Boson Boson Scattering at LHC with PHASE

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E. Maina - VV at LHC with Phase - Les Houches 2005 1 Boson Boson Scattering at LHC with PHASE

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Boson Boson Scattering at LHC with PHASE. What can we observe at LHC?. Higgs!. Higgs discovery. Unitarity. Unitarization: eg:Butterworth,Cox,Forshaw PRD65(02)96014 different ways of constructing amplitudes which are unitary from low order amp. At the LHC. Incoming V’s are always - PowerPoint PPT Presentation

Transcript of Boson Boson Scattering at LHC with PHASE

Page 1: Boson Boson Scattering at LHC with PHASE

E. Maina - VV at LHC with Phase - Les Houches 2005

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Boson Boson Scattering at LHC with PHASE

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What can we observe at LHC?

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Higgs!

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Higgs discovery

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Unitarity

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Unitarization: eg:Butterworth,Cox,Forshaw PRD65(02)96014different ways of constructing amplitudes which are unitary from low order amp

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At the LHC

Incoming V’s are always off-shell

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Large interferences Kleiss-Stirling, PLB182(86)75

The HE off-shell behaviour is worse than on-shell€

VL (q12 = m2 + 4 sΔ1)VL (q2

2 = m2 + 4 sΔ2) ⏐ → ⏐ X

When the V’s are off-shelll emission from f-lines must be included(a;b)= linear combination of a and b

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PHASE hep-ph/0504009

PHact Adaptive Six-fermion Event-GeneratorE. Accomando, A. Ballestrero, E. Maina- Univ. Torino

q1q2 ⏐ → ⏐ q3q4q5q6l1l2

Dedicated event generator All One-shot Efficient: good coverage of phase-space Interfaced with showering/hadronization

Problems Large number of processes Large number of diagrams/process Large number of channels/enhanced regions

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PHACT PLB350(95)225

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Processes in PHASE1.0

All particles outgoingAdding ud<-->cs and e<-->mu ---> 1K processes

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An interesting example:

It includes:

• ZZ --> W+W- Higgs --> WW• ZW- --> ZW-• W-Z --> ZW-• W-W- --> W-W- • W- --> W-W+W- with 2 Higgs --> WW channels• W- --> ZZW- Higgs --> ZZ

Homework: check it out

1046 diagrams

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Future Improvements

2q --> 4qlnu @ O(as2aw

4) First result later

2q --> 4ql+l- in integration test ZW&ZZ final states semilept 2q --> 2q4l all ingredients ready ZW&ZZ final states lept 2g --> 4qlnu @ O(as

2aw4) & @ O(as

4aw2)

Main TOP channel! Amp O(as2aw

4) ready

Good control of tails is essential 2g --> 2q4l

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First look

pT(q,l+/-)> 10 GeV E(q,l+/-)>20GeV M(q,q)>20GeV Abs(eta(q))<6.5 Abs(eta(l+/-))<3 Abs(eta(jc))<3 eta(jf)>2 eta(jb)<-2

Reject 160<M(blnu)<190GeV 160<M(bqq)<190GeVRequire 70<M(qq)<90GeV

With C. Mariotti and S. Bolognesi, E. Accomando, S. Ballestrero(Torino)

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PHASE vs PYTHIA

PYTHIA has only LL in EVBA approximation

mH=500GeV No Higgs

Top rejectionW mass

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VV scattering

Expect: central high pT JJ and lnu from W’s high energy, high pT forward and backward spectator J

Background:

Cannot be separated from all other EW contributions

tt VV+jets V+jets

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S/B from EW processes in PHASE at parton level

Main bkg: tt(EW!), single t, VVV

pT(q,l+/-)> 10 GeVE(q,l+/-)>20GeVM(q,q)>20GeVAbs(eta(q))<6.5Abs(eta(l))<3

Reject160<M(blnu)<190GeV160<M(bqq)<190GeVRequire70<M(qq)<90GeV70<M(lnu)<90GeV M(jf-jb)MW,MZ

If more than one qq pair is close to MW,Z

best match is chosen. Flavour info used.

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Spectator vs decay partons

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V(qcqc) spectrum

No flavour info Flavour info

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S/B kinematics

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Neural Net Selection of Signal

mH=500GeV NoHiggs

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Internal gluon QCD correctionswith G. Bevilacqua (Torino)

Includes qq-->tt No external g

First results: no real analysis 70<M(jcjc)<90GeV

All PHASE1.0 processes

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Conclusions

A new 6f Event Generator is available for VV scattering, Higgs in VBF, top(soon), VVV physics First results in VV scattering and Higgs productionExtracting Signal is hard

WORK is in PROGRESS

New processes More realistic simulations: FAMOS, CMKIN