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A viable RS Model for Quarks and Leptons with
T´ Flavor SymmetryFelix Yu
University of California, IrvinePheno 2010
M-C. Chen, K. T. Mahanthappa, FY – Phys. Rev. D 81, 036004 (2010)[arXiv: 0907.3963 [hep-ph]]
Motivation• Fermion mass hierarchy unexplained• Gauge hierarchy problem motivates new
physics at about TeV• Randall-Sundrum (RS1) model with bulk
fermions provides a good framework– Can get fermion mass hierarchy with O(1)
coefficients– Need to suppress FCNCs
Randall-Sundrum• RS1 Model – warped geometry
– 5th dimension compactified via S1/2
– Higgs field confined to TeV brane (y = R), other fields propagate in bulk
– From compactification and boundary conditions, can find Fourier modes for bulk fields
– SM masses and mixings arise from zero modes• Integrate out y to find overlap between SM fields and
Higgs
Gherghetta, Pomarol (2000), Huber, Shafi (2000), Grossman, Neubert (1999)
222 dydxdxeds )y(
yk)y(
Randall, Sundrum (1999)
Flavor Changing Neutral Currents in RS• Change from gauge interaction basis to mass basis
• Generically get FCNCs if bulk masses are not equal• Solutions: (1) alignment, (2) degeneracy
233
222
211
4
00
00
00
)c,c(f
)c,c(f
)c,c(f
GgDiedy MM|y|k
mm V
)c,c(f
)c,c(f
)c,c(f
VGg
233
222
211
00
00
00†
The Finite Group T´• Double covering of A4
– A4 is the discrete invariant rotations of a tetrahedron
• Has two generators: S=(1234) (4321), T=(1234) (2314)– S2=R, T3=1, (ST)3=1, R2=1
• R=1: 1, 1´, 1´´, 3 (vector) [use for leptons]• R=-1: 2, 2´, 2´´ (spinorial) [use for quarks]
Frampton, Kephart (1995)
Assignment of T´ Representations• Motivated by neutrino mixing data: assign L ~ 3 (LH
lepton doublets), N ~ 3 (RH neutrinos) under T to obtain the tri-bimaximal mixing pattern– Introduce e ~ 1, ~ 1, ~ 1 for charged lepton masses– Tree-level lepton FCNCs are eliminated via degeneracy
(left-handed lepton doublets share a common bulk mass term) and alignment (right-handed lepton singlets can freely rotate)
• Motivated by quark masses, use 2 1 assignment– Tree-level quark FCNCs involving first and second
generations are eliminated via degeneracy (up- and down-type first two generations share a common bulk mass term)
• Require additional flavon fields to break T symmetry on the IR brane
.c.h
NLyHk
Ry
yyNNk
yL
Dc,SS,
SSD
b,Dc,SSD
a,SS,T
lepSS,,Yuk
5
55
1
1
Leptons in T´
.c.hLyLyeLyHk
)Ry(L DDDe
lepl,Yuk
5551)NcNcceceLcL(kL
LLLLL
NeLlepBulk
,Yukawal,YukawaBulkKineticleptonic
.c.hyyNLHk
)Ry(L DcDb,Dc,
DcDa,Dc,
lepDc,,Yuk
551
Purely Dirac neutrino masses
Seesaw type 1 neutrino masses
Quarks in T´: 2 1 Framework
.c.h)]TQyTQy
UQy)(UQy(H)[Ry(L
TUT
UUUUYukawa
331212
331212
)BcBDcD
TcTUcUQcQQcQ(kL
BD
TUQQBulk
331212 312
Down-type Yukawa Lagrangian is exactly analogous
YukawaBulkKineticquark LLLL
Parameter Counting• Input parameters (Naïve counting)
– Charged lepton: 8 (= 4 bulk + 3 Yukawa + 1 flavon)– Neutrino: [seesaw] 6 [7] (= 2 bulk + 2 [3] Yukawa + 2
flavon) – Quark: 24 = (6 bulk + 8 Yukawa + 10 flavon)
• Actual number of independent input combinations– 16 = Lepton matrix (3) + Neutrino matrix (2) + Quark
matrices (6 + 5)
• Contrast with anarchic case– 36 [30] for leptons, 36 for quarks
• Fit parameters– Lepton and quark masses (3 + 6 = 9)– CKM matrix (+ CP violating phase) (3 + 1 = 4)– Neutrino mixing angles (3)
16 Inputs, 16 Outputs
Results –Leptons
571260664960829250400000 .c,.c,.c,.c eL
Set all leptonic Yukawas to 1. Renormalization effects negligible.
Gives me=511 keV, m=105.7 MeV, m=1.777 GeV10
For normal hierarchy
For inverted hierarchy
Normal, Dc: msol2 = 7.6370 10-5 eV2, matm
2 = 2.4031 10-3 eV2
Inverted, SS: msol2 = 7.6560 10-5 eV2, matm
2 = –2.4009 10-3 eV2
Experimental: msol2 = 7.65 10-5 eV2, matm
2 = 2.40 10-3 eV2
Fusaoka, Koide (1998), Schwetz, Tortola, Valle (2008)
0944.0,1768.0,27000.1,40000.0 ,0,0 DcDcNL cc
Normal, SS: msol2 = 7.6520 10-5 eV2, matm
2 = 2.4001 10-3 eV2
06191.0,07427.0,40000.0,40000.0 ,0,0 SSSSNL cc
115241.0,02321.0,40000.0,40000.0 ,0,0 SSSSNL cc
For normal hierarchy
Results – Quarks
508.0350.0150.0
503.0512.0503.0
3
12
BTQ
DUQ
ccc
ccc
Bulk mass parameters
Flavons and Yukawas
060.0
00.1
540.0540.0
1135.0
00230.0
181.0
448.0
00200.0
00104.000143.0
3
3
0
0
00
0
0
B
T
D
D
D
U
UU
y
y
i
i
Prediction (3 TeV) Fit bounds
mu 1.49 MeV 0.75-1.5 MeV
md 2.92 MeV 2-4 MeV
mc 0.541 GeV 0.56 ± 0.04 GeV
ms 36.6 MeV 47 ± 12 MeV
mt 134.8 GeV 136.2 ± 3.1 GeV
mb 2.41 GeV 2.4 ± 0.04 GeV
Csaki, Falkowski, Weiler (2008)Other Yukawas set to 1
Results – CKM and Jarlskog
Fusaoka, Koide (1998), Charles, et al. (CKMfitter Group) (2009)
000078.0000047.0
0011.00020.0
00057.000064.0
0011.00019.0
00053.000052.0
0022.00022.0
00044.000032.0
0022.00022.0
00052.000052.0
999146.00404.000859.0
0412.097349.02250.0
00351.02251.097433.0
|| ExpCKMV
999176.00395649.000910164.0
040450.0973485.0225147.0
003464.0225305.0974282.0
|| TheoryCKMV Corrections to quark mixings from running are small.
Perform fit at mZ
510023 .Jth5450
250 10932 .
.ex .J
Leading FCNC Estimate• Leading contribution is from dim-6
operators arising from fermion zero-modes mixing with KK modes
• Scaled to Z-coupling, leading contribution is
• Using MKK ~ 3 TeV, kR ~ 11, v = 246 GeV:– coefficient is 2.96510-6 for u-c transition– coefficient is 4.15610-6 for d-s transition
2
42
222
)0()0(2)1(2
00 4 KK
kRkji
M
ve
Rk
fff
Conclusions• RS1 + T´ provides a framework for
realistic fermion masses and mixings– Motivated by neutrino mixings and quark
masses, we choose T´ representations• This choice eliminates tree-level lepton FCNCs
and first-second generation quark FCNCs
– Can fit for all SM fermion masses, CKM matrix, and Jarlskog invariant with 16 input parameter combinations
– Allows a low first KK mass scale, testable at colliders
Group Algebra of T´
ie
eiA
/i
/i
12
12
12
2
3
1
2 S=A1, T=A2,
2´ S=A1, T=2A2,
2´´ S=A1, T=A2
1 S=1, T=1,1´ S=1, T=,1´´ S=1, T=2
10
02A
122
212
221
3
1
2
2
2
S
200
00
001
T
Feruglio, Hagedorn, Lin, Merlo (2007)
3
Neutrino Constraints• Neutrino measurements (at 2)
• (at 1)• Well-fit by Tri-Bimaximal Mixing
(TBM) Harrison, Perkins, Scott (1999)
14012023
2 50 ...sin
0440032012
2 3040 ...sin
0160011013
2 010 ...sin
213161
213161
03132
///
///
//
UTBM
TBM can be easily obtained from A4 or T´ group symmetries
Schwetz, Tortola, Valle (2008)
Ma, Rajasekeran (2001)
Leptons in T´ 3
3
2
1
~
L
L
L
L
1
1
1
~
~
~e3
0
0
1
0 ~
1113333 AS
)c,c(fy
)c,c(fy
)c,c(fy
hM
LD
LD
eLD
e
e
5
5
5
0
00
00
00
2332111 1221331 1331221
T´ contraction:
Diagonal charged lepton mass matrixbecause of T´ assignments and flavon VEVs
.c.hLyLyeLyHk
)Ry(L DDDe
lepl,Yuk
5551
Quarks in T´: The 2 1 Framework
)c,c(fy)c,c(f
)c,c(fcos)c,c(f)c,c(fi
)c,c(fsin)c,c(fi
)c,c(fi
hM
TQT
TQU
UQUU
UQUQ
UQUU
UQUQ
U
312
31212
31212
30
0000
0000
02
12
1
2 1
Quarks in T´: The 2 1 Framework
)c,c(fy)c,c(f
)c,c(fcos)c,c(f)c,c(fi
)c,c(fsin)c,c(fi
)c,c(fi
hM
BQB
BQD
DQDD
DQDQ
DQDD
DQDQ
D
312
31212
31212
30
0000
0000
02
12
1
2 1
CitationsC. Amsler et al. (Particle Data Group), Phys. Lett. B667, 1 (2008)S. Bar-Shalom and A. Rajaraman, Phys. Rev. D 77, 095011 (2008). arXiv:0711.3193 [hep-ph]S. Bar-Shalom, A. Rajaraman, D. Whiteson, FY, Phys. Rev. D 78, 033003 (2008). arXiv:0803.3795 [hep-
ph]CKMfitter Group (J. Charles et al.), Eur. Phys. J. C41, 1-131 (2005). arXiv:hep-ph/0406184M.C. Chen and S.F. King, arXiv:0903.0125 [hep-ph]M.C. Chen and K.T. Mahanthappa, arXiv:0904.1721 [hep-ph]V. Cirigliano, B. Grinstein, G. Isidori and M. B. Wise, Nucl. Phys. B 728, 121 (2005).
arXiv:hep-ph/0507001G. D’Ambrosio, G.F. Giudice, G. Isidori and A. Strumia, Nucl. Phys. B 645, 155 (2002).
arXiv:hep-ph/0207036G. Engelhard, J.L. Feng, I. Galon, D. Sanford and FY, arXiv:0904.1415 [hep-ph]J.L. Feng, C.G. Lester, Y. Nir and Y. Shadmi, Phys. Rev. D 77, 076002 (2008) arXiv:0712.0674 [hep-ph].F. Feruglio, C. Hagedorn, Y. Lin and L. Merlo, Nucl. Phys. B 775, 120 (2007) arXiv:hep-ph/0702194P.H. Frampton and T.W. Kephart, Int. J. Mod. Phys. A 10, 4689 (1995). arXiv:hep-ph/9409330T. Gherghetta and A. Pomarol, Nucl. Phys. B 586, 141 (2000). arXiv:hep-ph/0003129Y. Grossman and M. Neubert, Phys. Lett. B 474, 361 (2000). arXiv:hep-ph/9912408 P.F. Harrison, D.H. Perkins and W.G. Scott, Phys. Lett. B 458, 79 (1999). arXiv:hep-ph/9904297S.J. Huber and Q. Shafi, Phys. Lett. B 544, 295 (2002). arXiv:hep-ph/0205327C.I. Low and R.R. Volkas, Phys. Rev. D 68, 033007 (2003). arXiv:hep-ph/0305243E. Ma and G. Rajarasekaran, Phys. Rev. D 64, 113012 (2001). arXiv:hep-ph/0106291L. Randall and R. Sundrum, Phys. Rev. Lett. 83, 4690 (1999). arXiv:hep-th/9906064L. Randall and R. Sundrum, Phys. Rev. Lett 83, 3370 (1999). arXiv:hep-ph/9905221L. Randall and R. Sundrum, Nucl. Phys. B 557, 79 (1999). arXiv:hep-th/9810155T. Schwetz, M. Tortola and J.W.F. Valle, New J. Phys. 10, 113011 (2008). arXiv:0808.2016 [hep-ph]