TeVatron SUSY searches in final states leptons and photons

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Veme Rencontres du Vietnam, 2004 1 TeVatron SUSY searches TeVatron SUSY searches in in final states leptons and photons final states leptons and photons Vu Anh Tuan Laboratoire de l’Accélérateur Linéaire, Orsay, France for CDF and D collaborations mSUGRA chargino and neutralino trilepton GMSB inclusive search in diphoton plus missing ET

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TeVatron SUSY searches in final states leptons and photons. mSUGRA chargino and neutralino trilepton GMSB inclusive search in diphoton plus missing ET. Vu Anh Tuan Laboratoire de l’Accélérateur Linéaire, Orsay, France for CDF and D  collaborations. SUSY@TeVatron (1/2). mSUGRA - PowerPoint PPT Presentation

Transcript of TeVatron SUSY searches in final states leptons and photons

Page 1: TeVatron SUSY searches in final states leptons and photons

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TeVatron SUSY searchesTeVatron SUSY searchesinin

final states leptons and photonsfinal states leptons and photons

Vu Anh TuanLaboratoire de l’Accélérateur Linéaire, Orsay, France

forCDF and D collaborations

mSUGRA chargino and neutralino trilepton GMSB inclusive search in diphoton plus

missing ET

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SUSY@TeVatron (1/2)SUSY@TeVatron (1/2)

• R-parity conservation missing energy

mSUGRAo SUSY breaking mediated

by gravityo LSP is most likely

neutralino 01

o Mass: 1 0

2 201

GMSBo Mediated by gauge fieldso LSP is gravitinoo Phenomenology is entirely

determined by NLSP (slepton or neutralino)

• Analysis in this talk interpreted within mSUGRA or GMSB frameworks

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SUSY@TeVatron (2/2)SUSY@TeVatron (2/2)

• Squarks and gluinos– large cross-section– decay most of the time into jets plus MET– huge QCD multijets background

• Processes w/ lepton(s) and/or photon(s) in final state (e.g., chargino/neutralino production)– smaller cross-section (BR)– much lower QCD background Subject of this talk

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DD trilepton searches trilepton searches

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Chargino-neutralino searchesChargino-neutralino searches

• Very clean decay mode: trilepton plus MET

• Searches at DØ– Di-electron plus (any) lepton (e, ou )– Electron-muon plus (any) lepton– Like-sign dimuon ( )

• Optimized for mSUGRA parameters (near LEP II limit)– tan = 3, > 0, A0 = 0

– m0 = [72, 88] GeV, m1/2 = [165, 185] GeV

mass 1 0

2 [97, 114] GeV

mass slepton 1 enhance leptonic

decay BR 0.2-0.4 pb

• Integrated luminosity 150-175 pb-1

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eel (1/2)eel (1/2)

Signal

• DY reduction (ee) < 2.8– MET > 20 GeV

• Top pair veto: jet veto• W+ (ee)

– Require hits in the tracker innermost layers

• Third lepton: an isolated track present , pT > 3 GeV– Include e, and

(even -hadronic decays)

• Backgrounds: Z/DY, W+, diboson, Z/DY , top pair• 2 electrons: isolated, ET > 12(8) GeV, || < 1.1(3.0)• Z veto: keep M(ee) in [15, 60] GeV

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eel (2/2)eel (2/2)

• To optimize signal selection– Use the product of MET

and track pT Final cut

METpT(track) > 250 GeV2

• Observed: 1 event• Expect:

– 0.27 background event– 0.8-1.6 events from SUSY

• Remaining DY background has low MET and track pT

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eel l

Before track pT > 3 GeV cut

• Background:– Z/DY : dominant– WW, WZ, ZZ, top pair– W+j/, QCD

• e: isolated, ET > 12 GeV, pT > 8 GeV

• MET > 15 GeV Similar Z, W+ and top pair

vetoes as in eel analysis• Same isolated track (pT > 3

GeV) requirement• Observed: 0 event• Expect:

– 0.54 background events– 0.63-0.93 events from SUSY

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Like-sign dimuonLike-sign dimuon

• Backgrounds– b/c pairs (dominant)– W+jets, top pair– Charge sign-flip: Z/DY

isolated, pT > 5 GeV• bb/cc estimated from data

– Calibrated from QCD-dominated region (one µ nearly “isolated”, (µµ) > 2.7)

• Charge sign-flip: from MC and cross-checked w/ data

• Cuts– µ pT > 11(5) GeV, both

isolated, (µµ) < 2.7– Z veto, MET > 15 GeV– LS mass (µµ) < 80 GeV

• Observed: 1 events• Expect:

• 0.13 background events• 0.2-0.4 events from SUSY

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Combined trileptonCombined trilepton

• Gain better sensitivity• See 3 events from data,

expect 3.4 from SM background

• Set a 95% CL limit on trilepton cross-section– Significant improvement

over Run I– Approaching mSUGRA

sensitivity region• Result interpreted within

mSUGRA framework– Can be used to constrain

other models with similar mass hierarchy

Channel Data Background

e + e + l 1 0.27 0.42 0.02

e + 1 2.49 0.37 0.18

e + + l 0 0.54 0.24 0.04

+ 1 0.13 0.06 0.02

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CDF and DCDF and D inclusive diphoton search inclusive diphoton search

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Inclusive diphoton search (1/3)Inclusive diphoton search (1/3)

• In GMSB, neutralino could be NLSP– Assume short lifetime decays well inside detector

• SUSY particles decay down to neutralino into gravitino and photon

quark

Signature: two photons plus MET in final state

quark

SUSY production

neutralino

gravitino

gamma

neutralino

gravitino

gamma

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Diphoton search (2/3)Diphoton search (2/3)

• Background– QCD plus photon or jet fake photon (dominant)– Electron fake photon: Z/DY, W+ e+

• QCD: estimated from data– at least one EM cluster fails

standard ID cut– QCD dominated at low MET

(<20(15) GeV) normalized to predict contribution at high MET

• e: from data using identified e and

scaled by (e) fake rate

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Diphoton search (3/3)Diphoton search (3/3)

• Two photons ET > 13(20) GeV, || < 1.0(1.1)• MET > 45(40) GeV• CDF: 202 pb-1, D: 185 pb-1

• Parameters- N = 1, Mmessenger = 2

- µ > 0

- tan = 15 (CDF), 5 (D - Snowmass slope)

• Signal dominated by chargino-neutralino production

• Observed: 0 (CDF), 1 (D) events

• SM background: 0.6 (CDF), 2.5 (D) events

Lower limit on neutralino mass

CDF: 93 GeV D: 105 GeV (beyond LEP!)

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ConclusionConclusion

• CDF and DØ produce solid physics results based on up to 200 pb-1 of luminosity

• Limits exceed Run I– mSUGRA: Trilepton

analysis of chargino and neutralino

– GMSB: inclusive diphoton

• TeVatron luminosity increases steadily

• New results coming out soon!

1.00E+32