4.4 Article

Time-integrated luminosity recorded by the BABAR detector at the PEP-II e+e- collider

出版社

ELSEVIER SCIENCE BV
DOI: 10.1016/j.nima.2013.04.029

关键词

BABAR; Integrated luminosity; Electron-positron collider; PEP-II

资金

  1. US Department of Energy and National Science Foundation
  2. Natural Sciences and Engineering Research Council (Canada)
  3. Commissariat a l'Energie Atomique and Institut National de Physique Nucleaire et de Physique des Particules (France)
  4. Bundesministerium fur Bildung und Forschung and Deutsche Forschungsgemeinschaft (Germany)
  5. Istituto Nazionale di Fisica Nucleare (Italy)
  6. Foundation for Fundamental Research on Matter (The Netherlands)
  7. Research Council of Norway
  8. Ministry of Education and Science of the Russian Federation
  9. Ministerio de Ciencia e Innovacion (Spain)
  10. Science and Technology Facilities Council (United Kingdom)
  11. Marie-Curie IEF program (European Union)
  12. A. P. Sloan Foundation (USA)
  13. STFC [ST/K001604/1] Funding Source: UKRI
  14. Science and Technology Facilities Council [ST/K001604/1 SuperNEMO, ST/K001604/1 LHCb, ST/K001604/1 T2K, ST/K001604/1, ST/K001604/1 MICE/UKNF, ST/K001604/1 GRIDPP, ST/K001604/1 LHCb Upgrades, ST/K001604/1 DMUK, ST/K001604/1 CMS Upgrade] Funding Source: researchfish
  15. Direct For Mathematical & Physical Scien
  16. Division Of Physics [0969487] Funding Source: National Science Foundation

向作者/读者索取更多资源

We describe a measurement of the time-integrated luminosity of the data collected by the BABAR experiment at the PEP-II asymmetric-energy e(+)e(-) collider at the Upsilon(4S), Upsilon(3S), and Upsilon(2S) resonances and in a continuum region below each resonance. We measure the time-integrated luminosity by counting e(+)e(-)-> e(+)e(-) and (for the Upsilon(4S) only) e(+)e(-)->mu(+)mu(-) candidate events, allowing additional photons in the final state. We use data-corrected simulation to determine the cross-sections and reconstruction efficiencies for these processes, as well as the major backgrounds. Due to the large cross-sections of e(+)e(-)-> e(+)e(-) and e(+)e(-)->mu(+)mu(-), the statistical uncertainties of the measurement are substantially smaller than the systematic uncertainties. The dominant systematic uncertainties are due to observed differences between data and simulation, as well as uncertainties on the cross-sections. For data collected on the Upsilon(3S) and Upsilon(2S) resonances, an additional uncertainty arises due to Upsilon -> e(+)e(-)X background. For data collected off the Upsilon resonances, we estimate an additional uncertainty due to time dependent efficiency variations, which can affect the short off-resonance runs. The relative uncertainties on the luminosities of the on-resonance (off-resonance) samples are 0.43% (0.43%) for the Upsilon(4S), 0.58% (0.72%) for the Upsilon(3S), and 0.68% (0.88%) for the Upsilon(2S). (C) 2013 Elsevier B.V. All rights reserved.

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