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Performance of the PtmissPlusLeptonsFilter

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developed for the invisible Higgs analysis in HZ channel with Z l l ... Use 8 discriminative variables in a likelihood analysis to extract signal ... – PowerPoint PPT presentation

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Title: Performance of the PtmissPlusLeptonsFilter


1
Performance of the PtmissPlusLeptonsFilter
  • Pauline Gagnon and Siva Subramania
  • Indiana University

developed for the invisible Higgs analysis in HZ
channel with Z ? l l
2
Z0H0? ll- invisible initial analysis
strategy(Fortran-based ATLFAST,
ATL-PHYS-PUB-2005-011)
  • Trigger 1 or 2 prompt leptons
  • Preselection
  • large missing pT
  • 2 leptons of opposite sign and same flavour
  • loose cut on Z mass
  • Final selection
  • Use 8 discriminative variables in a likelihood
    analysis to extract signal

3
Invisible Higgs decay in HZ channelall MC
samples generated with Pythia
  • Signal
  • H ? ?? and Z ? l l
  • Large missing pT
  • Two prompt leptons forming a Z
  • Main backgrounds
  • ZZ ? l l ??
  • Z inclusive with Z ? l l and jets lost in the
    beam pipe
  • tt ? b l ? b l ? with bb jets lost in the beam
    pipe
  • W W ? l ? l ?
  • W Z ? l l l ? with one lepton lost in the beam
    pipe
  • ZZ ? l l ??

4
Most background were rejected at preselection
level in ATL-PHYS-PUB-2005-011
Create a filter to emulate preselection cuts
ptmiss cut, 2 leptons reconstructing a Z with
loose mass cut
5
Missing pT in reconstruction code
  • Missing pT - ? (visible transverse energies)
  • Isolated photons, electrons and muons
  • Jets, b-jets and c-jets
  • Clusters not accepted as jets
  • Non-isolated muons not added to a jet
  • Transverse energies in cells not used elsewhere

6
Missing pT at generator level
  • Vectorial sum of transverse momenta of
  • Invisible particles (stable Higgs, neutrinos)
  • Lost particles those falling outside the
    detector acceptance region
  • Calorimeter acceptance ? lt 5.0

Ptmiss calculated differently in filter and full
reconstruction chain So we are not comparing the
same object
7
Second handle in filter leptons
  • Two leptons within the tracker acceptance region
  • One or both leptons must pass the lepton trigger
    requirements
  • Two leptons of same flavor but opposite sign
  • The reconstructed mass must be close to mZ

8
Filter versus preselection cuts
  • Filter cuts looser cuts
  • 2 leptons with ?lt 2.7
  • Trigger requirements
  • - 1 e with pT gt 18 GeV or
  • - 2 e with pT gt 23 GeV or
  • - 1 µ with pT gt 8 GeV or
  • - 2 µ with pT gt 13 GeV
  • Missing pT gt 50 GeV
  • mZ 55 GeV
  • Preselection cuts
  • 2 leptons with ?lt 2.5
  • Trigger requirements
  • - 1 e with pT gt 20 GeV or
  • - 2 e with pT gt 25 GeV or
  • - 1 µ with pT gt 10 GeV or
  • - 2 µ with pT gt 15 GeV
  • Missing pT gt 90 GeV
  • mZ 50 GeV

9
Comparison with ATLFAST 10.5.0
Conclusion no significant event loss at the
filter level w.r.t. ATFAST with 10.5.0 or 11.0.41
(mZ cut)
10
Cross-check no statistical difference between
filtered and unfiltered events at AOD level
11
CPU time savings to simulate 100 fb-1 of data
From 8360 CPU years down to 20 CPU years
12
Cut flow on ATLFAST AOD after filter with mZ cut
jet and b-tag values not yet reliable in ATLFAST
13
  • Reference plots done with ATLFAST AOD for
    unfiltered and filtered before selection
  • for HZ events (plots are superimposed)

14
Reference plots after selection unfiltered and
filtered HZ events(stacked histograms)
pT lepton 2
pT lepton 1
Cos between leptons (3D)
Cos between leptons (2D)
15
Reference plots after selection unfiltered and
filtered HZ events(stacked histograms)
transverse mass
missing pT
Cos pTmiss-pT lepton 1
mZ
16
Filter performance with full AOD
  • Tested with 1000 fully reconstructed events for
    HZ ???l l and for ZZ ? l l ??
  • More checks in progress with ttbar samples
  • All events preselected on fully reconstructed AOD
    events were retained by the filter

This filter should be used when producing signal
and background samples for HZ ??? l l analysis
17
Comparison of cut flow for fast and full
reconstruction
18
Conclusion
  • This filter significantly reduces the amount of
    events to be reconstructed
  • There is no significant loss of events for signal
    and main backgrounds w.r.t. events preselected
    with ATLFAST and full simulation AOD
  • Filter has been tested with releases 10.5.0 and
    11.0.41 yielding consistent results
  • This filter should be used for official signal
    and background production for invisible Higgs in
    HZ channel
  • Filter is going to be in release 11.5.0
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