N. Madden
Lawrence Livermore National Laboratory
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Physical Review Letters | 2011
J. Angle; E. Aprile; F. Arneodo; L. Baudis; A. Bernstein; A. Bolozdynya; L. Coelho; C. E. Dahl; L. DeViveiros; A. D. Ferella; L.M.P. Fernandes; S. Fiorucci; R.J. Gaitskell; Karl-Ludwig Giboni; R. Gomez; R. Hasty; L. Kastens; J. Kwong; J. A. M. Lopes; N. Madden; A. Manalaysay; A. Manzur; D. N. McKinsey; M.E. Monzani; K. Ni; U. Oberlack; J. Orboeck; G. Plante; R. Santorelli; J.M.F. dos Santos
We report results of a search for light (≲10u2009u2009GeV) particle dark matter with the XENON10 detector. The event trigger was sensitive to a single electron, with the analysis threshold of 5 electrons corresponding to 1.4 keV nuclear recoil energy. Considering spin-independent dark matter-nucleon scattering, we exclude cross sections σ(n)>7×10(-42)u2009u2009cm(2), for a dark matter particle mass m(χ)=7u2009u2009GeV. We find that our data strongly constrain recent elastic dark matter interpretations of excess low-energy events observed by CoGeNT and CRESST-II, as well as the DAMA annual modulation signal.
Physical Review D | 2009
J. Angle; E. Aprile; F. Arneodo; L. Baudis; A. Bernstein; A. Bolozdynya; L. Coelho; C. E. Dahl; L. DeViveiros; A. D. Ferella; L.M.P. Fernandes; S. Fiorucci; R.J. Gaitskell; Karl-Ludwig Giboni; R. Gomez; R. Hasty; L. Kastens; J. Kwong; J. A. M. Lopes; N. Madden; A. Manalaysay; A. Manzur; D. N. McKinsey; M.E. Monzani; K. Ni; U. Oberlack; J. Orboeck; G. Plante; R. Santorelli; J.M.F. dos Santos
It has been suggested that dark matter particles which scatter inelastically from detector target nuclei could explain the apparent incompatibility of the DAMA modulation signal (interpreted as evidence for particle dark matter) with the null results from CDMS-II and XENON10. Among the predictions of inelastically interacting dark matter are a suppression of low-energy events, and a population of nuclear recoil events at higher nuclear recoil equivalent energies. This is in stark contrast to the well-known expectation of a falling exponential spectrum for the case of elastic interactions. We present a new analysis of XENON10 dark matter search data extending to E{sub nr} = 75 keV nuclear recoil equivalent energy. Our results exclude a significant region of previously allowed parameter space in the model of inelastically interacting dark matter. In particular, it is found that dark matter particle masses m{sub x} {approx}> 150 GeV are disfavored.
Astroparticle Physics | 2011
E. Aprile; J. Angle; F. Arneodo; L. Baudis; A. Bernstein; A. Bolozdynya; P.P. Brusov; L. Coelho; C. E. Dahl; L. DeViveiros; A. D. Ferella; L.M.P. Fernandes; S. Fiorucci; R.J. Gaitskell; Karl-Ludwig Giboni; R. Gomez; R. Hasty; L. Kastens; J. Kwong; J. A. M. Lopes; N. Madden; A. Manalaysay; A. Manzur; D. N. McKinsey; M.E. Monzani; K. Ni; U. Oberlack; J. Orboeck; D. Orlandi; G. Plante
Abstract XENON10 is the first two-phase xenon time projection chamber (TPC) developed within the XENON dark matter search program. The TPC, with an active liquid xenon (LXe) mass of about 14xa0kg, was installed at the Gran Sasso Underground Laboratory (LNGS) in Italy, and operated for more than one year, with excellent stability and performance. Results from a dark matter search with XENON10 have been published elsewhere. In this paper, we summarize the design and performance of the detector and its subsystems, based on calibration data using sources of gamma-rays and neutrons as well as background and Monte Carlo simulation data. The results on the detector’s energy threshold, position resolution, and overall efficiency show a performance that exceeds design specifications, in view of the very low energy threshold achieved (
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009
P. Sorensen; A. Manzur; C. E. Dahl; J. Angle; E. Aprile; F. Arneodo; L. Baudis; A. Bernstein; A. Bolozdynya; L. Coelho; L. DeViveiros; A. D. Ferella; L.M.P. Fernandes; S. Fiorucci; R.J. Gaitskell; Karl-Ludwig Giboni; R. Gomez; R. Hasty; L. Kastens; J. Kwong; J. A. M. Lopes; N. Madden; A. Manalaysay; D. N. McKinsey; M.E. Monzani; K. Ni; U. Oberlack; J. Orboeck; G. Plante; R. Santorelli
XENON10 is an experiment designed to directly detect particle dark matter. It is a dual phase (liquid/gas) xenon time-projection chamber with 3D position imaging. Particle interactions generate a primary scintillation signal (S1) and ionization signal (S2), which are both functions of the deposited recoil energy and the incident particle type. We present a new precision measurement of the relative scintillation yield View the MathML source and the absolute ionization yield View the MathML source, for nuclear recoils in xenon. A dark matter particle is expected to deposit energy by scattering from a xenon nucleus. Knowledge of View the MathML source is therefore crucial for establishing the energy threshold of the experiment; this in turn determines the sensitivity to particle dark matter. Our View the MathML source measurement is in agreement with recent theoretical predictions above 15 keV nuclear recoil energy, and the energy threshold of the measurement is View the MathML source. A knowledge of the ionization yield View the MathML source is necessary to establish the trigger threshold of the experiment. The ionization yield View the MathML source is measured in two ways, both in agreement with previous measurements and with a factor of 10 lower energy threshold.
Journal of Physics: Conference Series | 2006
E. Aprile; Karl-Ludwig Giboni; S. Kamat; K. Ni; B K Singh; M. Yamashita; R.J. Gaitskell; P. Sorensen; L. de Viveiros; R. Gomez; U. Oberlack; P. Shagin; A. Bolozdynya; E. Dahl; J. Kwong; T. Shutt; J. Angle; L. Baudis; A. Manalaysay; J Orboeck; R. Hasty; A. Manzur; D. N. McKinsey; A. Bernstein; N. Madden; C. Winant; F. Arneodo; A. Ferella; J A Matias Lopes; Joaquim M. F. Dos Santos
The XENON experiment searches for dark matter particles called WIMPs using liquid xenon (LXe) as the active target. The detector is a 3D position sensitive Time Projection Chamber optimized to simultaneously measure the ionization and scintillation produced by a recoil event of energy as low as 16 keV. The distinct ratio of the two signals for nuclear recoils arising from WIMPs and neutrons and for electron recoils from the dominant gamma-ray background determines its event-by-event discrimination. With 1 ton of LXe distributed in ten identical modules, the proposed XENON1T experiment will achieve a sensitivity more than a factor of thousand beyond current limits. A phased program will test a 10 kg detector (XENON10) followed by a 100 kg (XENON100) one as unit module for the XENON1T scale experiment. We review the progress of the XENON R & D phase before presenting the status of XENON10. The experiment will be based at the Gran Sasso Underground Laboratory and is expected to start data taking in early 2006.
Physical Review Letters | 2013
J. Angle; E. Aprile; F. Arneodo; L. Baudis; A. Bernstein; A. Bolozdynya; L. Coelho; C. E. Dahl; L. DeViveiros; A. D. Ferella; L.M.P. Fernandes; S. Fiorucci; R.J. Gaitskell; Karl-Ludwig Giboni; R. Gomez; R. Hasty; L. Kastens; J. Kwong; J. A. M. Lopes; N. Madden; A. Manalaysay; A. Manzur; D. N. McKinsey; M.E. Monzani; K. Ni; U. Oberlack; J. Orboeck; G. Plante; R. Santorelli; J.M.F. dos Santos
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2005
Eric H. Silver; G. Austin; Jeffrey W. Beeman; F. S. Goulding; E. E. Haller; D. Landis; N. Madden
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2006
Stanley G. Prussin; Marie-Anne Descalle; James M. Hall; J. Pruet; Dennis R. Slaughter; M.R. Accatino; O. Alford; Stephen John Asztalos; A. Bernstein; J.A. Church; Thomas B. Gosnell; A. Loshak; N. Madden; D.R. Manatt; G.J. Mauger; A.W. Meyer; T.L. Moore; E. B. Norman; B.A. Pohl; D.C. Petersen; B. Rusnak; T.B. Sundsmo; W.K. Tenbrook; Rosemary S. Walling
arXiv: Astrophysics | 2008
P. Sorensen; A. Manzur; C. E. Dahl; J. Angle; E. Aprile; F. Arneodo; L. Baudis; A. Bernstein; A. Bolozdynya; P.P. Brusov; L. Coelho; L. DeViveiros; A. D. Ferella; L.M.P. Fernandes; S. Fiorucci; R.J. Gaitskell; Karl-Ludwig Giboni; R. Gomez; R. Hasty; L. Kastens; J. Kwong; J. A. M. Lopes; N. Madden; A. Manalaysay; D. N. McKinsey; M.E. Monzani; K. Ni; U. Oberlack; J. Orboeck; G. Plante
Nuclear Physics B - Proceedings Supplements | 2008
E. Aprile; Karl-Ludwig Giboni; S. Kamat; M.E. Monzani; G. Plante; M. Yamashita; R.J. Gaitskell; S. Fiorucci; P. Sorensen; L. DeViveiros; A. Bernstein; N. Madden; C. Winant; T. Shutt; J. Kwong; A. Bolozdynya; E. Dahl; U. Oberlack; P. Shagin; R. Gomez; D. N. McKinsey; A. Manzur; R. Hasty; K. Ni; F. Arneodo; A. Ferella; L. Baudis; J. Angle; J. Orboeck; A. Manalaysay