highlights from the tevatronresearch.kek.jp/group/riron/workshop/kekph0712/dec... · 3 tevatron...
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Highlights from the Tevatron
Kazuhiko HARAUniversity of Tsukuba
KEKPH0712December 13, 2007, KEK
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Tevatron
DØCDF
Chicago
Booster
⎯p sourceMain Injector
Tevatron ProtonTevatron Proton--Antiproton Antiproton ColliderColliderC.M.E.=1.96 TeV
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TevatronTevatron LuminosLuminosityity
2001
2002 2003 20
04 2005
2006
2007
• ~3.3 fb-1 delivered (initial Run II target 2 fb-1 achieved) • CDF/D0 are recording ~85% of the delivered luminosity• Run until April 2010 (for 6-9 fb-1)
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The DetectorsThe Detectors
( )2/tanln θ−=η
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winter07
Tevatron Goals for Run II Tevatron Goals for Run II (CDF TDR)(CDF TDR)• Higgs Physics*• Properties of the Top Quark
– Top mass– σtt – Br(t→b) and any anomalies – Single top quark production*
• Precision Electroweak Program– W boson mass and width– Gauge boson couplings (Wγ, Zγ, WW, WZ, ZZ)– AFB of Z
• Search for New Phenomena– SUSY, Z´/ W´, Topcolor, Leptoquark, Compositeness, …
• Precision QCD at Large Q2
• Constraining the CKM Matrix– CP violation in the B system– Bs oscillation frequency ∆ms– Rare B decays ( B spectroscopy )
*added in beyond 2 fb-1 program
summer07winter08
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Higgs Boson Search at TevatronHiggs Physics
low-mass (mH<135) Higgs Boson;decay: dominantly into bb ← b taggingproduction: WH, ZH ← leptonic W/Z decays provide best signature
high-mass (mH>135) Higgs Boson;decay: WW, ZZ ← leptonic decay enhances S/Nproduction: gg fusion
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CDF Search for low-mass (mH<135) Higgs Boson
Low signal rates in enormous backgroundsplots are for double SECVTX b-tagged events (least BG)
NN trained for120 GeV Higgs
SECVTX b-tagging
Higgs Physics
summer07
U. TsukubaMasubuchi
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D0 Search for low-mass (mH<135) Higgs BosonHiggs Physics
summer07
S/N<0.1 for both experimentsneed to combine various search channelsneed to control systematics (JES, V+jets rate)
winter08
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CDF Search for high-mass (mH>135) Higgs Boson
LR= PH
PH+PBGLikelihood ratio:
expect S/N~1.6/6 @ MH=160 GeVCharged leptons from Higgs decay tend to have small opening angle
Higgs Physics
summer07
( ) ( )22 φ∆+η∆=∆R
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D0 Search for high-mass (mH>135) Higgs BosonHiggs Physics
winter08
2.8 expected2.4 observed
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SM Higgs SM Higgs SensitivitiesSensitivities
VH→Vbb
H→WW
Higgs Physics
summer07
winter08
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Combined Combined SM Higgs SearchSM Higgs SearchSummer 2007
Combining 28 NN/LR/mass distributionsWithout D0 update for Winter2008
Higgs Physics
summer07
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Prospect for Prospect for SM Higgs SearchSM Higgs SearchHiggs Physics
For MH=160 GeV
Improvements:
•NN/ME discriminants•extended lepton acceptance•NN b-tagger•include (yet) unused triggers
Demonstrated 1.5-2.5 increase in sensitivity
With improvements
7 fb-1: •exclude all masses <188 GeV at 2σ•3σ sensitivity in [150-170] GeV
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14So far the data are consistent with SM
~30 results using 1 – 1.5 fb-1 available: Summer2007(updating for Winter2008 using ~2.5 fb-1 )
Top Quark PhysicsTop Quark PhysicsProperties of the Top Quark
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Top Quark Top Quark MassMassProperties of the Top Quark
★1.5 GeV
summer07
wint
er08
Projection
1.1TOTAL0.1Monte Carlo statistics0.1QCD modeling0.2Background composition0.2Background Shape0.3Generators0.2Parton Distribution Functions0.2FSR0.4ISR0.4Background JES0.6Residual JES0.6b-jet energy scaleSystematics GeV/c2
In CDF Lepton+Jets
winter07
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Γt < 12.7GeV @ 95% CLMt = 175 GeV
Γt < 12.7GeV @ 95% CLMt = 175 GeV
Top Quark WidthTop Quark WidthProperties of the Top Quark
summer07
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Top Cross Section and RTop Cross Section and RProperties of the Top Quark
σ tt = 8.10−0.82+0.87(sta+ sys) ± 0.49(lumi)
8.2 ± 0.5 (stat) ± 0.8 (syst) ± 0.5 (lum) pb
summer07
R = BR(t → Wb)BR(t → Wq)
= Vtb2
assuming 3 generations
L+2 b-jets
L+b-jet
summer07
σ theory (p p → tt ) ≈ 6.7 pb
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MMtttt and Zand Z´́
For Technicolor leptophobic Z´(Harris, Hill, Parke hep-ph/9911288)
CDF : MZ´ > 720 GeV (95%CL)D0: MZ´ > 680 GeV (95% CL)
Properties of the Top Quark
summer07
Limits on narrow tt resonance production
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In SM BR(t→Zq) = O(10–14)cf. BR(b →sγ)= O(10–4)
BSMs predict up to O(10–2)LEP limit BR(t→Zq)<13.7%
Top FCNCTop FCNC
BR(t → Zq) < 10.6%@95%C.L.
Properties of the Top Quark
CDF sees no excess in 1 fb-1
summer07
• Z+4j events• divide to tagged and anti-tagged selections• calculate mass χ2 for bkg (Z+jets, tt) suppression
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Boosted decision tree
Single Top ProductionSingle Top Production
σs+t= 3.0 ± 1.2 pbσs= 1.1, σt =1.9 pbσs+t= 3.0 ± 1.2 pbσs= 1.1, σt =1.9 pb
3.1 σEvidence
Adding three analyses
3.6σ!
σs+t= 4.7 ±1.3 pbσs= 1.0, σt =4.0 pbσs+t= 4.7 ±1.3 pbσs= 1.0, σt =4.0 pb
Properties of the Top Quark
|Vtb|= 1.02 ± 0.18 (expt)± 0.07 (theory)|Vtb|= 1.02 ± 0.18 (expt)± 0.07 (theory)
|Vtb| = 1.3 ± 0.2|Vtb| = 1.3 ± 0.2summer07
s-channel t-channel
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W MassW MassPrecision Electroweak Program
W m
ass
prec
isio
n
luminosity1 fb-1100 pb-110 pb-1
Projection: 15-20 MeV
No update since 2006 summerNo D0 Run II result, yet
CDF PRL paper accepted
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W WidthW WidthPrecision Electroweak Program
(2007 winter)
CDF PRL paper submitted
PDG 2007 and update for 2008
*extracted:( )[ ]
( )[ ]llZBlW
R W
Z
W
→Γν→Γ
⎥⎦
⎤⎢⎣
⎡σσ
=
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W and Top Mass in MSSMW and Top Mass in MSSMPrecision Electroweak Program
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DiDi--boson Cross Sections: boson Cross Sections: ExploringExploring to Higgs and New Physicsto Higgs and New Physics
Precision Electroweak Program
>6σ observation
3σ significance
summer07
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2522,2,
21 Tvisvis
vis pppm /++= ττ
ττττ channels (MSSM Higgs?)channels (MSSM Higgs?)
excess is gone!
Search for New Phenomena
summer07
winter07
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BBss Mixing and Mixing and ∆∆mmss2006
PRL 97, 242003 2006
DØ Run II Preliminary
3.1 σ significance
CDF:DØ:
CDF:Theoretical uncertainty ~ 10 x Experimental uncertainty
2.4 fb-1
Constraining the CKM Matrix
winter08
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• In SM Bs→µµ is suppressed (FCNC)– SM predicts
• SUSY can enhance BR (@large tanβ)
9105.3)( −−+ ×≈µµ→sBBR
BR(Bs µµ) < 5.8×10-8 BR(Bs µµ) < 9.3×10-8
BBss →µµ→µµ
No excess seen in 2 fb-1
Rare B decays
summer07
@95%C.L
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BBcc Lifetime and MassLifetime and Mass
Mass(Bc) = 6274.1 ± 3.2 ± 2.6 MeV/c2
V. Kiselev
bc
cc
πud
J/ψBc
Theory:
B spectroscopy
summer07
winter08
W
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Ξb DiscoveriesDiscoveriesB spectroscopysummer07
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SUMMARYSUMMARY• Approaching to the SM Higgs detection
3σ evidence for Higgs of 110 GeV, 150-175 GeVor, exclude Higgs <190 GeV
with further analysis improvements and luminosity reach of 7 fb-1
• Top properties are being explored. No hints of beyond the SM physics, yet.
• Achieved initial Run II precision goals on Mt, Mw, ∆ms Improving further.
The Tevatron continues to provide exciting data.Will run till 2010.