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The current landscape The current landscape of neutrino physics of neutrino physics José W F Valle http://astroparticles.es/ Laboratori Nazionali di Frascati - Infn, Feb 2015

The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

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Page 1: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

The current landscape The current landscape 

of neutrino physicsof neutrino physicsJosé W F Valle

http://astroparticles.es/

Laboratori Nazionali di Frascati - Infn, Feb 2015

Page 2: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

Page 3: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

Page 4: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

Page 5: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

Page 6: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

Page 7: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

Page 8: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

confirmed

Page 9: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

confirmed

Page 10: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Where do neutrinos come from?336 / cm3: bilions of Cosmic neutrinos Cross us every second

Needto reviseStandardmodel

confirmed

Page 11: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

The Standard Model up to energies ~ 100 GeV is the most

precise theory of particle interactions we have

Page 12: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

The Standard Model up to energies ~ 100 GeV is the most

precise theory of particle interactions we have

based on gauge principle and the Higgs mechanism

BEH

Page 13: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 With the historic Higgs discovery

SM complete

Page 14: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 With the historic Higgs discovery

complete were it not forneutrinos & cosmology

Page 15: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 With the historic Higgs discovery

complete were it not forneutrinos & cosmology

no neutrino massesno dark matterno baryon asymmetryno inflation

Page 16: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 Neutrinos &Invisible Higgs 

http://arxiv.org/abs/1502.01649

Page 17: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 Neutrinos &Invisible Higgs 

http://arxiv.org/abs/1502.01649

Page 18: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 Neutrinos &Invisible Higgs 

http://arxiv.org/abs/1502.01649

Page 19: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 Neutrinos &Invisible Higgs 

http://arxiv.org/abs/1502.01649

Page 20: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

 Neutrinos &Invisible Higgs 

http://arxiv.org/abs/1502.01649

Page 21: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Schechter & JV PRD22 (1980) 2227 & PDG

LEPTONIC CKM MATRIXLEPTONIC CKM MATRIX

Rodejohann, JV Phys.Rev. D84 (2011) 073011

Page 22: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Schechter & JV PRD22 (1980) 2227 & PDG

LEPTONIC CKM MATRIXLEPTONIC CKM MATRIX

Rodejohann, JV Phys.Rev. D84 (2011) 073011

Page 23: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

THE ERA OF LEPTONIC CPV STARTS 

Page 24: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

ORIGIN OF NEUTRINO MASS AND SEESAW

Page 25: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

SCALE

MECHANISM

FLAVOR STRUCTURE

ORIGIN OF NEUTRINO MASS AND SEESAW

Page 26: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

SCALE

MECHANISM

FLAVOR STRUCTURE

ORIGIN OF NEUTRINO MASS AND SEESAW

Page 27: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Minkowski 77 Gellman Ramond Slansky 80 Glashow, Yanagida 79 Mohapatra Senjanovic 80 Lazarides Shafi Weterrich 81 Schechter-Valle, 80 & 82

fermion exchangeTYPE I

ORIGIN OF NEUTRINO MASS AND SEESAW

SCALE

MECHANISM

FLAVOR STRUCTURE

Page 28: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Schechter-Valle 80/82 Minkowski 77 Gellman Ramond Slansky 80 Glashow, Yanagida 79 Mohapatra Senjanovic 80 Lazarides Shafi Weterrich 81 Schechter-Valle, 80 & 82

fermion exchangeTYPE I

Scalar-exchange TYPE II

ORIGIN OF NEUTRINO MASS AND SEESAW

SCALE

MECHANISM

FLAVOR STRUCTURE

Page 29: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Schechter-Valle 80/82 Minkowski 77 Gellman Ramond Slansky 80 Glashow, Yanagida 79 Mohapatra Senjanovic 80 Lazarides Shafi Weterrich 81 Schechter-Valle, 80 & 82

fermion exchangeTYPE I

Scalar-exchange TYPE II

ORIGIN OF NEUTRINO MASS AND SEESAW

Number & properties of messengers

SCALE

MECHANISM

FLAVOR STRUCTURELOW-SCALE SEESAW Mohapatra-Valle 86Akhmedov et al PRD53 (1996) 2752 Malinsky et al PRL95(2005)161801 Bazzocchi et al, PRD81 (2010) 051701

Page 30: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Radiative neutrino mass in 331 scheme

Singer, Valle, Schechter, Phys.Rev. D22 (1980) 738

# generations = # coloursGauge vs Higgs

Page 31: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Radiative neutrino mass in 331 scheme

Singer, Valle, Schechter, Phys.Rev. D22 (1980) 738

# generations = # coloursGauge vs Higgs

Page 32: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Radiative neutrino mass in 331 scheme

Singer, Valle, Schechter, Phys.Rev. D22 (1980) 738

# generations = # coloursGauge vs Higgs

Page 33: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Radiative neutrino mass in 331 scheme

Singer, Valle, Schechter, Phys.Rev. D22 (1980) 738

# generations = # coloursGauge vs Higgs

arXiv:1404.3751many other low-scale neutrino mass schemes ...

Page 34: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

gauge coupling unification : a near miss in SM ?

Boucenna, Fonseca, Gonzalez-Canales, JV arXiv:1411.0566

Page 35: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

gauge coupling unification : a near miss in SM ?

What makes the gauge couplings unify? - A GUT (p decay)

Boucenna, Fonseca, Gonzalez-Canales, JV arXiv:1411.0566

Page 36: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

gauge coupling unification : a near miss in SM ?

What makes the gauge couplings unify? - A GUT (p decay) - SUSY (LHC-II)

Boucenna, Fonseca, Gonzalez-Canales, JV arXiv:1411.0566

Page 37: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

gauge coupling unification : a near miss in SM ?

What makes the gauge couplings unify? - A GUT (p decay) - SUSY (LHC-II) - NEUTRINO PHYSICS

The physics responsible for gauge coupling unification may also induce small neutrino masses

Boucenna, Fonseca, Gonzalez-Canales, JV arXiv:1411.0566

Page 38: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Order in the chaos?

FLAVOR GUT

Flavor symmetries have the potential of relating Q & L masses ...

Page 39: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Order in the chaos?

FLAVOR GUT

Flavor symmetries have the potential of relating Q & L masses ...

Morisi et al Phys.Rev. D84 (2011) 036003

Page 40: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Order in the chaos?

FLAVOR GUT

Morisi et al Phys.Rev. D88 (2013) 036001

King et al Phys. Lett. B 724 (2013) 68

Bonilla et al

Flavor symmetries have the potential of relating Q & L masses ...

Phys.Lett. B742 (2015) 99

Morisi et al Phys.Rev. D84 (2011) 036003

Page 41: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

CHARGED LEPTONS

Sectors are separatedSectors are separatedby an extra Abelian Znby an extra Abelian Zn

FLAVORSYMMETRY

Page 42: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

CHARGED LEPTONS

Sectors are separatedSectors are separatedby an extra Abelian Znby an extra Abelian Zn

Babu-Ma-Valle PLB552 (2003) 207Hirsch et al PRD69 (2004) 093006

A4

FLAVORSYMMETRY

Page 43: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

CHARGED LEPTONS

Sectors are separatedSectors are separatedby an extra Abelian Znby an extra Abelian Zn

Babu-Ma-Valle PLB552 (2003) 207Hirsch et al PRD69 (2004) 093006

A4

FLAVORSYMMETRY

Tri-BiMaximal ansatz Harrison, Perkins, Scott 2000

(CP assummed)

Page 44: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

CHARGED LEPTONS

Sectors are separatedSectors are separatedby an extra Abelian Znby an extra Abelian Zn

A4

Tri-BiMaximal ansatz Harrison, Perkins, Scott 2000

(CP assummed)

Altarelli, Feruglio 2005

FLAVORSYMMETRY

Babu-Ma-Valle PLB552 (2003) 207Hirsch et al PRD69 (2004) 093006

Page 45: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Gflavor

FLASY2011, 2012,2013, 2014, 2015 Jun29-Jul2

Page 46: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Gflavor

Deviationof TBM

Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1

Holthausen et al 1212.2411

Page 47: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

change ansatz:

Albright,Dueck,Rodejohann 1004.2798

Gflavor

Deviationof TBM

Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1

Holthausen et al 1212.2411

Page 48: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

change ansatz:

Albright,Dueck,Rodejohann 1004.2798

Gflavor

Deviationof TBM

Abelian Ding, Morisi, JV PRD87 (2013) 1211.6506

Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1

Holthausen et al 1212.2411

Boucenna,M,Tortola, JVPRD86 (2012) 051301

Page 49: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

change ansatz:

Albright,Dueck,Rodejohann 1004.2798

Gflavor

Deviationof TBM

AnarchyDonoghue et al PRD73Hall,Murayama,Weiner,PRLAltarelli, Feruglio,Masina,JHEP

Abelian Ding, Morisi, JV PRD87 (2013) 1211.6506

Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1

Holthausen et al 1212.2411

Boucenna,M,Tortola, JVPRD86 (2012) 051301

Page 50: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

change ansatz:

Albright,Dueck,Rodejohann 1004.2798

Gflavor

Deviationof TBM

AnarchyDonoghue et al PRD73Hall,Murayama,Weiner,PRLAltarelli, Feruglio,Masina,JHEP

Abelian Ding, Morisi, JV PRD87 (2013) 1211.6506

Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1

Holthausen et al 1212.2411

Flavor roadmap Fortsch.Phys. 61 (2013) 466-492 

Boucenna,M,Tortola, JVPRD86 (2012) 051301

Page 53: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

OSCILLATION PARAMETER CORRELATIONS

Boucenna et alPhysRevD.86.073008

Page 54: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

OSCILLATION PARAMETER CORRELATIONS

Boucenna et alPhysRevD.86.073008

Dorame et al Nucl Phys B861, 259–270

Page 55: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

OSCILLATION PARAMETER CORRELATIONS

Boucenna et alPhysRevD.86.073008

Dorame et al Nucl Phys B861, 259–270Bonilla et al Phys.Lett. B742 (2015) 99

Page 56: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Bi­large mixing & Cabibbo angle Boucenna et al, Phys. Rev. D 86, 051301(R)

Page 57: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Bi­large mixing & Cabibbo angle

reactor seeds solar & atmBoucenna et al, Phys. Rev. D 86, 051301(R)

Page 58: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Bi­large mixing & Cabibbo angle

reactor seeds solar & atmBoucenna et al, Phys. Rev. D 86, 051301(R)

Page 59: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Bi­large mixing & Cabibbo angle

reactor seeds solar & atmBoucenna et al, Phys. Rev. D 86, 051301(R)

arXiv:1410.3658

Abelian Flavor Models Ding, et al Phys.Rev. D87 (2013) 053013 Roy, Singh, ..arXiv:1211.7207

Page 60: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

A.S. Barabash arXiv:1104.2714

Neutrinoless Double Beta Decay

Page 61: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Family symmetry dependent lower bound

A.S. Barabash arXiv:1104.2714

Bonilla et al arXiv:1411.4883

Neutrinoless Double Beta Decay and flavor

Page 62: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Family symmetry dependent lower bound

A.S. Barabash arXiv:1104.2714

Bonilla et al arXiv:1411.4883

Dorame et alNPB861 (2012) 259-270

PhysRevD.86.056001 King et al Phys. Lett. B 724 (2013) 68

Neutrinoless Double Beta Decay and flavor

Page 63: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Schechter, JWFV 82Lindner et al JHEP 1106 (2011) 091

A.S. Barabash arXiv:1104.2714

Neutrinoless Double Beta Decay significance

Page 64: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Neutrinoless Double Beta Decay

Schechter, JWFV 82Lindner et al JHEP 1106 (2011) 091

Short versus long­range and the LHC

A.S. Barabash arXiv:1104.2714

Page 65: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Neutrinoless Double Beta Decay

Schechter, JWFV 82Lindner et al JHEP 1106 (2011) 091

Short versus long­range and the LHC

A.S. Barabash arXiv:1104.2714

Page 66: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Neutrinos affect the CMB and large scale structure in the Universe …

BIGBANG

Page 67: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Neutrinos affect the CMB and large scale structure in the Universe …

are key in the synthesis of light elements

BIGBANG

Page 68: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Neutrinos affect the CMB and large scale structure in the Universe …

are key in the synthesis of light elements

can “probe” the Universe earlier than photons …

BIGBANG

Page 69: The current landscape of neutrino physics · Albright,Dueck,Rodejohann 1004.2798 Gflavor Deviation of TBM Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

Boucenna et al arXiv:1405.2332

type-I seesaw

PRD90 (2014) 055023

SEESAW INFLATION  & MAJORON DARK MATTER  

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Boucenna et al arXiv:1405.2332

type-I seesaw

PRD90 (2014) 055023

SEESAW INFLATION  & MAJORON DARK MATTER  

but http://arxiv.org/pdf/1502.00612v1

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DARK MATTER MAJORONS Berezinsky, Valle PLB318 (1993) 360

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DARK MATTER MAJORONS Berezinsky, Valle PLB318 (1993) 360

Lattanzi & Valle, PRL99 (2007) 121301Lattanzi & Valle, PRL99 (2007) 121301

Esteves et al, PRD 82, 073008 (2010)

Bazzocchi & al JCAP 0808 (2008) 013Bazzocchi & al JCAP 0808 (2008) 013

Consistency with CMB

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DARK MATTER MAJORONS Berezinsky, Valle PLB318 (1993) 360

Lattanzi & Valle, PRL99 (2007) 121301Lattanzi & Valle, PRL99 (2007) 121301

Esteves et al, PRD 82, 073008 (2010)

Bazzocchi & al JCAP 0808 (2008) 013Bazzocchi & al JCAP 0808 (2008) 013

Lattanzi et al PRD88 (2013) 063528

Consistency with CMB

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DARK MATTER MAJORONS Berezinsky, Valle PLB318 (1993) 360

Lattanzi & Valle, PRL99 (2007) 121301Lattanzi & Valle, PRL99 (2007) 121301

Esteves et al, PRD 82, 073008 (2010)

Bazzocchi & al JCAP 0808 (2008) 013Bazzocchi & al JCAP 0808 (2008) 013 128

Lattanzi et al PRD88 (2013) 063528

Consistency with CMB

Aristizabal et al arXiv:1405.4706

– Leptogenesis in dynamical seesaw JCAP

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DARK MATTER STABILITY FROM FLAVOUR SYMMETRY  

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DARK MATTER STABILITY FROM FLAVOUR SYMMETRY  

accidental? Lavoura, Morisi, JV JHEP 1302(2013) 118 unbroken subgroup

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DARK MATTER FROM FLAVOUR SYMMETRY  

Z2 PARITY

HIGGS PORTAL DIRECT DETECTION

accidental? Lavoura, Morisi, JV JHEP 1302(2013) 118 unbroken subgroup

Boucenna et al

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ISBN: 978-3-527-41197-9456 pagesFebruary 2015

Thank you !! more at

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Now the back up slides 

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Lightest neutralino decay length

De Campos et al Phys.Rev. D86 (2012) 075001

LIGHTEST NEUTRALINO DECAYS: PROBING NEUTRINOS @ LHC

Lightest neutralino decay correlates with atm angle

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decaying Gravitino dark matterdecaying Gravitino dark matter    decays suppressed by Planck mass & smallness of m-nu

chosen to fit neutrino osc. data

excluded by gamma line searches @

Egret & Fermi-LAT

relic abundance

+ LHC searches

Restrepo et al PRD85 (2012) 023523 LHCLHC

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Forero, Tortola, JWFV arXiv:1405.7540Oscillations after nu2014

Double Chooz: 467.9 days [arXiv:1406.7763]RENO: 800 days [talk by Seon-Hee Seo@ICHEP2014]Daya Bay: 621 days of data (6AD + 8AD) [Talk by Chao Zhang@ICHEP2014]

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LSP is SNEUTRINO-like

instead of neutralino ..

Arina et al PRL101 (2008) 161802Bazzocchi, Cerdeno, Munoz, J.V., PRD81 (2010) 051701De Romeri, Hirsch, JHEP 1212 (2012) 106

If neutrinos get mass a la Inverse seesaw susy Spectrum can change so …

WIMP DARK MATTER