studies of the higgs boson at the...
TRANSCRIPT
Studies of the Higgs Boson at
the Tevatron
Koji Sato
On Behalf of CDF and D0 Collaborations
25th Rencontres de Blois
Chateau Royal de Blois, May 29, 2013
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Tevatron Run II
π π collisions at s = 1.96 TeV(1.8 TeV in Run I).
Run II: Summer 2001 - Autumn 2011.
Collisions at world highest energy until Nov 2009. Energy frontier for ο½25
years!! Two detectors (CDF and D0)
for wide range of physics studies.
β’ Delivered: 12 fb-1.
β Recorded by CDF: 10 fb-1.
β Recorded by D0: 10 fb-1.
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CDF and D0 Detectorsβ’ Both are multipurpose detectors:
β Top/EWK measurements, Searches for Higgs and New
Phenomena, and B physics.
β’ Precision tracking with Silicon in 1.5 (CDF)/1.9 T (D0) Solenoid field.
β’ EM/Had calorimeters for e/g/jet measurement.
β’ Outer muon chambers.
CDF D0
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Before TevatronRun II results (Spring 2004)
With TevatronRun II results (Winter2013)
Constraint on Higgs Mass
Mhiggs < 152 GeV/c2 οΌ95% CL) .β¦.was Mhiggs < 251 GeV/c2 (95% CL) in Spring 2004.
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β’ Mass of W Boson (World Average):
Before Tevatron Run IIοΌ
mW=80.426Β±0.034 GeV/c2
With Tevatron Run II resultsοΌ
mW=80.385Β±0.015 GeV/c2
β’ Mass of Top Quark (World Average):
Tevatron Run I resultοΌ
mtop = 178.0 4.3 GeV/c2
With Tevatron Run II resultsοΌ
mtop = 173.2 0.9 GeV/c2
Higgs Discovery by LHC, Summer 2012
ATLAS: 5.9 Ο from Background CMS: 5.0 Ο from Background
Discovery was driven by π» β πΎπΎ, ZZ and WW decay modes.
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What We Want to Remember!!
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TEVATRON Summer 2012: Excess at ππ― = πππ β πππ GeV/c2 mass region.3.1 Ο from Background in Combination of searches for π― β ππ analyses.Complementary to LHC results
Discovery was driven by π» β πΎπΎ, ZZ and WW decay modes.
Tevatron Winter 2013 Combination
β’ Although we know ππ» βΌ 125 GeV/π2 from LHC results,
we present our analyses over full mass range.
β’ Analysis updates in a few channels since last Summer.
β’ Studies of Higgs couplings to Fermions and Bosons.
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SM Higgs Production and Decay at
Tevatron
Channels with best sensitivity are:
β’ mH<135 GeV (low mass):
β ggβHβbb is difficult to see.
β Look for WH/ZH with leptonic vector boson decays.
β’ mH>135 GeV (high mass):
β Easiest to look for HβWWβlnln. 8
CDF and D0 analysesChannel CDF Luminosity
fb-1
D0 Lumiosityfb-1
ππ» β ππππ 9.45 9.7
Zπ» β ππππ 9.45 9.7
Zπ» β ππππ 9.45 9.5
π» β ππ 6.0 9.6
ππ» β ππππ / ππ» β ππππ 8.6
π» β πΎπΎ 10.0 9.6
ππ» β ππππ 9.45
π‘π‘π» β ππππππ 9.45
π» β ππ β πΒ±ππβπ 9.7 9.7
π» β ππ β πΒ±ππβπ 9.7 7.3
ππ» β πππ β πππ + π 9.7 9.7
ππ» β πππ β πΒ±πΒ± + π 9.7 9.7
ππ» β ππππππ 9.7
π» β ππ β ππππ 9.7
π» β ππ β ππππ 9.7 9
β’ NN B-tagging algorithm.
β Two operation points
(T/L).
β Subdivision of events to
4 b-tag categories
(TT/TL/Tx/LL)
β’ Trained 3 NN to further
subdivide analysis sample.
β Separate signal from π‘ π‘, π+jets, diboson.
β’ Final discrimintnt NN
trained to separate signal
from all backgrounds.
10Candidateevent
Final Discriminant = separate Signal from all Bkgd.
π π NN π+jets NN Diboson NN
π‘ π‘ likeπ+jets
likediboson
likesignal
like
CDF: ππ» β ππππ Analysis
β’ π+πβ or π+πβ + 2 or 3 jets.
β’ π /π trigger + MET trigger (for πβs which trigger failed to identify).
D0: π» β π+πβ β π+πβ + ππΈπChannelβ’ π+πβ, π+πβ or πΒ±πβ pair within πππ > 15 GeV.
β’ BDT to reject π/πΎβ β ππ in π+πβ, π+πβ events.
β’ ππ β π»,ππ», ππ», ππ΅πΉ are considered as signal.
β Events with different jet multiplicity have different s/b composition.
β Separately analyze 0, 1, β₯2 jet bins.
β’ Subdivision of sample into WW-enriched/depleted by WW-BDT.
β’ Train a final BDT discriminant against all background.
Distributions of the Final discriminant (only showing ππ channel):
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0 jetWW-enriched
β₯2 jet0 jetWW-depled
General Strategy for Improved Sensitivity
β’ Utilize Multivariate Algorithms (MVA) for better S/B
separation.
β Neural Net, Boosted Decision Tree, Matrix Element, etc.
β Training of multiple MVAs in many channels.
β’ Maximize trigger efficiency of each analysis.
β Analysis of events through different triggers.
β’ Improved b-jet energy scale measurement (low mass analyses)
β b-jet energy correction based on NN at CDF.
β’ Improved b-tagging (low mass analyses)
β Algorithms based on MVA.
β’ Divide analysis sample into high/low purity subsamples.
β Subdivision due to lepton and b-tag quality. 12
Analysis improvements we just reviewed are implemented for most of the channels.
CDF and D0: Combined Limit
CDF D0
CDF excludes (95% C.L.):
90 < mH < 102 GeV/c2
149 < mH < 172 GeV/c2
Expected exclusion (95% C.L.):
90 < mH < 94, 96 < mH < 106 GeV/c2
153 < mH < 175 GeV/c2
D0 excludes (95% C.L.):
90 < mH < 101 GeV/c2
157 < mH < 178 GeV/c2
Expected exclusion (95% C.L.):155< mH < 175 GeV/c2
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CDF+D0 Combined Limit
Tevatron excludes:
90<mH<109, 149<mH<182 GeV/c2
Expected exclusion:
90<mH<120, 140<mH< 184 GeV/c2
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Broad excess at 115-140 GeV/c2
History of Analysis Improvement
β’ Tevatron analyses have been constantly improved.
β Improvement is far better than expected due to
increase in data!!
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Expected sensitivity for CDF searches: (D0 sensitivities are similar)
ππ― = πππ πππ/ππ ππ― = πππ πππ/ππ
Distribution of the Candidate Events
Candidate events in all the
combined analyses:
Data - Background
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P-value of the Tevatron Combination
β’ 3.0 standard deviations at ππ» = 125 GeV/π2.
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Signal Cross Section Best Fit
β’π
SM= 1.44β0.56
+0.59 for ππ» = 125 GeV/π2.
β’ Consistent across different decay modes.
β’ Assuming the SM Higgs branching ratio:
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β’ Fit separately by decay mode for ππ» = 125 GeV/π2:
Studies of Higgs Couplings
β’ Coupling scale factor w.r.t. SM:
β Kf : Fermion coupling Hff
β KW, KZ, KV : Boson couplings HWW, HZZ, HVV
β’ π π½π― β π©π π― β ππ = π²π½π π²π
πΓ π β π©π πΊπ΄
β’ π ππ β π― β π©π π― β π½π½ = π²ππ π²π½
πΓ π β π©π πΊπ΄
β’ Follow prescription of LHC Higgs working group arxiv:1209.0040.
β’ Assume a SM-like Higgs particle of 125 GeV.
KZ
Kf
KfKW
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Test of Custodial Symmetry
β’ πΎπ floating.
β’ Compute posterior probability density for
πππ = tanβ1(πΎπ/πΎπ).
πππ = 0.68β0.41+0.21
π²πΎ/π²π = π. ππβπ.ππ+π.ππ
SM
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Constraint on HVV and Hff Couplings
β’ Assuming:
πΎπ = πΎπ β‘ πΎπ
β’ Result is consistent with SM.
β’ Preferred regions around
πΎπ, πΎπ = (1.05,β2.40),
(1.05, 2.30)
β’ Negative values preferred for πΎπ
due to π» β πΎπΎ excess.
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Summaryβ’ Extensive search for Higgs boson with full Tevatron dataset.
β Analyses evolved through Run II to state of art.
β Excluded: 90<mH<109, 149<mH<182 GeV/c2 (95% C.L.)
β’ Observed a broad excess in 115<mH<140 GeV/c2.
β’ Higgs Mass consistent with LHC.
β 3.0 standard deviations at ππ» = 125 GeV/π2.
β Excess is shared between CDF and D0.
β Excess mainly from π» β π π.
βπ
SM= 1.44β0.56
+0.59 for ππ» = 125 GeV/π2.
β’ Studies of Fermion and Boson couplings.
β Consistent with SM expectations.
β Complementary to LHC studies.
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Backup
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Tevatron Combination by Channel
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Sensitivity of Individual Channel
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Old plot, just for illustration purposes
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HCP
Summer2012
Summer 2012
Improved b-tagging
Light Flavor Eff.
HOBIT Eff. SecVtx Eff.(old tagger)
0.89% 42% 39%
8.9% 70% 47%
Light Flavor Eff. Lb Eff.
0.5% 50%
4.5% 70%
CDF and D0 combine information of secondary vertex and tracks within jet cone by MVA (NN and BDT).
Primary Vertex Secondary Vertex
Displaced Tracks
Jet
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B-jet energy correction by NN
(CDF llbb channel)
Before NN Correction: After NN Correction:
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Resolution on ππ― βΌ ππ%
Systematics (CDF llbb channel)
Source %
Luminosity 6
Trigger efficiency 1-5
Lepton energy scale 1.5
ISR/FSR 1-15
B-tag efficiency 5-20
Jet energy scale 5-15
Signal xsec/br 5
Bkgd. Normalization 6-40
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Bkgd. Process
%
Mis-ID π 50
π + π π/π π 40
π‘ π‘ 10
Diboson 6
β’ The effect of Jet Energy Scale on the distribution shape is also considered.
β’ Sysyrmstic uncertainty degrade sensitivity to ZH signal byapproximately 13%.
2013 Collected Event Distribution
Tevatron CDF D0
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2013 Best Fit ππ» β π΅π/ππ
Tevatron
CDFD0
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HWW, HZZ and Hff Couplings
π²π = π²π = π π²π = π²πΎ = π
π²πΎ = π²π = π
π²πΎ = βπ. ππβπ.ππ+π.ππ, or π. ππ < π²πΎ < π. ππ
π²π = Β±(π. ππβπ.ππ+π.ππ)
π²π = βπ. ππβπ.ππ+π.ππ
Negative values preferred for πΎπ and
πΎπ due to π» β πΎπΎ excess.
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HWW and HZZ Couplings
β’ πΎπ floating.
β’ Result is consistent with SM.
β’ Preferred region around:
πΎπ, πΎπ = (1.25,Β±0.90)
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π» β πΎπΎ Limits by Experiment
D0 π― β πΈπΈ
CDF π― β πΈπΈ
CDF H->Ξ³Ξ³
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Coupling Factor for π» β πΎπΎ
KW Kf
+
2
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