non standard interactions with light mediators
play

Non-Standard Interactions with light mediators Yasaman Farzan IPM, - PowerPoint PPT Presentation

Non-Standard Interactions with light mediators Yasaman Farzan IPM, Tehran Effects of NSI on neutrinos Neutral current Non-Standard Interaction (NSI): propagation of neutrinos in matter Charged current Non-Standard Interaction (NSI):


  1. Non-Standard Interactions with light mediators Yasaman Farzan IPM, Tehran

  2. 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

  3. 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

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

  5. Standard Oscillation

  6. Non-Standard matter effects

  7. 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

  8. LMA-Dark solution ´ LMA-Dark solution provides even a better fit. (suppression of low energy upturn)

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

  10. 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

  11. 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

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

  13. Too small NSI

  14. 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

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

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

  17. Bounds on Couplings of neutrinos

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

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

  20. 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

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

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

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

  24. Anomaly cancelation: Reproducing best fit

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

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

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

  28. Neutrino scattering experiments Suppression factor

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

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

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

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

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

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

  35. 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

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

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

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

  39. LMA-Dark after COHERENT data Denton, YF Shoemaker, arXiv:1804.03660, to appear in JHEP

  40. Denton, YF Shoemaker, arXiv:1804.03660, to appear in JHEP

  41. Even lighter mediator Hardy and Lasenby,JHEP 1702 (2017) 33 Free streaming at recombination: Cherry, Denton, YF and Shoemaker, Work in progress

  42. 1 . 0 Cherry, Denton, Y.F. and shoemaker, Work in progress 0 . 8 P ( ν µ → ν µ ) 0 . 6 0 . 4 Liao and Marfatia, PRL 117 (2016) 71802 0 . 2 0 . 0 10 0 10 1 E ν [TeV]

  43. 1 . 0 Cherry, Denton, Y.F. and shoemaker, Work in progress 0 . 8 ν µ ) 0 . 6 ν µ → ¯ P (¯ 0 . 4 Liao and Marfatia, PRL 117 (2016) 71802 0 . 2 0 . 0 10 0 10 1 E ν [TeV]

  44. 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

  45. Backup slides

  46. ´ Observational consequences

  47. Emission in Supernova ´ Similar to Kamada and Yu, arXiv:1504.00711 ´ Reduced mean free path for

  48. High energy cosmic neutrino ´ Kamada and Yu, arXiv:1504.00711 Background neutrino at rest

  49. Dip or gap in ICECUBE spectrum

  50. ´ Theoretical prediction of dip in 400 TeV to PeV is robust! ´ Testing model

  51. Maltoni and Gonzalez-Garcia, JHEP 2013

  52. Kamada and Yu, 1504.00711

  53. Yukawa coupling of neutrinos Basis change: Mix: No mixing:

  54. Majorana masses If there is no Majorana mass for right-handed neutrinos: 1) 2) Smallness of neutrino mass

  55. Majorana masses

  56. Neutrino trident scattering ´ CCFR collaboration: PRL66 (1991) ´ CHARM II collaboration PLB 245 (1990)

  57. Neutrino trident scattering Altmannshofer et al., PRL113 (2014)

  58. Davidson, Pena-Garay, Rius, SantaMaria, JHEP 2003 NuTeV: Muon neutrino energy~75 GeV

  59. Davidson, Pena-Garay, Rius, SantaMaria, JHEP 2003

  60. Standard coherent interaction

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend