Changes between Version 1 and Version 2 of Korea2020-04-CMS-HIG-18-011


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Timestamp:
Feb 10, 2020, 3:05:10 PM (5 years ago)
Author:
Eric CONTE
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  • Korea2020-04-CMS-HIG-18-011

    v1 v2  
    1 dede
     1= The second !MadAnalysis 5 workshop on LHC recasting @ Korea =
     2= Analysis 4: CMS-HIG-18-011 =
     3
     4||= Students =||  ||
     5||= Supervisor(s) =|| Robin Ducrocq ||
     6
     7
     8== 1. Analysis summary ==
     9
     10
     11== 2. Analysis global information ==
     12
     13*  CMS contact person: nobody
     14*  Center of mass energy: 13 TeV
     15*  Integrated luminosity: 35.9 fb−1
     16*  Link to the public CMS page: http://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-18-011/
     17
     18== 3. Selection description ==
     19
     20=== 3.1 Trigger selection ===
     21
     22Only events using single-electron OR single-muon triggers are accepted:
     23- single-electron: one electron with pT > 24 GeV
     24- single-muon: one muon with pT > 20 GeV
     25
     26PS: This part cannot usually be described by the fast-simulation of detector.
     27
     28=== 3.2 Object definition ===
     29
     30*   electron:
     31      * pT > 7 GeV,
     32      * |eta|<2.47. Are excluded electrons in the end-cap, i.e. 1.37 < |eta| < 1.52.
     33      * 'medium' likelihood identification.
     34      * transverse impact parameter: |d0|/err(d0) < 5.
     35      * longitudinal impact parameter: |z_0 x sin\theta | < 0.5 mm
     36      * isolation criterion:
     37         * sum PT of tracks in a cone around the electron (the electron track is subtracted) of size = min(10 GeV/PT,0.2) < 6% electron PT.
     38         * sum ET of clusters in a cone around the electron (the electron cluster is subtracted) of size DR=0.2 < 6% electron PT.
     39       
     40 
     41*   muon:
     42      * pT > 7 GeV
     43      * |eta|<2.4
     44      * 'medium' identification.
     45      * transverse impact parameter: |d0|/err(d0) < 3.
     46      * longitudinal impact parameter: |z_0 x sin\theta | < 0.5 mm
     47      * isolation criterion: sum PT of tracks in a cone around the muon (the muon track is subtracted) of size = min(10 GeV/PT,0.3) < 6% muon PT.
     48 
     49*   jet:
     50      * clustering: anti-kT with =0.4
     51      * pT > 25 GeV
     52      * |eta|<2.5
     53      * Pile-up rejection: jets with pT < 60 GeV and |η| < 2.4 are required to satisfy pile-up rejection criteria (JVT)
     54
     55*   b-jet: MV2c20 algorithm. In simulation, the tagging algorithm gives a rejection factor of about 130 against light-quark and gluon jets, and about 4.5 against jets containing charm quarks.
     56   
     57*   preventing double-counting:
     58      * the closest jet within DR=0.2 cone of an electron is removed.
     59      * if, after the previous selection cut, the nearest jet of an electron is in DR=0.4 cone, then the electron is removed.
     60      * muons in a DR=0.4 cone around a given jet are removed. BUT if the jet has fewer than three associated tracks, the muon is kept.
     61
     62
     63=== 3.3 Cut-flow chart ===
     64
     65'''Common:'''
     66
     67  * 0. Trigger confirmation: at least one lepton (muon/electron) with PT > 25 GeV
     68
     69
     70'''1. Analysis 1: SS-muons'''
     71
     72  * 1.1. 2 muons of same charge, with PT > 25 GeV
     73  * 1.2. Events with additional leptons are vetoed
     74  * 1.3. MET > 40 GeV
     75  * 1.4. HT > 240 GeV
     76  * 1.5. At least 2 b-jets
     77
     78
     79'''2. Analysis 2: trilepton analysis'''
     80   
     81  * 2.1. Exactly 3 leptons
     82  * 2.2. 2 opposite sign, same flavour leptons, and
     83  * 2.2. Leading lepton with PT > 25 GeV, the other leptons with PT > 20 GeV
     84  * 2.3. Defining 4 signal regions according the final states:
     85    * 3l-Z-1b4j
     86    * 3l-Z-2b3j
     87    * 3l-Z-2b4j
     88    * 3l-noZ-2b
     89  * 2.4. Compatibility with a Z:
     90    * [3l-Z-1b4j]+[3l-Z-2b3j]+[3l-Z-2b4j]: compatible with a Z i.e. (invM-MZ)<10 GeV
     91    * [3l-noZ-2b]: not compatible with a Z i.e. (invM-MZ)>10 GeV
     92  * 2.5. Number of light jets (no b-jet):
     93    * [3l-Z-2b3j]: #jets = 3
     94    * [3l-Z-1b4j]+[3l-Z-3b4j]: #jets >= 4
     95    * [3l-noZ-2b]: #jets = 2, 3 or 4
     96  * 2.6. Number of b-jets:
     97    * [3l-Z-1b4j]: #b-jets = 1
     98    * [3l-Z-2b3j]+[3l-Z-3b4j]+[3l-noZ-2b]: #b-jets >= 2
     99
     100'''3. Analysis 3: tetralepton analysis'''
     101
     102  * 3.1. Exactly 4 leptons
     103  * 3.2. 2 pairs of opposite sign
     104  * 3.3. At least one pair must have same flavour leptons
     105  * 3.4. We define Z1 = reconstructed Z from opposite-sign same-flavour pair the closest to the Z mass. We define Z2 = reconstructed Z from the other pair (same-flavour or not).
     106  * 3.5. Defining 4 signal regions according the final states:
     107    * 4l-DF-1b
     108    * 4l-DF-2b
     109    * 4l-SF-1b
     110    * 4l-SF-2b
     111  * 3.5. Cut on PT34 = scalar sum of the transverse momenta of the leptons used in Z2:
     112    * [4l-DF-1b]: PT34 > 35 GeV
     113    * [4l-SF-1b]: PT34 > 25 GeV
     114  * 3.6. MET:
     115    * [4l-SF-1b]: If |MZ2-MZ| > 10 GeV then imposing MET > 40 GeV else imposing MET > 80 GeV
     116    * [4l-SF-2b]: If |MZ2-MZ| < 10 GeV then imposing MET > 40 GeV
     117  * 3.7. Number of b-jets:
     118    * [4l-DF-1b]+[4l-SF-1b]: #b-jets = 1
     119    * [4l-DF-2b]+[4l-SF-2b]: #b-jets >= 2
     120
     121=== 3.4 Definition of exotic observables ===
     122
     123No exotic observables.
     124
     125== 3. Detector simulation ==
     126
     127Official Delphes package could be enough.
     128
     129To improve the realism of the simulation, Delphes_Track could be used for cutting on D0. Is it necessary? To try...
     130
     131== 4. Validation material ==
     132
     133=== 4.1 Monte-Carlo samples ===
     134
     135* LO (but xsections are normalized to NLO)
     136* Model used: SM
     137  * Mtop = 172.5 GeV
     138  * Mhiggs = 125 GeV
     139  * processes = ttZ (including gamma*) & ttW (but no ttWW)
     140  * xsections: Table 5 of ATL-PHYS-PUB-2016-005
     141* MC generator program (name + version): MG5_aMC
     142* Shower program (name + version): Pythia v8.210
     143* Tune of Pythia: A14 tune (see http://cds.cern.ch/record/1966419)
     144* PDF set: NNPDF2.3LO
     145* ME/PS merging????
     146
     147=== 4.2 Reference plots / cut-flows ===
     148
     149* MC xsections and plots: http://cds.cern.ch/record/2120826/files/ATL-PHYS-PUB-2016-005.pdf?version=1:
     150  * Table 5
     151  * Figure 5
     152
     153* Final number of signal events after the selection in each signal region:
     154  * https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2015-22/tabaux_06.pdf
     155
     156* Plots for Analysis 1: SS-muons:
     157  * Figure 1 of the paper
     158
     159* Plots for Analysis 2: trileptons
     160  * Figure 5 of the paper
     161
     162* Plots for Analysis 3: tetraleptons
     163  * Figure 6 of the paper
     164
     165* Rivet analyses
     166
     167
     168== 4. Validation results ==
     169
     170== 5. Reinterpretation (optional) ==
     171
     172== 6. Questions / issues ==
     173
     174