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Neutrino pathways to cosmology Neutrino pathways to cosmology Jos W - - PowerPoint PPT Presentation

Neutrino pathways to cosmology Neutrino pathways to cosmology Jos W F Valle http://astroparticles.es / Frontiers of Fundamental Physics 2014, Marseille 1 Where do neutrinos come from? 336 / cm3: bilions of Cosmic neutrinos Cross us every


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http://astroparticles.es/

José W F Valle

Frontiers of Fundamental Physics 2014, Marseille

Neutrino pathways to cosmology Neutrino pathways to cosmology

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

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

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

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

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

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

confirmed

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

Necessary to revise Standard model

confirmed

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Schechter & JV PRD22 (1980) 2227 & PDG

LEPTONIC CKM-MATRIX LEPTONIC CKM-MATRIX

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

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Schechter & JV PRD22 (1980) 2227 & PDG

LEPTONIC CKM-MATRIX LEPTONIC CKM-MATRIX

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

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Schechter & JV PRD22 (1980) 2227 & PDG

LEPTONIC CKM-MATRIX LEPTONIC CKM-MATRIX

use this approx. in oscillation analyses

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

Forero, Tortola, JWFV arXiv:1405.7540

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Schechter & JV PRD22 (1980) 2227 & PDG

LEPTONIC CKM-MATRIX LEPTONIC CKM-MATRIX

use this approx. in oscillation analyses

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

Forero, Tortola, JWFV arXiv:1405.7540

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ORIGIN OF NEUTRINO MASS AND SEESAW

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SCALE MECHANISM FLAVOR STRUCTURE

ORIGIN OF NEUTRINO MASS AND SEESAW

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SCALE MECHANISM FLAVOR STRUCTURE

ORIGIN OF NEUTRINO MASS AND SEESAW

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SCALE MECHANISM

Minkowski 77

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

FLAVOR STRUCTURE

fermion exchange

TYPE I

ORIGIN OF NEUTRINO MASS AND SEESAW

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SCALE MECHANISM

Schechter-Valle 80/82

Minkowski 77

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

FLAVOR STRUCTURE

fermion exchange

TYPE I

Scalar-exchange

TYPE II

ORIGIN OF NEUTRINO MASS AND SEESAW

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SCALE MECHANISM

Schechter-Valle 80/82

Minkowski 77

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

FLAVOR STRUCTURE

fermion exchange

TYPE I

Scalar-exchange

TYPE II

ORIGIN OF NEUTRINO MASS AND SEESAW

Number & properties of messengers

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SCALE MECHANISM

Schechter-Valle 80/82

Minkowski 77

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

FLAVOR STRUCTURE LOW-SCALE SEESAW

Mohapatra-Valle 86

Akhmedov et al PRD53 (1996) 2752 Malinsky et al PRL95(2005)161801 Bazzocchi et al, PRD81 (2010) 051701

fermion exchange

TYPE I

Scalar-exchange

TYPE II

ORIGIN OF NEUTRINO MASS AND SEESAW

Number & properties of messengers

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R a d i a t i v e n e u t r i n

  • m

a s s i n 3 3 1 s c h e m e

Boucenna, Morisi & JWFV arXiv:1405.2332 Singer, Valle, Schechter, Phys.Rev. D22 (1980) 738

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Boucenna, Morisi & JWFV arXiv:1405.2332

R a d i a t i v e n e u t r i n

  • m

a s s i n 3 3 1 s c h e m e

# generations = # colours

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

Add 3 gauge singlets ...

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Boucenna, Morisi & JWFV arXiv:1405.2332

R a d i a t i v e n e u t r i n

  • m

a s s i n 3 3 1 s c h e m e

# generations = # colours

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

Add 3 gauge singlets ...

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Boucenna, Morisi & JWFV arXiv:1405.2332

R a d i a t i v e n e u t r i n

  • m

a s s i n 3 3 1 s c h e m e

# generations = # colours

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

Add 3 gauge singlets ...

arXiv:1404.3751

more on the low-scale approach to neutrino masses ...

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Order in the chaos?

FLAVOR

GUT

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Order in the chaos?

FLAVOR

GUT

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

Order in the chaos?

FLAVOR

GUT

King et al

  • Phys. Lett. B 724 (2013) 68-72
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CHARGED LEPTONS Sectors are separated Sectors are separated by an extra Abelian Zn by an extra Abelian Zn

THE FLAVOR PROBLEM

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CHARGED LEPTONS Sectors are separated Sectors are separated by an extra Abelian Zn by an extra Abelian Zn

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

A4

THE FLAVOR PROBLEM

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CHARGED LEPTONS Sectors are separated Sectors are separated by an extra Abelian Zn by an extra Abelian Zn

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

A4

THE FLAVOR PROBLEM

Altarelli, Feruglio 2005

Tri-BiMaximal ansatz

Harrison, Perkins, Scott 2000

(CP assummed)

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arXiv:1305.6774

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arXiv:1305.6774

STRIKING CORRELATION

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OSCILLATION PARAMETER CORRELATIONS

Boucenna et al PhysRevD.86.073008

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OSCILLATION PARAMETER CORRELATIONS

Boucenna et al PhysRevD.86.073008

Dorame et al Nucl Phys B861, 259–270

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FLASY 2011, 2012, 2013, 2014, ...

Gfmavor

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Gfmavor

Deviation

  • f TBM

Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

FLASY 2011, 2012, 2013, 2014, ...

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change ansatz:

Albright,Dueck,Rodejohann 1004.2798 Boucenna,M,Tortola, JV PRD86 (2012) 051301

Gfmavor

Deviation

  • f TBM

Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

FLASY 2011, 2012, 2013, 2014, ...

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change ansatz:

Albright,Dueck,Rodejohann 1004.2798 Boucenna,M,Tortola, JV PRD86 (2012) 051301

Gfmavor

Deviation

  • f TBM

Abelian

Ding, Morisi, JV PRD87 (2013) 1211.6506 Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

FLASY 2011, 2012, 2013, 2014, ...

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change ansatz:

Albright,Dueck,Rodejohann 1004.2798 Boucenna,M,Tortola, JV PRD86 (2012) 051301

Gfmavor

Deviation

  • f TBM

Anarchy

Donoghue et al PRD73 Hall,Murayama,Weiner,PRL Altarelli, Feruglio,Masina,JHEP

Abelian

Ding, Morisi, JV PRD87 (2013) 1211.6506 Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

FLASY 2011, 2012, 2013, 2014, ...

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change ansatz:

Albright,Dueck,Rodejohann 1004.2798 Boucenna,M,Tortola, JV PRD86 (2012) 051301

Gfmavor

Deviation

  • f TBM

Anarchy

Donoghue et al PRD73 Hall,Murayama,Weiner,PRL Altarelli, Feruglio,Masina,JHEP

Abelian

Ding, Morisi, JV PRD87 (2013) 1211.6506 Ishimori.etal ProgTheor Phys Suppl 183 (2010) 1 Holthausen et al 1212.2411

FLASY 2011, 2012, 2013, 2014, ...

Flavor roadmap

Fortsch.Phys. 61 (2013) 466-492

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Bi-large mixing & Cabibbo angle

Abelian Flavor Models

Boucenna et al, Phys. Rev. D 86, 051301(R)

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Bi-large mixing & Cabibbo angle

Abelian Flavor Models

reactor seeds solar & atm

Boucenna et al, Phys. Rev. D 86, 051301(R)

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Bi-large mixing & Cabibbo angle

Abelian Flavor Models

reactor seeds solar & atm

Boucenna et al, Phys. Rev. D 86, 051301(R)

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Bi-large mixing & Cabibbo angle

Abelian Flavor Models

reactor seeds solar & atm

Models Ding, et al Phys.Rev. D87 (2013) 053013

Roy, Singh, ..arXiv:1211.7207

Boucenna et al, Phys. Rev. D 86, 051301(R)

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4 4

Neutrinoless Double Beta Decay

Schechter, JWFV 82 Lindner et al JHEP 1106 (2011) 091 A.S. Barabash arXiv:1104.2714

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4 5

Neutrinoless Double Beta Decay

Dorame et al

NPB861 (2012) 259-270 PhysRevD.86.056001 Schechter, JWFV 82 Lindner et al JHEP 1106 (2011) 091

Family symmetry dependent lower bound

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

A.S. Barabash arXiv:1104.2714

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4 6

Neutrinoless Double Beta Decay

Dorame et al

NPB861 (2012) 259-270 PhysRevD.86.056001 Schechter, JWFV 82 Lindner et al JHEP 1106 (2011) 091

Family symmetry dependent lower bound

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

A.S. Barabash arXiv:1104.2714

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BIG- BANG

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

BIG- BANG

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

BIG- BANG

are key in the synthesis of light elements

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

BIG- BANG

are key in the synthesis of light elements can probe the Universe much earlier than photons …

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

BIG- BANG

are key in the synthesis of light elements can probe the Universe much earlier than photons …

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Seesaw inflation & majoron dark matter + ...

Boucenna et al arXiv:1405.2332

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Seesaw inflation & majoron dark matter + ...

Boucenna et al arXiv:1405.2332

inflaton

type-I seesaw

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Seesaw inflation & majoron dark matter + ...

Boucenna et al arXiv:1405.2332

tree-level

Coleman-Weinberg radiative corrections

inflaton

type-I seesaw

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Seesaw inflation & majoron dark matter + ...

Boucenna et al arXiv:1405.2332

tree-level

Coleman-Weinberg radiative corrections

inflaton

type-I seesaw

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seesaw leptogenesis

Aristizabal et al arXiv:1405.4706

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seesaw leptogenesis

Aristizabal et al arXiv:1405.4706

RH neutrino scatterings

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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) 121301

Lattanzi & Valle, PRL99 (2007) 121301

Esteves et al, PRD 82, 073008 (2010) Bazzocchi & al JCAP 0808 (2008) 013 Bazzocchi & al JCAP 0808 (2008) 013 Consistency with CMB

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DARK MATTER MAJORONS Berezinsky, Valle PLB318 (1993) 360

Lattanzi & Valle, PRL99 (2007) 121301

Lattanzi & Valle, PRL99 (2007) 121301

Esteves et al, PRD 82, 073008 (2010) Bazzocchi & al JCAP 0808 (2008) 013 Bazzocchi & 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) 121301

Lattanzi & Valle, PRL99 (2007) 121301

Esteves et al, PRD 82, 073008 (2010) Bazzocchi & al JCAP 0808 (2008) 013 Bazzocchi & al JCAP 0808 (2008) 013

61

Lattanzi et al PRD88 (2013) 063528

Consistency with CMB Add also Dark Energy? George Smoot arXiv:1405.2776

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WI MP D A R K MA T T E R

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SNEUTRINO-like instead of neutralino ..

Arina et al PRL101 (2008) 161802 Bazzocchi, Cerdeno, Munoz, J.V., PRD81 (2010) 051701

If neutrinos get mass a la Inverse seesaw susy

Spectrum can change so …

WI MP D A R K MA T T E R

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SNEUTRINO-like instead of neutralino ..

Arina et al PRL101 (2008) 161802 Bazzocchi, Cerdeno, Munoz, J.V., PRD81 (2010) 051701

If neutrinos get mass a la Inverse seesaw susy

Spectrum can change so …

WI MP D A R K MA T T E R

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Dark Matter (quasi) STABILITY

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Dark Matter (quasi) STABILITY

from FLAVOUR SYMMETRY

ACCIDENT? Lavoura, Morisi, JV JHEP 1302(2013) 118

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Dark Matter (quasi) STABILITY

Z2 PARITY

from FLAVOUR SYMMETRY

ACCIDENT? Lavoura, Morisi, JV JHEP 1302(2013) 118

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Dark Matter (quasi) STABILITY

Z2 PARITY HIGGS PORTAL DIRECT DETECTION

from FLAVOUR SYMMETRY

ACCIDENT? Lavoura, Morisi, JV JHEP 1302(2013) 118

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OSCILLATIONS ROBUST ... PHASE, SPECTRUM, OCTANT, NSI ?

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OSCILLATIONS ROBUST ... PHASE, SPECTRUM, OCTANT, NSI ? ORIGIN OF NEUTRINO MASS : WHICH MESSENGER ?

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OSCILLATIONS ROBUST ... PHASE, SPECTRUM, OCTANT, NSI ? ORIGIN OF NEUTRINO MASS : WHICH MESSENGER ?

FLAVOR PATTERN ?

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OSCILLATIONS ROBUST ... PHASE, SPECTRUM, OCTANT, NSI ? ORIGIN OF NEUTRINO MASS : WHICH MESSENGER ? NEUTRINOS : TESTABLE @ LHC ?

FLAVOR PATTERN ?

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OSCILLATIONS ROBUST ... PHASE, SPECTRUM, OCTANT, NSI ? ORIGIN OF NEUTRINO MASS : WHICH MESSENGER ?

FLAVOR PATTERN ?

IS DARK MATTER RELATED TO NEUTRINOS ? NEUTRINOS : TESTABLE @ LHC ?

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OSCILLATIONS ROBUST ... PHASE, SPECTRUM, OCTANT, NSI ? ORIGIN OF NEUTRINO MASS : WHICH MESSENGER ?

FLAVOR PATTERN ?

IS DARK MATTER RELATED TO NEUTRINOS ?

WHY STABLE ?

NEUTRINOS : TESTABLE @ LHC ?

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OSCILLATIONS ROBUST ... PHASE, SPECTRUM, OCTANT, NSI ? ORIGIN OF NEUTRINO MASS : WHICH MESSENGER ?

FLAVOR PATTERN: ANARCHY OR SYMMETRY ?

IS DARK MATTER RELATED TO NEUTRINOS ?

WHY STABLE ?

Non-SUSY WIMP ? Non-WIMP: MAJORON or GRAVITINO DECAYING DM … NEUTRINO PROPERTIES : TESTABLE @ LHC ?

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sneutrino

Masiero & Valle, PLB251 (1990) 273 Bhattacharyya & Pal, PRD82 (2010) 055013 Diaz et al PRD68 (2003) 013009, PRD62 (2000) 113008 Bazzocchi et al JHEP 01 (2013) 033 arXiv:1202.1529

sneutrino

SUSY ATM SCALE SUSY-SEESAW SOLAR SCALE RADIATIVE SUSY ORIGIN OF NEUTRINO MASS EFF . BILINEAR RPV EFF . BILINEAR RPV

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Lightest neutralino decay length

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

LIGHTEST NEUTRALINO DECAYS: PROBING NUs @ LHC

Lightest neutralino decay correlates with atm angle

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Gamma line from decaying Gravitino dark matter Gamma line from decaying Gravitino dark matter

decays suppressed by Planck mass & smallness of m-nu chosen to fjt neutrino osc. data

excluded by gamma line searches @ Egret & Fermi-LAT

relic abundance + LHC searches Restrepo et al

PRD85 (2012) 023523

LHC LHC

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Schechter & JV PRD22 (1980) 2227 & PDG

LEPTON MIXING MATRIX LEPTON MIXING MATRIX

Approximation used adopted in oscillation analyses

majorana phases majorana phases (cf KM)

  • scillations versus L-violating processes

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

K Rectangular K_eff. non-unitary P Non-trivial NSI & LFV NSI & LFV

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Forero, Tortola, JWFV arXiv:1405.7540

Oscillations 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]