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2015:groups:tools:backgrounds [2015/06/03 17:53] jonathan.butterworth |
2015:groups:tools:backgrounds [2015/06/04 01:22] paolo.francavilla [WW versus ttbar] |
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* pT leptons all > 25 GeV | * pT leptons all > 25 GeV | ||
* |η| leptons all < 2.4 | * |η| leptons all < 2.4 | ||
- | * count the jets, and b-jets with p > 25 GeV, rapidity |y| < 4.5 | ||
* m(ll′) > 10 GeV | * m(ll′) > 10 GeV | ||
+ | * count the jets, and b-jets, with p > 25 GeV, rapidity |y| < 4.5 | ||
+ | ... but I haven't check the CMS paper yet. | ||
3. Consider WWbb as the signal, motivated by WWH (H->bb). Same study (DR/SR/C/Sum). | 3. Consider WWbb as the signal, motivated by WWH (H->bb). Same study (DR/SR/C/Sum). | ||
+ | For HH->WWbb, a possible proposal could be: | ||
+ | |||
+ | Objects Definition: | ||
+ | * electrons and muons: pT > 25 GeV; |eta| < 2.4 | ||
+ | * jets: pT > 25 GeV; | eta | <4.5 | ||
+ | * bjets: jets with | eta |< 2.5 and b-labelled | ||
+ | |||
+ | NOTE 1: in the ATLAS WW analysis, the jets are build from all the particles, excluding muons and neutrinos. | ||
+ | If we adopt this definition, we will need to run an Overlap Removal between electrons and jets, to avoid counting jets which are in fact electrons. | ||
+ | NOTE 2: The ATLAS WW analysis is vetoing events if (among the other selections) : | ||
+ | * there are jet (and b-jet), or | ||
+ | * there are extra leptons. | ||
+ | If we want to extend to events with b-jets, we should consider how to handle the semi-leptonic b-decays in jets ()to avoid to veto the event because of the leptons in jets. | ||
+ | |||
+ | Event Selection: | ||
+ | ->fill()CutFlow | ||
+ | * 2 opposite charged leptons | ||
+ | * 1 muon, 1 electron | ||
+ | ->fill()CutFlow | ||
+ | * MET_rel>25 GeV, | ||
+ | ->fill()CutFlow | ||
+ | * mll>10 GeV, | ||
+ | ->fill()CutFlow | ||
+ | * ptll>30 GeV, | ||
+ | ->fill()CutFlow | ||
+ | ->fill(electron) pt, eta | ||
+ | ->fill(muon) pt, eta | ||
+ | ->fill(b-jet1) pt, eta | ||
+ | ->fill(b-jet2) pt, eta | ||
+ | ->fill(b-jets) #b-jets | ||
+ | ->fill(other jets), pt, eta, #jets | ||
+ | * 100<mT(MET,e,mu)/GeV<150 | ||
+ | ->fill()CutFlow | ||
+ | ->fill(electron) pt, eta | ||
+ | ->fill(muon) pt, eta | ||
+ | ->fill(b-jet1) pt, eta | ||
+ | ->fill(b-jet2) pt, eta | ||
+ | ->fill(b-jets) #b-jets | ||
+ | ->fill(other jets), pt, eta, #jets | ||
+ | * 100<m(bb)/GeV<150 | ||
+ | ->fill()CutFlow | ||
+ | ->fill(electron) pt, eta | ||
+ | ->fill(muon) pt, eta | ||
+ | ->fill(b-jet1) pt, eta | ||
+ | ->fill(b-jet2) pt, eta | ||
+ | ->fill(b-jets) #b-jets | ||
+ | ->fill(other jets), pt, eta, #jets | ||
+ | |||
+ | |||
+ | NOTE: it would be nice to use some top veto. | ||
+ | the pseudo-top definition could be a nice idea, but it is defined | ||
+ | in a straightforward way for the Semi-leptonic channel. | ||
+ | One can test the b-lepton mass (associating the b to the closer lepton). | ||
+ | |||
Semi-leptonic channel: | Semi-leptonic channel: | ||
4. Consider ttbar as signal. Look at distortion in b-lepton mass from SR/C/Sum/WWbb-non-top contributions. | 4. Consider ttbar as signal. Look at distortion in b-lepton mass from SR/C/Sum/WWbb-non-top contributions. | ||
- | |||
==== Wb versus t ==== | ==== Wb versus t ==== | ||