September 2011
Francesco Sannino
Technicolor after the Higgs Discovery
CP3-DESY-Goettingen School 11-14 October 2011 SCGT12 @ Nagoya 2012
Thursday, December 6, 12
Technicolor after the Higgs Discovery Francesco Sannino SCGT12 @ - - PowerPoint PPT Presentation
Technicolor after the Higgs Discovery Francesco Sannino SCGT12 @ Nagoya 2012 September 2011 CP3-DESY-Goettingen School 11-14 October 2011 Thursday, December 6, 12 Now Atoms 4% Dark Energy Dark Matter 74% 22% ? ? Thursday, December 6,
Thursday, December 6, 12
Atoms 4% Dark Matter 22% Dark Energy 74%
Thursday, December 6, 12
Thursday, December 6, 12
Thursday, December 6, 12
Thursday, December 6, 12
SM Higgs Expectation
Thursday, December 6, 12
In <4d: Sung-Sik Lee 06 4d: Antipin, Mojaza, Pica, Sannino 10
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Thursday, December 6, 12
Thursday, December 6, 12
Thursday, December 6, 12
0.0 0.2 0.4
0.0 0.1 0.2 0.3 0.4 0.5 S T
SU(3) + 1 Fund. Doublet
Weinberg, Susskind
1 TeV
TC alone = massless SM fermions Extend TC to generate fermion masses [Eichten & Lane] MH = FT C Fπ Mσ ' 1.5 TeV
Thursday, December 6, 12
Thursday, December 6, 12
UV IR
IR Conformal behavior
Holdom, Appelquist, Miranski, Yamawaki, Wijewardhana...
Thursday, December 6, 12
Gauge Group: SU, SO, SP, Exceptional Matter Representation # of Flavors per Representation
Thursday, December 6, 12
α
Energy
Interesting structure at large Nf
First coefficients at large Nf are known
Pica & Sannino 10
αUV = 3π TF Nf
Ciuchini, Derkachov, Gracey, Manashov ‘99
Thursday, December 6, 12
Thursday, December 6, 12
2 3 4 5 6 7 8 2 4 6 8 10 12 14 16 18 N nf
Ryttov & Sannino 07 Dietrich & Sannino 07 Sannino & Tuominen 04
Ryttov & Shrock 10
Poppitz & Unsal 9, 10 Pica & Sannino 10
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2 3 4 5 6 7 8 2 4 6 8 10 12 14 16 18 N nf
Thursday, December 6, 12
5 6 7 8 2 4 6 8 10 12 N nf
SO(N)
2 3 4 5 6 7 8 2 4 6 8 10 12 14 16 18 20 22 n nf
SOH2n+2L
All Orders g*=1 Four Loops g*=1 Ladder 2 3 4 5 6 7 8 2 4 6 8 10 12 14 16 18 n nf
SOH2n+1L
All Orders g*=1 Four Loops g*=1 Ladder
G2 F4 E6 E7 E8 ê Ad 2 4 6 8 10 12 nf
All Orders g*=1 Four Loops g*=1 Ladder
Sannino 09 Pica & Sannino 10 Mojaza, Pica, Ryttov Sannino 12 Mojaza, Pica, Ryttov Sannino 12 Mojaza, Pica, Ryttov Sannino 12
Thursday, December 6, 12
Thursday, December 6, 12
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4 ln m aHmL
d=-1ê8 d=-0.01 d=-0.002 d=-0.001 d=0.0005
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
0.0 0.1 a bMY
d=0.1 d=0 d=-0.1 d=-0.2
Miransky & Yamawaki 89 Miransky & Yamawaki 97 Yamawaki, Bando, Matumoto 86 Appelquist, Karabali, Wijewardhana 86
f
Sannino 2012
Thursday, December 6, 12
α(Λ)
α(Λ)
Thursday, December 6, 12
0.0 0.2 0.4 0.6 0.8 1.0 1.2 ln m aHmL
d=0.1 d=0.05 d=0 d=-0.2 d=-0.1 d=-0.05
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
1 a bJump
d=0 d=-0.05 d=-0.2
0.0 0.2 0.4 0.6 0.8 1.0 1.2 1.4
1 2 a bJump
d=0 d=0.05 d=0.2
Sannino 2012
f
Thursday, December 6, 12
c
LJump LMY
ΛMY = µ0 nc
f − nf
exp " − π 2pnc
f − nf
#
ΛJump = Λc ⇥ 1 − (nc
f − nf) ln
f − nf
⇤
Thursday, December 6, 12
2 3 4 5 6 7 8 2 4 6 8 10 12 14 16 18 N nf
Thursday, December 6, 12
Antipin, Mojaza, Sannino 1107.2932 Grinstein, Uttayarat 1105.2370 Antipin, Di Chiara, Mojaza, Mølgaard, Sannino 1205.6157
Thursday, December 6, 12
Nf −Nc Nc
Nf
Nc
Nf
2Nc Nf
Antipin, Mojaza, Sannino 2011
Thursday, December 6, 12
Antipin, Di Chiara, Mojaza, Mølgaard, Sannino 2012
12% of the CW is Walking
4.42 4.4167 4.4133 x = 4.41 0.00 0.01 0.02 0.03 0.04 0.05 0.06
0.0 ag 105âbag
Thursday, December 6, 12
Thursday, December 6, 12
Sannino, Tuominen 04 Hong, Hsu, Sannino 04 Dietrich, Sannino, Tuominen 05
Extra Electron
N
Extra Neutrino
t-up
t-down
t-glue
Higgs
ζ
SU(3) SU(2) U(1)
Higgs
Can feature Light TC/Dilaton Higgs
Smallest S-parameter & FCNC
Dark matter candidates
Thursday, December 6, 12
Sannino & Schechter 95 PRD [‘t Hooft 1/N, crossing, chiral, pole mass] Harada, Sannino & Schechter 95 PRD [f0(980)], 96PRL Pelaez - Confinement X - lecture
Thursday, December 6, 12
L = LSM + ✓ 1 + 2rπ v H + sπ v2 H2 ◆ v2 4 Tr DµU †DµU + 1 2 ∂µH ∂µH − mt ⇣ 1 + rt v H ⌘ " qL U 1 2 + T 3 ! qR + h.c. # − mb ⇣ 1 + rb v H ⌘ " qL U 1 2 − T 3 ! qR + h.c. # + · · · − ∆S W a
µνBµν Tr T aUT 3U † + O
✓ 1 Mρ ◆
U = exp ⇣ iπaT a/v ⌘
DµU ≡ ∂µU − igW a
µT aU + ig0UBµT 3
Thursday, December 6, 12
t W Z
LH ⊃ 2 m2
W rπ
v H W +
µ W −µ + m2 Z rπ
v H Zµ Zµ − mt rt v H ¯ t t + m2
W sπ
v2 H2 W +
µ W −µ + m2 Z sπ
2 v2 H2 Zµ Zµ
M 2
H = (M TC H )2 + 3(4πκFΠ)2
16π2v2 −4r2
t m2 t + 2sπ
✓ m2
W + m2 Z
2 ◆ + ∆M 2
H(4πκFΠ)
Foadi, Frandsen, Sannino, 12
Thursday, December 6, 12
H )2 ' M 2 H + 12 κ2r2 t m2 t
0.0 0.5 1.0 1.5 2.0 200 400 600 800 1000 1200 k rt MH
TCHGeVL
Thursday, December 6, 12
d(2 − indexT C) = NT C NT C ± 1 2
H
Sannino 08 Sannino & Schechter 07 Foadi, Frandsen, Sannino 12
Thursday, December 6, 12
Thursday, December 6, 12
Thursday, December 6, 12
Γ(H → γγ) ∼ @rt − 7rW + 3 4 X
QTC
d(RTC)e2
TC
1 A
2
W rW
µ W −µ − mt rt
t
Sensitive TC-fermion content H to γγ can help discriminate different models and to the H-tt coupling rt (Extended TC)
Thursday, December 6, 12
Potential discovery of composite dynamics at the LHC
Belyaev, Foadi, Frandsen, Jarvinen & Sannino 08
Composite spin-1 mesons like QCD ρ & a1
) (GeV)
+
l b M(b 400 500 600 700 800 900 1000 1100 /dM (fb/10 GeV) σ d
10
10
10
10 1
=5, S=0.3 g ~ =700 GeV,
A
M =125 GeV
h
sm, m =702 GeV
R1
M =1055 GeV
R2
M > 25GeV
2,b
> 45GeV, p
1,b
| < 4.5, p
b
|y > 20GeV
l
| < 2.5, p
l
|y ) < 135 GeV b )>0.7, 110 GeV < M(b, b R(b, Δ = 8TeV s pp @ )
+
l → Z, (Z b b → pp
Preliminary MWTC - theoretical updated analysis by T. Hapola
Thursday, December 6, 12
Thursday, December 6, 12