Published April 1, 2009 | Version v1
Journal article

The scintillation and ionization yield of liquid xenon for nuclear recoils

  • 1. Department of Physics, Brown University, Providence, RI 02912 (United States)
  • 2. Department of Physics, Yale University, New Haven, CT 06511 (United States)
  • 3. Department of Physics, Princeton University, Princeton, NJ 08540 (United States)
  • 4. Department of Physics, University of Florida, Gainesville, FL 32611 (United States)
  • 5. Physics Institute, University of Zuerich, Winterthurerstrasse 190, CH-8057 Zuerich (Switzerland)
  • 6. Department of Physics, Columbia University, New York, NY 10027 (United States)
  • 7. Gran Sasso National Laboratory, Assergi, L'Aquila 67010 (Italy)
  • 8. Lawrence Livermore National Laboratory, 7000 East Ave., Livermore, CA 94550 (United States)
  • 9. Department of Physics, Case Western Reserve University, Cleveland, OH 44106 (United States)
  • 10. Department of Physics, University of Coimbra, R. Larga, 3004-516 Coimbra (Portugal)
  • 11. Department of Physics and Astronomy, Rice University, Houston, TX 77251 (United States)

Description

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 Leff and the absolute ionization yield Qy, for nuclear recoils in xenon. A dark matter particle is expected to deposit energy by scattering from a xenon nucleus. Knowledge of Leff is therefore crucial for establishing the energy threshold of the experiment; this in turn determines the sensitivity to particle dark matter. Our Leff measurement is in agreement with recent theoretical predictions above 15 keV nuclear recoil energy, and the energy threshold of the measurement is ∼4keV. A knowledge of the ionization yield Qy is necessary to establish the trigger threshold of the experiment. The ionization yield Qy is measured in two ways, both in agreement with previous measurements and with a factor of 10 lower energy threshold.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.nima.2008.12.197

Additional details

Identifiers

DOI
10.1016/j.nima.2008.12.197;
arXiv
arXiv:0807.0459v2;
PII
S0168-9002(09)00012-6;

Publishing Information

Journal Title
Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment
Journal Volume
601
Journal Issue
3
Journal Page Range
p. 339-346
ISSN
0168-9002
CODEN
NIMAER

Optional Information

Copyright
Copyright (c) 2009 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.