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Search for Lepton-number Violating Processes

Search for Lepton-number Violating Processes. Pheno 2006 Anupama Atre. Neutrinos are massive. We also know There are only three “active” light neutrinos N  = 2.984 § 0.008, from Z pole at LEP-1. Direct lab bound: m  < 2.2 eV from Tritium beta decay

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Search for Lepton-number Violating Processes

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  1. Search for Lepton-number Violating Processes Pheno 2006 Anupama Atre

  2. Neutrinos are massive Anupama Atre

  3. We also know • There are only three “active” light neutrinos • N = 2.984 § 0.008, from Z pole at LEP-1. • Direct lab bound: m < 2.2 eV • from Tritium beta decay •  mi < 0.17 – 1 eV • from WMAP, SDSS (Ly spectra), SNIa. • The absence of neutrinoless double beta decay • bound on Majorana mass <m> ee < 1 eV Anupama Atre

  4. m3 m2 m2s m1 m2a m2a m2 m2s m1 m3 Inverted Normal • Absolute mass scale ? • Hierarchy – inverted or normal? • Dirac or Majorana? Anupama Atre

  5. Anupama Atre

  6. Anupama Atre

  7. Charged current and Neutral current Anupama Atre

  8. The transition rates are proportional to: • for light neutrino [1] • for intermediate mass neutrino [2] • for heavy neutrino [3] f1’ f1 [1] AA, V Barger, T Han, Phys. Rev. D 71, 113014 (2005) [arXiv:hep-ph/0502163] f2 f2’ [2] AA, T Han, S Pascoli to appear [3] T Han, B Zhang [arXiv:hep-ph/0604064] AA, T Han, S pascoli, B Zhang to appear L = 2 process  Majorana nature of neutrino generic diagram Anupama Atre

  9. f1’ f1 We have six effective neutrino masses : 0 , rare meson decay :  decay : - e+ conversion, rare meson decay :  decay : rare meson decay : none f2 f2’ Light (active) Majorana neutrino Anupama Atre

  10. Determination of effective neutrino masses • 3 masses: m1, m2 and m3 •  = m1 + m2 + m3 and •  m2a and  m2s • 3 mixing angles: a, s and x • 3 phases: , 2 and 3 AA, V Barger, T Han, Phys. Rev. D 71, 113014 (2005) [arXiv:hep-ph/0502163] Anupama Atre

  11. Anupama Atre

  12. (A,Z) Nuclear Physics (A,Z+2) = 0.14 (0.06) eV Neutrinoless Double Beta Decay (0) S.R. Elliott and J. Engel, J. Physics G30 (2004) R183, [arXiv:hep-ph/0405078] Anupama Atre

  13. Lepton Number Violating Tau Decays CLEO Collaboration, D.Bliss et al., Phys. Rev. D 57 (1998) 5903, [arXiv:hep-ex/9712010] Anupama Atre

  14. Rare Meson Decays Anupama Atre

  15. ·17(82) MeV SINDRUM II Collaboration, J. Kaulard et al., Phys. Lett. B 422 (1998) 334 Nuclear Physics (A,Z-2) (A,Z) Muon – Positron Conversion K. Zuber, [arXiv:hep-ph/0008080] Anupama Atre

  16. Summary * 90 GeV from K+ - e++ Anupama Atre

  17. f1’ f1 f2 f2’ Intermediate mass Majorana neutrino * • resonant enhancement, transition rates • tau decay, rare meson decay Anupama Atre * AA, T Han and S Pascoli, to appear

  18. Width of Intermediate mass Majorana neutrino • 2 body decays : • CC decays  • NC decays  • 3 body decays: • CC decays  • NC decays  • CC + NC decays  combination of CC + NC mixings Anupama Atre

  19. 36 decay modes to look for lepton number violation !!!! • Parameters for MC sampling • mass of neutrino m4 • resonant mass region • three mixings ~ 0 to 1 Anupama Atre

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  25. Current bounds on sterile neutrino: • peak searches • accelerator searches • heavy atmospheric neutrinos • cosmology, BBN, WMAP Anupama Atre

  26. It is of fundamental importance to verify Majorana nature of neutrinos • We look for genuine  L = 2 processes • For the three active ’s 0 is the best hope • For a sterile neutrino N (or 4) • Rare  and meson decays are sensitive to 140 MeV < m4 < 5 GeV, 10-9 < |V l4|2 < 10-2 • Depending on the unknown mixing and mass 4 can show up in any channel • Other processes to look for B+ e++ M-, B+ ++ M-, B+ ++ M- Anupama Atre

  27. Thank You !!!!! Anupama Atre

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