st. andrews, 08/2009 1. the sm and the higgs 2. the higgs ... · 4. measure couplings to fermions...
TRANSCRIPT
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Higgs and Electroweak Physics
Sven Heinemeyer, IFCA (Santander)
St. Andrews, 08/2009
1. The SM and the Higgs
2. The Higgs in Supersymmetry
3. Experimental facts and fiction (from a theorist’s view)
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/1
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Higgs and Electroweak Physics
Sven Heinemeyer, IFCA (Santander)
St. Andrews, 08/2009
1. The SM and the Higgs
2. The Higgs in Supersymmetry
3. Experimental facts and fiction (from a theorist’s view)
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/1
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Higgs and Electroweak Physics (III):
Experimental facts and fiction
Sven Heinemeyer, IFCA (Santander)
St. Andrews, 08/2009
1. Higgs boson searches at LEP
2. Higgs boson searches at the Tevatron
3. Higgs boson searches at the LHC
4. Higgs boson precision physics at the ILC
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/2
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Discovering the Higgs boson
What has to be done?
1. Find the new particle
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/3
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Discovering the Higgs boson
What has to be done?
1. Find the new particle
2. measure its mass (⇒ ok?)
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/3
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Discovering the Higgs boson
What has to be done?
1. Find the new particle
2. measure its mass (⇒ ok?)
3. measure coupling to gauge bosons
4. measure couplings to fermions
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/3
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Discovering the Higgs boson
What has to be done?
1. Find the new particle
2. measure its mass (⇒ ok?)
3. measure coupling to gauge bosons
4. measure couplings to fermions
5. measure self-couplings
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/3
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Discovering the Higgs boson
What has to be done?
1. Find the new particle
2. measure its mass (⇒ ok?)
3. measure coupling to gauge bosons
4. measure couplings to fermions
5. measure self-couplings
6. measure spin, . . .
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/3
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Discovering the Higgs boson
What has to be done?
1. Find the new particle T
2. measure its mass (⇒ ok?) T
3. measure coupling to gauge bosons
4. measure couplings to fermions
5. measure self-couplings
6. measure spin, . . .
T = Tevatron,
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Discovering the Higgs boson
What has to be done?
1. Find the new particle T L
2. measure its mass (⇒ ok?) T L
3. measure coupling to gauge bosons L
4. measure couplings to fermions L
5. measure self-couplings
6. measure spin, . . .
T = Tevatron, L = LHC,
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/3
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Discovering the Higgs boson
What has to be done?
1. Find the new particle T L I
2. measure its mass (⇒ ok?) T L I
3. measure coupling to gauge bosons L I
4. measure couplings to fermions L I
5. measure self-couplings I
6. measure spin, . . . I
T = Tevatron, L = LHC, I = ILC
We need the ILC to find the Higgs
and to establish the Higgs mechanism!
But the LHC can do a crucial part already!
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/3
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1. Higgs search at LEP:
Dominant SM production process:
e+e− → ZH:e−
e+
Z
HZ
σ(e+e− → ZH) =G2
µM4Z
96π s
[
v2e + a2
e
]
ββ2 + 12M2
Z/s
(1 − M2Z/s)2
with β2 = (1 − (MH + MZ)2/s) (1 − (MH − MZ)2/s) (1)
Dominant decay process: H → bb
b
b
H
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Search for the Standard Model Higgs at LEP: [LEP Higgs WG ’03]
Exclusion limit
at the 95% C.L.:
MH > 114.4 GeV
expected: 115.3 GeV
(LEP has seen exactly as
many Higgs-like events
as could be expected
for MH ≈ 116 GeV,
not more, not less)-30
-20
-10
0
10
20
30
40
50
106 108 110 112 114 116 118 120
mH(GeV/c2)
-2 ln
(Q)
ObservedExpected for backgroundExpected for signal plus background
LEP
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Search for the MSSM Higgs bosons:
Situation is more involved due to many SUSY parameters
→ investigate benchmark scenarios:
→ Vary only MA and tanβ
→ Keep all other SUSY parameters fixed
1. mmaxh scenario:
→ obtain conservative tanβ exclusion bounds (Xt = 2MSUSY)
2. no-mixing scenario
→ no mixing in the scalar top sector (Xt = 0)
3. small αeff scenario
→ hbb coupling ∼ sinαeff/ cos β can be zero: αeff → 0:
main decay mode vanishes, important search channel vanishes
4. gluophobic Higgs scenario
→ hgg coupling is small: main LHC production mode vanishes[M. Carena, S.H., C. Wagner, G. Weiglein ’02]
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Search for neutral SUSY Higgs bosons:
e+e− → Zh, ZH
e−
e+
Z
h, HZ
σhZ ≈ sin2(β − αeff)σSMhZ
σHZ ≈ cos2(β − αeff)σSMhZ
e+e− → Ah, AH
e−
e+
A
h, HZ
σhA ∝ cos2(β − αeff)σSMhZ
σHA ∝ sin2(β − αeff)σSMhZ
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Constraints from the Higgs search at LEP [LEP Higgs Working Group ’06]
Experimental search vs. upper mh-bound (FeynHiggs 2.0)
mmaxh -scenario (mt = 174.3 GeV, MSUSY = 1 TeV):
mh > 92.8 GeV
(expected: 94.9 GeV), 95% C.L.
MA > 93.4 GeV
(expected: 95.2 GeV)
1
10
0 20 40 60 80 100 120 140
1
10
mh (GeV/c2)
tanβ
Excludedby LEP
TheoreticallyInaccessible
mh-max(b)
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Parameter region where experimental lower bound on Mh is significantly
lower than SM bound, MH > 114.4 GeV, corresponds to sin2(β −αeff) ≪ 1
“Excluded” tanβ region:
1
10
165 170 175 180 185
1
10
mtop
tanβ
mh-max
Excludedby LEP
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Constraints from the Higgs search at LEP [LEP Higgs Working Group ’06]
Experimental search vs. upper mh-bound (FeynHiggs 2.0)
no-mixing scenario (mt = 174.3 GeV, MSUSY = 1 TeV):
mh > 93.6 GeV
(expected: 96.0 GeV), 95% C.L.
MA > 93.6 GeV
(expected: 96.4 GeV)
1
10
0 20 40 60 80 100 120 140
1
10
mh (GeV/c2)
tanβ
Excludedby LEP
TheoreticallyInaccessible
No Mixing(b)
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2. Higgs search at the Tevatron
Tevatron: pp accelerator: → T
Production processes as at LEP:
q
q′
W
H
W
q
q
Z
H
Z
Other important production channels:
t
t
tg
g
H
q
q
q′
q′
W
W
H
Dominant decays:
b, τ−
b, τ+
H
W
W
H
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Overview of SM production cross sections:
[F. Maltoni et al. ’05]
1
10
10 2
10 3
100 120 140 160 180 200
qq → Wh
qq → Zh
gg → h
bb → h
gg,qq → tth
qq → qqh
mh [GeV]
σ [fb]
SM Higgs production
TeV II
TeV4LHC Higgs working group
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Expectations for Higgs discovery at the Tevatron:
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Real performance compared with expectations: [T. Dorigo ’09]
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Current Status of SM Higgs searches at the Tevatron:
1
10
100 110 120 130 140 150 160 170 180 190 200
1
10
mH(GeV/c2)
95%
CL
Lim
it/S
MTevatron Run II Preliminary, L=0.9-4.2 fb-1
ExpectedObserved±1σ Expected±2σ Expected
LEP Exclusion TevatronExclusion
SMMarch 5, 2009
⇒ applies also to a SM-like light MSSM Higgs boson
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Possible problem in SUSY:
h → bb
can be strongly suppressed
→ “Small αeff scenario”
[M. Carena, S.H., C. Wagner,
G. Weiglein ’02]
⇒ Strong suppression of
h → bb possible,
up to MA <∼ 350 GeV
(not realized in
mSUGRA/CMSSM, GMSB,
AMSB, . . . )
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Tevatron MSSM Higgs searches: “Heavy” MSSM Higgs bosons
Search modes: b b → φ b b , φ = h, H, A
p p → φ → τ+ τ− , φ = h, H, A
Strong enhancement compared to the SM:
σ(bbA) × BR(A → bb) ≃ σ(bbA)SMtan2 β
(1 + ∆b)2× 9
(1 + ∆b)2 + 9
σ(gg, bb → A)× BR(A → τ+τ−) ≃ σ(gg, bb → A)SMtan2 β
(1 + ∆b)2 + 9
∆b =2αs
3πmg µ tanβ × I(mb1
, mb2, mg)
+αt
4πAt µ tanβ × I(mt1
, mt2, µ)
Either H ≈ A or h ≈ A ⇒ another factor of 2
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Example: pp → h/H/A → τ+τ− at D0 with 2 fb−1 [D0 ’08]
(GeV)AM100 120 140 160 180 200 220 240
βta
n
0
10
20
30
40
50
60
70
80
90
100
Observed limitExpected limitLEP 2
100 120 140 160 180 200 220 2400
10
20
30
40
50
60
70
80
90
100-1DØ prel., 1-2.2 fb
= +200 GeVµ, maxhm
(GeV)AM100 120 140 160 180 200 220 240β
tan
0
10
20
30
40
50
60
70
80
90
100
Observed limitExpected limitLEP 2
100 120 140 160 180 200 220 2400
10
20
30
40
50
60
70
80
90
100-1DØ prel., 1-2.2 fb
= +200 GeVµNo-mixing,
⇒ exclusion for light MA and large tanβ
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3. Higgs search at the LHC:
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The (un)official (optimistic?) LHC time line:
2009: repairs, cool-down etc.,
first collisions by the end of the year?
2010: 0.1 fb−1 – 0.2 fb−1 (at√
s ≤ 10 TeV) ⇒ first physics results?
2011: O (few) fb−1 ⇒ first physics results?
2012 – 2015: 10 fb−1 per year ⇒ physics results with “low” luminosity
2016 – ?: 100 fb−1 per year ⇒ physics results with “high” luminosity
2019 + X (X > 0): upgrade to SLHC?
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The (un)official (optimistic?) LHC time line:
2009: repairs, cool-down etc.,
first collisions by the end of the year?
2010: 0.1 fb−1 – 0.2 fb−1 (at√
s ≤ 10 TeV) ⇒ first physics results?
2011: O (few) fb−1 ⇒ first physics results?
2012 – 2015: 10 fb−1 per year ⇒ physics results with “low” luminosity
2016 – ?: 100 fb−1 per year ⇒ physics results with “high” luminosity
2019 + X (X > 0): upgrade to SLHC?
YOU live in an exciting time!!!
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Important SM production channel at the LHC:
Gluon-Fusion:
t
t
tg
g
H
WBF:
q
q
q′
q′
W
W
H
Important decay for Higgs mass measurement:
W
W
W γ
γ
H t
t
t γ
γ
H
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Overview of SM Higgs production at the LHC:
10 2
10 3
10 4
10 5
100 200 300 400 500
qq → Wh
qq → Zh
gg → h
bb → h
qb → qth
gg,qq → tth
qq → qqh
mh [GeV]
σ [fb]
SM Higgs production
LHC
TeV4LHC Higgs working group
gluon fusion: gg → H
weak boson fusion (WBF):
qq → q′q′H
top quark associated
production: gg, qq → ttH
weak boson associated
production: qq′ → WH, ZH
SM Higgs search at the LHC: ⇒ full parameter space accessible!?
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SM Higgs search at the LHC: ⇒ full parameter space accessible
[ATLAS ’05]
Sig
nal
Sig
nif
ican
ce
1
10
102
-1 L dt=10 fb∫
σ5
WW→VBF Hττ →VBF H
(inclusive + VBF)γγ→H 4l (with K-factors)→ ZZ→H 4l (no K-factors)→ ZZ→H
bb→ttH,Hν lν l→ WW→H
llbb→ ZZ→H llqq→ ZZ→VBF H
Combined
(GeV)HM100 200 300 400 500
⇒ most problematic case also at the LHC: MH = 115 . . .120 GeV
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Step 2: Measurement of the mass
Best channel for mass measurement in the SM: H → γγ[ATLAS ’99]
⇒ δMH ≈ 200 MeV
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Situation is a bit more complicated for SUSY Higgses (φ = h, H, A)
[Tev4LHC Higgs working group report ’06]
100 150 200 250 300 350 400 450 500MΦ [GeV]
10-1
100
101
102
103
104
105
106
Φ p
rodu
ctio
n cr
oss
sect
ion
[fb]
h
H
A
LHC, √s = 14 TeVmh
max, tanβ = 5
(bb)Φ
ggΦ
qqΦ
W/ZΦ
ttΦ
gluon fusion: gg → φ
weak boson fusion (WBF):
qq → q′q′φ
top quark associated
production: gg, qq → ttφ
weak boson associated
production: qq′ → Wφ, Zφ
NEW: bbφ
Search for the lightest MSSM Higgs at the LHC:
⇒ full parameter accessible But there might be problems . . .
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Possible problem in SUSY:
gg → h → γγ
can be strongly suppressed
→ “gluophobic Higgs scenario”
[M. Carena, S.H., C. Wagner,
G. Weiglein ’02]
⇒ Strong suppression of
gg → h → γγ possible
over the whole parameter space
(not realized in
mSUGRA/CMSSM, GMSB,
AMSB, . . . )0 200 400 600 800 1000
MA [GeV]
0
10
20
30
40
50
tanβ
0.0 - 0.2
0.2 - 0.4
0.4 - 0.6
0.6 - 0.8
0.8 - 1.0
> 1.0
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Mh measurement in the “nice” mmaxh scenario:
[CMS ’06]
Measurement possible only for
MA >∼ 250 GeV
⇒ δMh ≈ 200 MeV
other channels:
h → ZZ∗ → 4µ (Mh >∼ 130 GeV)
otherwise: δMh >∼ 1 − 2 GeV
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The heavy MSSM Higgs bosons
MSSM Higgs discovery contours in MA–tanβ plane
(mmaxh benchmark scenario): [ATLAS ’99] [CMS ’03]
ATLAS
LEP 2000
ATLAS
mA (GeV)
tan
β
1
2
3
4
56789
10
20
30
40
50
50 100 150 200 250 300 350 400 450 500
0h
0H A
0 +-H
0h
0H A
0 +-H
0h
0H A
00
h H+-
0h H
+-
0h only
0 0Hh
ATLAS - 300 fbmaximal mixing
-1
LEP excluded
areas where only h is observable ⇒ “LHC wedge”
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Latest results for neutral heavy Higgs bosons:
MSSM Higgs discovery contours in MA–tanβ plane (Φ = H, A)
(mmaxh benchmark scenario): [CMS PTDR ’06]
2,GeV/cAM100 200 300 400 500 600 700 800
βta
n
10
20
30
40
50
-1CMS, 30 fb
= h,H,Aφ, φ bb→pp scenariomax
hm2 = 1 TeV/cSUSYM2 = 200 GeV/c2M
2 = 200 GeV/cµ2 = 800 GeV/cgluinom
SUSY = 2 Mt
Stop mix: X
µ e
→ ττ → φ
+jet
µ → ττ
→ φe+jet→ ττ → φ
-1
jet+jet, 60 fb
→ ττ → φ
µµ → φ
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Charged Higgs boson searches:
MSSM Higgs discovery contours in MA–tanβ plane
(mmaxh benchmark scenario): [CMS PTDR ’06]
2,GeV/cAM100 200 300 400 500 600
βta
n
10
20
30
40
50
60
70
80-1CMS, 30 fb
νντ → ±, H± tbH→pp 2 = 175 GeV/ctm
scenariomaxhm
2 = 1 TeV/cSUSYM2 = 200 GeV/c2M
2 = 200 GeV/cµ2 = 800 GeV/cgluinom
SUSY = 2 Mt
Stop mix: X
jjb→ Wb →t
blν l→ Wb →t
light charged Higgs:
MH± < mt
heavy charged Higgs:
MH± > mt
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Differences compared to the SM Higgs:
Additional enhancement factors compared to the SM case:
b
b
Ayb → yb
tanβ
1 + ∆b
At large tanβ: either H ≈ A or h ≈ A
t
b
H+ ybtanβ
1 + ∆b
∆b =2αs
3πmg µ tanβ × I(mb1
, mb2, mg)
+αt
4πAt µ tanβ × I(mt1
, mt2, µ)
⇒ other parameters enter ⇒ strong µ dependence
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Most powerful search modes for heavy MSSM Higgs bosons:
bb → H/A → τ+τ− + X
gb → tH± + X, H± → τντ
pp → tt → H± + X, H± → τντ
Enhancement factors compared to the SM case:
H/A :tan2 β
(1 + ∆b)2× BR(H → τ+τ−) + BR(A → τ+τ−)
BR(H → τ+τ−)SM
H± :tan2 β
(1 + ∆b)2× BR(H± → τντ)
⇒ ∆b effects so far neglected by ATLAS/CMS
also relevant for BR(H/A → τ+τ−), BR(H± → τντ)
also relevant: correct evaluation of Γ(H/A/H± → SUSY)
⇒ additional effects on BR(H/A → τ+τ−), BR(H± → τντ)
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Suggestion for new benchmark scenarios:
[M. Carena, S.H., C. Wagner, G. Weiglein ’05]
→ investigate benchmark scenarios:
→ Vary only MA and tanβ (large!)
→ Keep all other SUSY parameters fixed
→ Vary in addition µ: µ = ±1000,±500,±200 GeV
(if perturbativity allows)
1. mmaxh scenario:
→ obtain conservative tanβ exclusion bounds (Xt = 2MSUSY)
At large ⇒ large O (αt) contribution to ∆b
2. no-mixing scenario
→ no mixing in the scalar top sector (Xt = 0)
At small ⇒ small O (αt) contribution to ∆b
⇒ large difference to mmaxh scenario
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Dependence of LHC wedge from bb → H/A → τ+τ− → 2 jets on µ:
[S.H., A. Nikitenko, G. Weiglein et al. ’06]
2,GeV/cAM100 200 300 400 500 600 700 800
βta
n
10
20
30
40
502 = -1000 GeV/cµ
2 = -200 GeV/cµ
2 = 200 GeV/cµ2 = 1000 GeV/cµ
-1CMS, 60 fb
j+j→ ττ → φ bb→pp scenariomax
hm2 = 1 TeV/cSUSYM2 = 200 GeV/c2M
SUSY = 0.8 Mgluinom
SUSY = 2 MtStop mix: X
2,GeV/cAM100 200 300 400 500 600 700 800
βta
n
10
20
30
40
502 = -1000 GeV/cµ
2 = -200 GeV/cµ
2 = 200 GeV/cµ2 = 1000 GeV/cµ
-1CMS, 60 fb
j+j→ ττ → φ bb→pp
no mixing scenario2 = 2 TeV/cSUSYM2 = 200 GeV/c2M
SUSY = 0.8 Mgluino
m = 0tStop mix: X
⇒ now based on full CMS simulation
⇒ non-negligible variation with the sign and absolute value of µ
(→ numerical compensations in production and decay)
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Precision of δM/M from bb → H/A → τ+τ− → 2 jets:
[S.H., A. Nikitenko, G. Weiglein et al. ’06]
⇒ now based on full CMS simulation
⇒ high precision measurement of heavy Higgs boson masses possible
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Charged Higgs: comparison with CMS PTDR (mmaxh scenario):
[M. Hashemi, S.H., R. Kinnunen, A. Nikitenko, G. Weiglein ’07]
2,GeV/cAM100 200 300 400 500 600
βta
n
10
20
30
40
50
60
70
80
2 = -1000 GeV/cµ2 = -200 GeV/cµ
2 = 200 GeV/cµ2 = 1000 GeV/cµ
scenariomaxhm
2 = 1 TeV/cSUSYM2 = 200 GeV/c2M
SUSY = 0.8 Mgluinom
SUSY = 2 MtX
→ note: MA–tanβ plane
light charged Higgs:
always worse than PTDR
better MH± calculation!
inclusion of ∆b effects
heavy charged Higgs:
PTDR in “the middle”
new results partially
substantially worse
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4. Higgs precision physics at the ILC
Higgs production at the ILC:
110
100100 200 300 400 500 600 700
�(e+e� ! Higgs) [fb]
ps = 350 500 800 GeV MHHZH���
Higgs-strahlung:
e+e− → Z∗ → ZH
e−
e+
Z
HZ
weak boson fusion (WBF):
e + e− → ννH
e+
e−
ν
ν
W+
W−
H
⇒ Measurement of masses, couplings, . . . in per cent/per mille
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Some ILC specifics:
recoil method: e+e− → ZH, Z → e+e−, µ+µ−
⇒ total measurement of Higgs production cross section
⇒ NO additional theoretical assumptions needed for absolute
determination of partial widths
⇒ all observable channels can be measured with high accuracy
Some ILC results (500 fb−1@√
s = 350 GeV):
δMH ≈ 50 MeV
δgZZH ≈ 2.5%, δgWWH ≈ 2 − 5%
δgHbb ≈ 1 − 2% (for MH <∼ 150 GeV)
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Higgs physics at the ILC:
SM Higgs @ ILC:
Precise measurement of:
1. Higgs boson mass,
δMH ≈ 50 MeV
2. Higgs boson width
(direct/indirect)
3. Higgs boson couplings,
O (few%) ⇒4. Higgs boson quantum
numbers: spin, . . .
[TESLA TDR ’01]
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Higgs physics at the ILC:
SM Higgs @ ILC:
Precise measurement of:
1. Higgs boson mass,
δMH ≈ 50 MeV
2. Higgs boson width
(direct/indirect)
3. Higgs boson couplings,
O (few%) ⇒4. Higgs boson quantum
numbers: spin, . . .
[TESLA TDR ’01]
But do we need the ILC precision?
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Higgs physics at the ILC:
SM Higgs @ ILC:
Precise measurement of:
1. Higgs boson mass,
δMH ≈ 50 MeV
2. Higgs boson width
(direct/indirect)
3. Higgs boson couplings,
O (few%) ⇒4. Higgs boson quantum
numbers: spin, . . .
[TESLA TDR ’01]
But do we need the ILC precision?
YES! To discriminate between the SM and extensions
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Example I: Higgs couplings in the MSSM:
“Normal” MSSM scenario:
⇒ measurable deviations over large parts of the parameter space
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Example II: Higgs couplings in model with extra dimensions:
Effects of Kaluza Klein towers:
-40%
-30%
-20%
-10%
0% (SM)
10%
20%
30%
c τ t W Z Hb40%
Devia
tion fr
om
SM
Valu
ehΓ
Extra DimensionsHiggs-radion mixing
?
⇒ measurable deviations over large parts of the parameter space
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Example III: Higgs couplings in a baryogenis motivated SM extension:
-40%
-30%
-20%
-10%
0% (SM)
10%
20%
30%
c τ t W Z Hb40%D
evia
tion fr
om
SM
Valu
ehΓ
Electroweak Baryogenesis
⇒ Only Higgs self coupling deviates, measurement possible!
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Step 5: measurement of the Higgs boson self-coupling
⇒ only possible at the ILCZ He�e+ HHZ Z HHZ Z HHZ1
Parton-level study:
[Djouadi, Kilian, Muhlleitner,
Zerwas ’99]
1 ab−1 ⇒ 20–30%
measurement of λ = λHHH
However:
λ = λHHHH out of reach
for all foreseeable colliders100 120 140 160 180
0
0.2
0.1
0.3
MH[GeV]
SM Double Higgs-strahlung: e+ e- → ZHH
σ [fb]
√s = 800 GeV
√s = 500 GeV
●
●
●
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⇒ only Lepton Colliders can “verify” the Higgs mechanism
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. . . including couplings to the second family!
⇒ coupling to the c quark:
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. . . including couplings to the second family!
⇒ coupling to the muon:
µ+µ− Mass (GeV)
Evt
s. /
1 ab
-1
0
5
10
15
20
25
115 120 125 130 135 140 145 150 155
(MH = 120 GeV,√
s = 800 GeV, Lint = 1 ab−1)
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Step 6: measurement of the Higgs boson spin
⇒ easy at the ILC
Threshold scan for
σ(e+e− → ZX):
X = H ⇒ σ ∼ β
(β from kinematics)
20 fb−1
⇒ identification easy
s (GeV)
cros
s se
ctio
n (f
b)
J=0
J=1
J=2
0
5
10
15
210 220 230 240 250
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Indirect determination of unknown Higgs sector parameters
LHC/ILC reach for MSSM Higgs bosons:
LHC:
h : all MA − tanβ plane
H, A : unreachable parts
CMS, 30 fb−1, mmaxh scenario: ⇒
ILC:
kinematic limit: MA <∼√
s/2
→√
s = 800 GeV
→√
s = 1000 GeV
γγ:
kinematic limit: MA <∼ 0.8√
sILC:
√s = 800 GeV√s = 1000 GeV
γγ:√
s = 800 GeVQ: Is it possible to extend the reach for heavy Higgs bosons ?
A: Yes, by direct and indirect measurements
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⇒ indirect determination of MA in LHC wedge
Existing LHC analyses neglect:
− MSSM intrinsic uncertainties
− parametric SM uncertainties
− anticipated parametric MSSM uncertainties
⇒ existing analyses unrealistic
One analysis includes all uncertainties: [K. Desch et al. ’04]
⇒ needs ILC uncertainty of
r ≡
[
BR(h → bb)/BR(h → WW ∗)]
MSSM[
BR(h → bb)/BR(h → WW ∗)]
SM
+ input for masses, mixing angles from LHC ⊕ ILC
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Analysis using r: [K. Desch et al. ’04]
∆r/r = 4%: upper limit on MA up to MA <∼ 800 GeV
∆r/r = 1.5%: ∆MA/MA = 20(30)% for MA = 600(800) GeV
inclusion of parametric errors crucial for reliable bounds
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Tricky scenario:
The LHC finds only a SM-like Higgs and nothing else
Q: Do we still need the ILC?
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Tricky scenario:
The LHC finds only a SM-like Higgs and nothing else
Q: Do we still need the ILC?
A: Of course!
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Tricky scenario:
The LHC finds only a SM-like Higgs and nothing else
Q: Do we still need the ILC?
A: Of course! Or better: even more!
The ILC provides:
− precise Higgs coupling measurements
− precision observable measurements with the GigaZ option
⇒ Only the ILC can find deviations from the SM predictions via the various
precision measurements
⇒ Only the ILC can point towards extensions of the SM
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Outlook
• The quest for electroweak symmetry breaking continues!
• Low-energy Supersymmetry continues to be our best bet for physics
beyond the Standard Model
• Data rules:
We need experimental information from Tevatron, LHC, ILC,
ν experiments, dark matter searches, low-energy experiments, . . .
to verify / falsify our ideas about electroweak symmetry breaking,
the Higgs, extensions of the SM, . . .
• The experiments in the next years will bring a decisive test of our ideas
about the Higgs and electroweak symmetry breaking
⇒ Very exciting prospects for the coming years
Expect the unexpected!
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/53
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Interested in Theory Predictions?
Interested in
• theory predictions for the Tevatron?
• theory predictions for the LHC?
• theory predictions for the ILC?
• phenomenology analyses in Higgs/SUSY?
⇒ You can do your PhD at IFCA (Santander, Spain)
contact: Sven.Heinemeyer @ cern.ch
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/54
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Santander, Spain: (15 minutes by foot from the institute :-)
contact: Sven.Heinemeyer @ cern.ch
Sven Heinemeyer – SUSSP65 – St. Andrews 2009 III/55