WIMP-nucleon cross-section results from the second science run of ZEPLIN-III
By D. Akimov, H. Araújo, E. Barnes, V. Belov, A. Bewick, A. Burenkov, V. Chepel, A. Currie, L. deViveiros, B. Edwards and 27 more. 2011
156 citations recorded by the source corpus.
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.
Subfields: Atomic and Molecular Physics, and Optics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/6660a0502ca088c18262755e83079f876c2f3de6
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Citations in the corpus
- Characterising dark matter searches at colliders and direct detection experiments: vector mediators (2014, unknown): “Two-phase xenon detector technology has a proven track record through the ZEPLIN [75–77], XENON [78– 80] and LUX [81] programs and is scalable to the much larger target masses required to probe very small scattering cross-sections.”
- Liquid noble gas detectors for low energy particle physics (2012, methodology): “crimination efficiency (which decreases for low energies, as illustrated in Figures 4 and 5. For example, the ZEPLIN-III and XENON100 experiments used similar thresholds of ˇ10 keV for nuclear recoils [56, 57]. Recoil energy can be reconstructed both from S1 and S2 signals, none of the methods being ”
- The Large Underground Xenon (LUX) experiment (2012, background): “Two-phase liquid xenon detectors use a powerful new technology for the detection of dark matter [1, 2, 3, 4, 5, 6].”
- Dark matter direct-detection experiments (2015, methodology): “The exclusion limits on the coupling of dark matter particles to nuclei placed by these detectors were most constraining at that time [213][348].”
- Colloquium: Annual modulation of dark matter (2013, unknown): “…2011), SIMPLE (Felizardo et al., 2012), TEXONO (Lin et al., 2009), WArP (Acciarri et al., 2011), XENON10 (Angle et al., 2008, 2011; Aprile et al., 2011b), XENON100 (Aprile et al., 2012b, 2012c), XENON1T (Aprile, 2012a), XMASS (Moriyama, 2011), ZEPLIN (Akimov et al., 2007, 2012), and many others.”