4.7 Article

T2K measurements of muon neutrino and antineutrino disappearance using 3.13 x 1021 protons on target

期刊

PHYSICAL REVIEW D
卷 103, 期 1, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevD.103.L011101

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资金

  1. MEXT, Japan
  2. NSERC, Canada [SAPPJ-2014-00031]
  3. NRC, Canada
  4. CFI, Canada
  5. CEA, France
  6. CNRS/IN2P3, France
  7. DFG, Germany
  8. INFN, Italy
  9. National Science Centre, Poland
  10. Ministry of Science and Higher Education, Poland
  11. RSF, Russia [19-12-00325]
  12. Ministry of Science and Higher Education, Russia
  13. MINECO, Spain
  14. ERDF funds, Spain
  15. SNSF, Switzerland
  16. State Secretary for Research and Innovation (SERI), Switzerland
  17. STFC, UK
  18. DOE, USA
  19. la Caixa Foundation [100010434, LCF/BQ/IN17/11620050]
  20. European Unions [713673, 754496, RISE-GA822070-JENNIFER2 2020, RISE-GA872549-SK2HK]
  21. JSPS, Japan
  22. Royal Society, UK
  23. French ANR [ANR-19-CE31-0001]
  24. DOE Early Career program, USA
  25. ERC (FP7)
  26. STFC [ST/S000739/1, 1947570, 2119274, ST/S000909/1, 1963041, 2067105, ST/S000933/1] Funding Source: UKRI
  27. Science and Technology Facilities Council [ST/S000879/1] Funding Source: researchfish

向作者/读者索取更多资源

The T2K experiment reported measurements of the parameters theta(23) and Delta m(32)(2) that govern the disappearance of muon neutrinos and antineutrinos. The experiment found no significant differences between the values of these parameters for muon neutrinos and antineutrinos. The data were consistent with a physical value for the mixing angle, supporting the three-flavor model of neutrino oscillations.
We report measurements by the T2K experiment of the parameters theta(23) and Delta m(32)(2), which govern the disappearance of muon neutrinos and antineutrinos in the three-flavor PMNS neutrino oscillation model at T2K's neutrino energy and propagation distance. Utilizing the ability of the experiment to run with either a mainly neutrino or a mainly antineutrino beam, muon-like events from each beam mode are used to measure these parameters separately for neutrino and antineutrino oscillations. Data taken from 1.49 x 10(21) protons on target (POT) in neutrino mode and 1.64 x 10(21) POT in antineutrino mode are used. The best-fit values obtained by T2K were sin(2)(theta(23)) = 0.51(-0.07)(+0.06) (0.43(-0.05)(+0.21)) and Delta m(32)(2) = 2.47(-0.09)(+0.08) (2.50(-0.13)(+0.18)) x 10(-3) eV(2)/c(4) for neutrinos (antineutrinos). No significant differences between the values of the parameters describing the disappearance of muon neutrinos and antineutrinos were observed. An analysis using an effective two-flavor neutrino oscillation model where the sine of the mixing angle is allowed to take nonphysical values larger than 1 is also performed to check the consistency of our data with the three-flavor model. Our data were found to be consistent with a physical value for the mixing angle.

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