18
Neutrinos and Flavour G.G.Ross, Coseners House, May 03 at is the origin of the Quark and lepton masses, mixing angle d CP violating phases? ? u GUT M M ? d l GUT M M (2) (2) ? L R SU SU (2) (2) ? L R SU SU Family? Family?

Neutrinos and Flavour

Embed Size (px)

DESCRIPTION

Neutrinos and Flavour. G.G.Ross, Coseners House, May 03. What is the origin of the Quark and lepton masses, mixing angles and CP violating phases?. Family?. Family?. Masses. 1. GeV. THEORY :. DATA :. ?. Mixing. Data. Theory ?. Hierarchy. Democracy. - PowerPoint PPT Presentation

Citation preview

Page 1: Neutrinos and Flavour

Neutrinos and Flavour

G.G.Ross, Coseners House, May 03

What is the origin of the Quark and lepton masses, mixing angles and CP violating phases?

?u GUTM M

?d lGUTM M

(2) (2) ?L RSU SU(2) (2) ?L RSU SU

Family?Family?

Page 2: Neutrinos and Flavour

DATA :

iu

Mixing

1 0.218 0.224 0.002 0.005

0.218 0.224 1 0.032 0.048

0.004 0.015 0.03 0.048 1CKMV

?

1GeV

i id il

1210 910 610 310 310

Masses

0d dij ijM Y H 0u u

ij ijM Y H

, ,u i c j d i c jYukawa ij ijL Y Q u H Y Q d H

THEORY :

0.72 0.89 0.45 0.69 0.2

0.24 0.58 0.39 0.76 0.52 0.84

0.24 0.58 0.39 0.76 0.53 0.84MNSV

Page 3: Neutrinos and Flavour

Data Theory ?

†u uL Diag RM V M V

†d dL Diag RM U M U

†CKM L LV V U

Underconstrained – need mixing angles but only VCKM measured.

2 22

2 2

1 2 1/ 2

1 1 21

a aa

a a

u dC

Hierarchy Democracy

Page 4: Neutrinos and Flavour

4 3 3

2 2?

? ? 1

d

b

M

m

dm usV

cbV

sm

ubV

23

33 33

12

2

32

2

2 22

13 1

3

1

3

3 33

23

12

13

s

b

d

s

d

b

mm m

mm m

mm

mm

mm

m

m

mmm m

V

V

V

11 12 13

22 2321

31 3 32 3

m m

m mm

m

m

M

mm

Hierarchy

Page 5: Neutrinos and Flavour

d

b

3 3

3 2 2

20

320 2

Mm

0 1.5 0.4

1.5 1.3 0.15

0.4 1.3 1

i

i

e

e

Symmetric fit

Asymmetric fit

d

b

3

3 2Mm

0 1.7 0

1.7 0 5

0 0.3 1

u

t

3

3Mm

0 2 0

0 2

0 0.6 1

u

t

3 3

3 2 2

3 2

Mm

0

0.05

1

?

?

? ?

RobertsRomaninoGGRVelasco Sevilla

Data Theory

Page 6: Neutrinos and Flavour

3 3

2 23

2 2

0

?

3 ?

?

?

1

lM

m

( ) 1bX

mM

m

( ) ( ) |X

l dMDet M Det M

1( )

3s

X

mM

m

Georgi Jarlskog

( ) 3dX

e

mM

m

Extension to charged leptons – GUT?

Page 7: Neutrinos and Flavour

Family symmetries

Hierarchical structure strongly suggests a broken symmetry

0 0 0

0 0 0

0 0 1

2

0 0 0

0 0

0 0 1

a

0

2(1),OM

a

MESSENGER SECTOR?

i X

j

H

Xij

H

Mm

FAMILY SYMMETRY? Froggatt, Nielsen

6Abelian, Non-Abelian (U(3))

Page 8: Neutrinos and Flavour

Abelian Family symmetry (1)U

3 4

3 2

4

0

1

R

R

R

d

s

b

L L Ld s bdR L

b

M

m

-3 2 1

-3 2 1

8( )O

X X

H H

M M

-1 -11 -1

Ibanez GGR

3(40.4 1.8)10 d

s

mcb mV O

uM lM ?M

Page 9: Neutrinos and Flavour

M Asymmetric charge assignment :

23

13

13

4 3 3

3 2 2

1 1

R

R

R

d

s

b

54 1

3 3 3

L L Ld s b

}

Large mixing… maximal?

3 3

3

3

0

(1) (1)

(1) (1)

2

1

1

eL

L

L

O O

O O

2 1 1

eL L L

effM

) 5(5

c

c

L

c

d

d

S dU

e

Ramond et al, Jack, Jones, …..

Page 10: Neutrinos and Flavour

Non-Abelian family symmetry

Near Bi (-Tri) maximal mixing suggests Non-Abelian symmetrycapable of relating e

Candidate group?

63: ( )Kinetic c cL L L LL U

Numerous suggestions for the symmetries of effM C3, S3, A4…

Harrison, Scott, PerkinsBabu, Ma, ValleWetterich…

But can such structures be consistent with all quark and lepton masses?

U(2), U(3)Various attempts :Barbieri et al,Chkareuli, Froggattt, NielsenKing, GGR….

Page 11: Neutrinos and Flavour

King, GGR

8 3 3

3 2 2

3 2 1

d

b

z zM

z w wm

z w

Coefficients equal due to SU(2)family symmetry d

s

mcb mV

(10) (3) familySO U

(4) (2) (2)L RSU SU SU

Maximal, large mixing, SUSY flavour problem

: d l uM M M MGUT q l

: ')(2) (d uR

lU M MS M M

form of from U(3) symmetryMSRHD M

?

?

23 23

1 ici j

j HM

23 (0, , )i x x

3

Page 12: Neutrinos and Flavour

Possible with “see-saw”

Extension to neutrinos???

???dDM M

( ) / 2b ea

( ) / 2a

i1R

j

1iDM

1D j

M

1M

TD DM MM M

3 3

3 2 3 2 3

3 2 3

0

1

M ( ) ( )

( )D a a

a

z z

z

Majorana Mass1

2 1 2 3

3

M

M

M M M M

M

M

Dirac Mass

100

10-1

10

10-2

10-3

10-4

eV

King, GGR

Page 13: Neutrinos and Flavour

SUMMARY

The measurement of neutrino properties is testing our ideas about the origin of flavour and raises interesting questions :

Is there a connection between quarks and leptons?

GUT?

Tests?

, [ ] [ ],d lb Xm m Det M Det M Seesaw M

Is there a family symmetry?

Abelian? Non-Abelian?

Origin of the hierarchy?

Froggatt Nielsen? Radiative corrections? New spatial dimensions?

Origin of CP violation?

Spontaneous?

Page 14: Neutrinos and Flavour

b

texture zeros

...GUT relations,

Precision tests . ..

...m m

Flavour changing neutral currents Mass matrix structure

, ,u c t, ,u c t

, ,..g W

, ,..g W

d

d

s

s

Probes RH angles

e , ,e

W W2 2

2 2

312 10c u

c u

m m

m m

2 2

2 2

312 10e

e

m m

m

l

m

22 , , , , ,R Ri i R Rq u q l em

232 2 1,2 1,2 1,2 31,2 3

22 22 2 2 2 2 2 2 2 21 13 23 ,, ,

R R R RL

i ii i q l u d u dMM M

m m m m m m m

soft mass speSUSY ctrum

SUSY CP : If CP is spontaneously broken in flavon sector the

SUSY CP violating phases are natural

prob

ly s

em

l

l

mal

TESTS?

Vives, GGR, Velasco Sevilla

Page 15: Neutrinos and Flavour

Neutrino texture zero ?

3 1,2 DRHD M M

*312 1 2

*1 2 1

2 213 12 det

. . Wm M mm M m W

W W

2

313 12 2sin sin emmm m

2/ 2 2 1n 1

2

210MM

Ibarra, GGR

2β decay,leptogenesis

† †. . . .D MNS lM mY D R D U U

Casas,Ibarra

0 cos sin

0 sin cos

1 0 0

z z

z z

}

†W

, ,D D D M1,1 1,1 0 ; 1, 2 2,1 (Y diagonal )l l l

DY Y Y Y

CHOOZ

Page 16: Neutrinos and Flavour

13

1 2ln( / )M M

/ 2

max

1 2ln( / )M M

(1,2) 0l (1,1) 0l

Page 17: Neutrinos and Flavour

(SUSY) Textures : FCNC, CP constraints

4 3 3

2

23

2

2

1

d

b

M

m

( , 0 0)dm S Q

0 0

( )

S Q

A

( )

CP

A

?Gauge mediat

SUGRA

ion

Vives, GGR

Page 18: Neutrinos and Flavour

2 2

2 2

i j

i j

m

ij

m

m m