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Non-Standard Interactions of neutrinos Yasaman Farzan IPM, Tehran Standard Neutrino interactions Charged current coupling to electroweak gauge boson: Neutral current coupling to electroweak gauge boson: Broad meaning of NSI Effective


  1. Non-Standard Interactions of neutrinos Yasaman Farzan IPM, Tehran

  2. Standard Neutrino interactions ´ Charged current coupling to electroweak gauge boson: ´ Neutral current coupling to electroweak gauge boson:

  3. Broad meaning of NSI ´ Effective NSI with matter fields ´ New gauge interaction for neutrinos ´ Yukawa interaction

  4. Effects of NSI on neutrinos ´ Neutral current Non-Standard Interaction (NSI): propagation of neutrinos in matter ´ Charged current Non-Standard Interaction (NSI): production and detection

  5. Effects of NSI on neutrinos ´ Neutral current Non-Standard Interaction (NSI): propagation of neutrinos in matter Focus of this talk ´ Charged current Non-Standard Interaction (NSI): production and detection

  6. Non-standard neutral current interaction Projection Matter field matrix Neutrino propagation:

  7. Standard Oscillation

  8. In parenthesis

  9. Non-Standard matter effects

  10. Effects of NSI in long baseline experiments ´ Renewed interest in NSI ´ NSI can fake CP-violation and lead to wrong determination of octant Masud and Mehta, PRD 94(2016); Forero and Huber, PLB 117 (2016); Liao, Marfatia and Whistnant PRD 93 (2016); Agarwalla, Chatterjee and Palazzo, PLB 762 (2016) Underlying models for NSI with light mediators Y.F., PLB 748 (2015) 311; Y.F. and I. Shoemaker, JHEP 1607 (2016) 033; Y.F. and J. Heeck, PRD94 (2016) no 5, 53010, Y.F. and M. Tortola, Front. In Phys 6 (2018) 10; J. Heeck, M. Lindner, W. Rodejohann and Vogl, arXiv:1812.04067

  11. LMA-Dark solution to the solar neutrino anomaly ´ LMA-Dark solution provides even a better fit. (suppression of low energy upturn) Miranda, Tortola, Valle, JHEP 2004

  12. Total solar neutrino flux measurement at SNO ´ Neutral current ´ Deuteron dissociation ´ Gamow-Teller transition ´ Sensitive only to axial-vector interaction ´ No effect from

  13. Scattering experiments NuTeV and CHARM rule out a large part (but not all) of parameter space of LMA-Dark solution. Davidson, Pena-Garay, Rius, SantaMaria, JHEP 2003

  14. Scattering experiments NuTeV and CHARM rule out a large part (but not all of) parameter space of LMA-Dark solution. Davidson, Pena-Garay, Rius, SantaMaria, JHEP 2003 But not in the model that we shall present

  15. Underlying theory for LMA-Dark? Various model with heavy intermediate particle For a review see:

  16. Too small NSI

  17. Suggestion ´ What if YF, A model for large non-standard interactions leading to LMA-Dark solution, Phys. Lett. B748 (2015) 311-315; YF and J Heeck, Neutrinophilic nonstandard interactions, PRD 94 (2016) 53010; YF and I Shoemaker, lepton flavor violating NSI via light mediator, JHEP 1607 (2016) 33. YF and M Tortola, “neutrino oscillations and non-standard interactions” to appear in Frontiers in Physics; J. Heeck, M. Lindner, W. Rodejohann and Vogl, arXiv:1812.04067

  18. Suggestion ´ What if ´ Bounds can be avoided not because the mass of the intermediate state is high But because coupling is small!

  19. Big Bang Nucleosynthesis ´ Huang, Ohlsson and Zhou, PRD 97 (2018) 75009

  20. Bounds on Couplings of neutrinos Barger et al, PRL 108 (2012); Laha et al, PRD 89 (2014); Pospelov, PRD 8 (2009)

  21. Constraining secret gauge interactions of neutrinos by meson decay Pouya Bakhti and YF, arXiv:1702.04187

  22. Suppression of two-body decay versus enhancement of three body decay

  23. NA62 bound Lazzeroni et al [NA62 collaboration] PRD 79 (2009) 326

  24. P Bakhti and YF, PRD 95 (2017) 095008

  25. Artamonov et al., BNL-E494 collaboration, PRD 79 (2009) 092004 P Bakhti and YF, PRD 95 (2017) 095008

  26. Coupling to quarks ´ Non-chiral couplings: No impact on total measurement at SNO ´ Flavor universal: Going to mass basis Y.F. and J Heeck, PRD 94 (2016) 053010

  27. Coupling to fermion Direct coupling to neutrinos Gauge symmetry: Coupling to neutrinos through mixing with : Gauge symmetry:

  28. Coupling to neutrinos ´ Direct coupling to neutrinos Gauge symmetry:

  29. Harnik, Kopp and Machado, JCAP 1207 (2012) 026

  30. Anomaly cancelation: Reproducing best fit

  31. Anomaly free combinatons J. Heeck, M. Lindner, W. Rodejohann and Vogl, arXiv:1812.04067

  32. Anomaly cancelation Adding a new generation of leptons (quarks) Non-perturbative Yukawa coupling Adding a pair of fermions with opposite hypercharges

  33. Coupling to neutrinos Direct coupling to neutrinos Gauge symmetry: Coupling to neutrinos through mixing with : Gauge symmetry:

  34. Coupling of neutrinos through mixing Fernandez-Martinez et al., JHEP 08 (2016) 033

  35. Coupling of neutrinos through mixing Fernandez-Martinez et al., JHEP 08 (2016) 033

  36. Neutrino scattering experiments Suppression factor

  37. Neutrino scattering experiments Relaxing bounds from scattering experiments, NuTeV and CHARM

  38. YF and J Heeck, PRD94 (2016) 053010 LUX-Zeplin SuperCDMS SNOLAB

  39. COHERENT experiment Coloma et al, JHEP 1704 (2017) 116 Neutrino source: Pion decay at rest

  40. COHERENT experiment ´ Akimov et al., “Observation of Coherent Elastic neutrino Nucleus Scattering,” science 357 (2017) No 6356, 1123 Freedman, PRD 9 (1974) 1389.

  41. Set-up of the COHERENT experiment ´ Detector: 14.6 kg CsI scintillator ´ Source: Spallation Neutron Source (SNS) at Oak Ridge National Lab

  42. Akimov et al., Science 357 (2017) No 6356, 1123

  43. JHEP 1704 (2017) 116 P. Coloma, P. Denton, Gonzalez-Garcia, Maltoni and Schwetz, “curtailing the dark Side in non-standard neutrino interaction,” JHEP 1704 (2017) 116 Akimov et al., Science 357 (2017) No 6356, 1123

  44. Esteban et al., JHEP 1808 (2018) 180

  45. Standard coherent interaction Liao and Marfatia, Phys Lett B775 (2017) 54

  46. Coherent interaction with light mediator Liao and Marfatia, Phys Lett B775 (2017) 54

  47. Liao and Marfatia, Phys Lett B775 (2017) 54

  48. LMA-Dark after COHERENT data Denton, YF Shoemaker, JHEP 1807 (2018) 037 , arXiv:1804.03660

  49. Denton, YF Shoemaker, JHEP 1807 (2018) 037, arXiv:1804.03660

  50. Solar neutrino interaction at DM direct 51 detection experiments Y.F. and J. Heeck, PRD94 (2016); Cerdeno et al,JHEP 05 (2016) 118 12/15/18 Yasaman Farzan

  51. LMA-DARK solution 52 Viable Z’ mass range BBN+CMB CONUS, COHERENT Future solar No Dip is cosmic neutrino spectrum 12/15/18 Yasaman Farzan

  52. Summary gauge boson with and ´ can lead to sizeable NSI. ´ COHERENT has not ruled out LMA-Dark yet! ´ Upcoming CE ν NS experiments can test this scenario

  53. Yukawa interaction 54 Y. Farzan, M. Lindner, Rodejohann and X-J Xu, 12/15/18 Yasaman Farzan JHEP 1805 (2018) 066

  54. Effects of LNV Yukawa on BBN 55 ´ Heavy scalar decays to neutrinos before neutrino decoupling ´ Lighter ones can contribute to extra relativistic degrees of freedom. 12/15/18 Yasaman Farzan

  55. 56 Huang, Ohlsson and Zhou, PRD 97 (2018) 075009 12/15/18 Yasaman Farzan

  56. LNC Yukawa and early universe 57 12/15/18 Yasaman Farzan

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