conventional NaI dark matter detectors with consequent ; 50% improvement in nuclear recoil discrimination at 10 keV. An overall improvement in sensitivity to spin dependent WIMP interactions of factor 50, based on 100 kg = yrs of data, is predicted relative to previous UKDMC limits. q 2000 Published by Elsevier Science B.V. All rights reserved.


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.


Applied Physics Letters | 2002

Table-top neutron source for characterization and calibration of dark matter detectors

F. N. Beg; K. Krushelnick; C. Gower; S. Torn; A. E. Dangor; A.S. Howard; T. J. Sumner; A. Bewick; V. N. Lebedenko; J. Dawson; D. Davidge; M. Joshi; J. R. Gillespie

A table-top plasma focus device is shown to be an ideal neutron source for the calibration and characterization of dark matter detectors and has been optimized to produce a maximum yield of 2.0310 7 neutrons per shot. The interaction of energetic neutrons is similar to that expected from weakly interacting massive particles ~WIMPs!—a favored candidate for the dominant component of dark matter in the universe. The weak interaction of a neutron with liquid xenon gas was measured in a prototype xenon two-phase detector. We have developed a detector system in which both the primary scintillation and ionization from the initial interaction can be detected. Both measurements are critical for identifying WIMP’s.


Physics Letters B | 1991

Demonstration of nuclear recoil discrimination for low temperature dark matter detectors, by measurement of simultaneous ionization and thermal pulses in silicon

N.J.C. Spooner; A. Bewick; G.J. Homer; P.F. Smith; J.D. Lewin

Abstract We report experiments using a silicon target exposed to a neutron source, giving both nuclear recoil events from neutron scattering and electron recoil events from photon scattering. We show that simultaneous measurement of ionization and thermal energy for each event allows the neutron and photon events to be separated. The degree of separation of the nuclear recoil events, and their absolute event rate, are consistent with theoretical expectation.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992

GaAs revisited as a room temperature X-ray detector

T.J. Summer; S.M. Grant; A. Bewick; J.P. Li; K. M. Smith; S. P. Beaumont

In recent years there has been a renewal of interest from many disciplines, including high energy physics, particle astrophysics and medicine, in developing GaAs as a detector. This work reports on the assessment of some Schottky barrier devices, made from LEC starting material for particle physics experiments [1], as X-ray detectors. The detectors measured 3.0 mm × 5.0 mm × 135 μm with a small, 1 mm diameter. Schottky contact in the centre. In the best devices a charge separation efficiency above 90% was achieved and measured resolutions at 122 keV and 60 keV were ∼8% and ∼6% HWHM respectively. Carrier trapping and device instabilities are the dominant limitations to better performance.


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.

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D. Davidge

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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M. Joshi

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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I. Liubarsky

Imperial College London

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T. J. Sumner

Imperial College London

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