D Ø Results from Run 2

23
D D Ø Results from Run 2 Ø Results from Run 2 Yuri Gershtein for the DØ collaboration

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D Ø Results from Run 2. Yuri Gershtein for the D Ø collaboration. A Truly International Collaboration. Totals: 18 countries Europe, Asia, and North, Central and South Americas 73 institutions & labs 33 US 40 non-US 646 physicists 334 US 312 non-US. - PowerPoint PPT Presentation

Transcript of D Ø Results from Run 2

Page 1: D Ø Results from Run 2

DDØ Results from Run 2Ø Results from Run 2

Yuri Gershtein

for the DØ collaboration

Page 2: D Ø Results from Run 2

Yuri Gershtein

D0 Results from Run 2: Wine & Cheese, July 26, 2002 2

A Truly International Collaboration

Totals: 18 countries

Europe, Asia, and North, Central and South Americas

73 institutions & labs

33 US 40 non-US

646 physicists 334 US 312 non-US

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Yuri Gershtein

D0 Results from Run 2: Wine & Cheese, July 26, 2002 3

Run 2 and our Physics Program

Started March 2001 Ecm=1.96 TeV Peak L = 2.1·1031

Delivered ~ 50 pb-1

Detector commissioning almost completeFirst physics results from ~10 pb-1 at new Ecm

Physics ProgramTop, W, HiggsNew PhenomenaB-physicsQCD

Tevatron

Chicago

p

p CDF DØ

You Are You Are HereHere

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Yuri Gershtein

D0 Results from Run 2: Wine & Cheese, July 26, 2002 4

DØ Detector

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Yuri Gershtein

D0 Results from Run 2: Wine & Cheese, July 26, 2002 5

DØ Detectormuon system

shielding

electronics

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Yuri Gershtein

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DØ Detector

Central Calorimeter

Solenoid

Fiber Tracker

Silicon

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Yuri Gershtein

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Detector Performance: Tracking

KS +-

p-side pulse-height (ADC)

n-si

de p

ulse

-hei

ght

(AD

C) p-side pulse-height (ADC)

Silicon cluster charge

1 mip ~25 ADC #Noise < 2 ADC #

track pseudorapidity

fiber light yield

Scintillating Fiber Tracker (CFT)first time in a collider detector

• performs as expected • > 98% (including dead channels)• good light yield• reconstruct tracks

Silicon (SMT)• good S/N• 95% detectors are working• Clusters are being understood• >97% (incl. dead)

zero is suppressed

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Yuri Gershtein

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Detector Performance: Tracking

Impact Parameter

KS +-

track

x

y

Secondary Vertices

mass +-

Almost on target with• no CFT alignment• 1st pass SMT alignment

DØ Run 2 Preliminary

width =36 beam ~30

DØ resolution: ~20

Page 9: D Ø Results from Run 2

Yuri Gershtein

D0 Results from Run 2: Wine & Cheese, July 26, 2002 9

J/e+e-

Muon System

Calorimeter

J/ and ’

We

E(cluster)/p(track)

Combine tracking with other systems

Detector Performance

Z+-

~170 evts

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Yuri Gershtein

D0 Results from Run 2: Wine & Cheese, July 26, 2002 10

Jet Physics

Only statistical errorsLuminosity L = 5.8 pb-1 (±10%)Preliminary jet energy scale

30-50% syst. error in cross section

Not fully corrected(for unsmearing, efficiencies)

Testing pQCD at new energy2x cross section for ET>400 GeV

Structure functions at large xCompositeness, W’, Z’, etc…

Inclusive jet pT spectrum

Dijet mass spectrum

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Yuri Gershtein

D0 Results from Run 2: Wine & Cheese, July 26, 2002 11

B Physics DataPYTHIA

New tracking in 2 Tesla fieldMuon triggers up to ||< 2

b-quark Production Cross Section New ECM

Luminosity ~5 pb-1

Jet || < 0.6muon tag only, b-content from pT

rel fits

J/ Cross Section Measurement Luminosity ~5 pb-1

First measurement in this rapidity region and ECM

J/ pseudorapidity

pT( J/ ) > 5 GeV pT( J/ ) > 8 GeVc

ross s

ecti

on

, au

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B Physics

Proper B decay length (B J/+X)Data

Background from sidebandsBackgrounds from prompt J/B-lifetime signalSignal + background

mass (+-K±)

B lifetime measurement from inclusive J/

• Measured lifetime consistent with the world average

• Track errors (esp. from large SMT clusters) are being understood

Exclusive B reconstruction

• B±J/ K±

• First time in DØ• Expect more soon!

~5 pb-1

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Electroweak Physics High priority measurements

We cross-section

dots: Datadots: Datahistogram: histogram: MCMC

ET ETe

MT pTw

diEM Invariant mass (GeV)

Ze+e- cross-section

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Yuri Gershtein

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W and Z Production Cross Section

Data Sample:Luminosity ~ 7.5 pb-1

No. of We: 3493±75±296No. of Z ee: 186±14±10

First measurements of the cross sections at 1.96 TeV!

pb 212020266

)(

lumisyststat

Z eeZB

nbeWB lumisyststatW 27.033.006.067.2)(

NNLO Van Neerven et al

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W and Z Production Cross section

Since we can measure both: Ratio of cross sectionsMost of the systematic effects cancel out

W boson width can be calculated from the above formula

Using (W)/(Z) from theory and BR(Zee) from LEP

In good agreement with world average

W = 2.135±0.069 GeV

WZ

ZWsyststat

Z

W

eeZ

eW

eeZB

eWBR

)(

)(6.08.00.10

)(

)(

GeV 04.013.018.026.2 theorysyststatW

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W/Z boson + jets eventsJet multiplicity distributions

W+ 2jetsTransverse massspectrum

•Top Physics: W+3jets, Z+2jets•Higgs Physics: W/Z + 2jets

•Need excellent b-jet identification

•Secondary vertex recons.•Soft leptons in jets

Z+-

We

Multi jet BGMulti jet BG

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WW productionSearch for ee+ET events

A lot of interest in this channel (tri-linear couplings, New Phenomena)

Exotic Higgs Models:4th SM family enhance Higgs cross sections by a factor of ~8.5 for Higgs mass between 100-200 GeV

Fermiophobic/Topcolor Higgs: BR(HWW) >98% for mH 100 GeV

Backgrounds due to misidentified objects. Azimuthal opening angle between the leptons

Require good e+e- Require good

e+e- , missing ET,

no jets

luminosity 8.8 pb-1

/

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Search for New Phenomena

An ee candidate

Tri-lepton signaturesOne of cleanest signatures of SUSY for example from chargino+neutralino production

Analyses in progress:Likesign dielectronsJets+Missing Et

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GMSB SUSYPhenomenology:

Light Gravitino (<<eV) is LSP, NLSP can be neutralino or slepton

If neutralino NLSP:

inclusive search for ET + XBackgrounds:

QCD: , +j (w/ jet misidentified )

W e (track is lost)WW, WZ, DY,

Sensitivity is still too low to exclude SUSY points“Model Independent” Limit

Missing Transverse Energy

DØ Run 2 Preliminary

QCD+DY

CLpb %[email protected]

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Leptoquarksparticles with properties of both quarks and leptonsSignature: eejj events

MLQ > 113 GeV/c2

at 95% CL, for =1

2

Cro

ss S

ecti

on

[p

b]

Consistent with Run1 result

8.8 pb-1

Data : 6 events

Background : 6.9 2.9 events

LQ (m = 100 GeV) : 13.8 1.8 eventsLQ (m = 140 GeV) : 2.9 0.3 events

BG from QCD and DY

LQ Mass, GeV ET of electrons and jets, GeV

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Extra DimensionsSearch for large extra spatial dimensions via virtual graviton effects e+e-, and +- events

Run2 Preliminary Limit:

MS(GRW) > 0.92 TeV (ee,)

DØ Run 1 limits: MS(GRW) > 1.2 TeV

Prospects for Run 2: 1.5-2.5 TeV (2fb-1)2.1 – 3.5 TeV (20 fb-1)

SM

SM+ED

DATA

instrumental background (from data)

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Future ProspectsContinue to Search for New Physics

SUSY, strong dynamics, extra dimensions, etc…

Measurements of cross sections at 1.96 TeVW and Z boson production, jet cross sectionsb-quark production, top quark production

Measure W/Z Properties (AFB, W mass to 30 MeV)

Rich program of B-physics Comprehensive study of Top quark Properties (2fb-1)

Cross section(7%), Mass (2 GeV) spin correlations, charge, top-gauge boson couplings

Precision measurements of Top quark and W Boson mass constrain the Higgs BosonDirect Searches for the Higgs Boson

Run 2A: MH > 115 GeV

Run 2B: MH > 180 GeV or see signal

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ConclusionFirst physics results at 1.96 TeV

W and Z production cross sectionsfirst generation LQ limit, limit on Large Extra Dimensions, many more analyses in the works

Enormous progress made over the last year detector performance optimizationdeveloping analysis tools

Improvements in store:optimization of event reconstruction and selection procedures triggers and DAQ performancescalibration and alignment of the detectors

Looking forward to large integrated luminosity!