Validation of the ATLAS Hadronic Calibration with LAr End-Cap Beam - - PowerPoint PPT Presentation

validation of the atlas hadronic calibration with lar end
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Validation of the ATLAS Hadronic Calibration with LAr End-Cap Beam - - PowerPoint PPT Presentation

Validation of the ATLAS Hadronic Calibration with LAr End-Cap Beam Tests data Teresa Barillari, MPI M unchen Calor 2008 Pavia, 26 - 30 May 2008 Introduction Hadronic Calibration Performances Linearity and Resolution Cluster


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SLIDE 1

Validation of the ATLAS Hadronic Calibration with LAr End-Cap Beam Tests data

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008

Introduction Hadronic Calibration Performances Linearity and Resolution Cluster Moment distributions Outlook

  • n behalf of the ATLAS LAr End-Cap Group:

Canada, China, France, Germany, Russia, Slovakia, Spain, U.S.A.

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SLIDE 2

Introduction

In this talk I will present the initial studies done to validate the MC simulation using the full ATLAS hadronic calibration procedure (see talk from G. Pospelov) with the EMEC-HEC-FCal beam tests data The data shown are πs obtained in the H6 2004 combined beam tests (see talk from P . Strizenec). They correspond to an ATLAS region 2.5 < |η| < 4.0, and cover a energy range 40 ≤ E ≤ 200GeV The MC simulation used in this analysis consists πs obtained using Geant 4 8.3 QGSP EMV To preliminary compare the MC with the beam tests data, the full ATLAS Geant 4 MC has been restricted so to approximately describe the beam tests area Results are presented for data taken at point D (EMEC-HEC) and and at point H (FCal), see red circles in the right figure

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 2

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SLIDE 3

Hadronic Calib. Performance: πs at Point D

Plots show the total reconstructed energy over the nominal beam energy for 60 GeVπ and 200 GeVπ at Point D for EM-scale (red); weighted (green); weighted + OOC (blue); weighted + OOC + DM (black) Data point D: 60 GeVπ

  • Mean improves in every step:

after em = 0.684, after weight = 0.780, after ooc = 0.844, after dm = 0.943

  • Resolution remains about

constant: after em = 16.27%,

after weight = 16.41%, after ooc = 15.7%, after dm = 15.63%

  • Final deviation from

Ereco/Eπ = 1 is 5.7%

π

/E

reco

E

0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 1.3 1.4 1.5 20 40 60 80 100 120 140 160

h_em Entries 3632 Mean 0.6988 RMS 0.104 Mean of the fit 0.6842 Sigma of the fit 0.1137 h_w Entries 3632 Mean 0.7883 RMS 0.1279 Mean of the fit 0.7804 Sigma of the fit 0.13 h_ooc Entries 3632 Mean 0.8456 RMS 0.1363 Mean of the fit 0.8436 Sigma of the fit 0.1358 h Entries 3632 Mean 0.944 RMS 0.1532 Mean of the fit 0.943 Sigma of the fit 0.1496

Data point D: 200 GeVπ

  • Mean improves in every step

after em = 0.756, after weight = 0.869, after ooc = 0.906, after dm = 0.993

  • Resolution improves in every

step after em = 12.61%,

after weight = 11.09%, after ooc = 10.91%, after dm = 10.39%

  • Final deviation from the

Ereco/Eπ = 1 is ≈ 0.7%

π

/E

reco

E

0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 1.3 1.4 1.5 100 200 300 400 500 600 700 800 900

h_em Entries 17223 Mean 0.756 RMS 0.08915 Mean of the fit 0.7556 Sigma of the fit 0.08684 h_w Entries 17223 Mean 0.8657 RMS 0.09844 Mean of the fit 0.8686 Sigma of the fit 0.08773 h_ooc Entries 17223 Mean 0.9019 RMS 0.1038 Mean of the fit 0.9056 Sigma of the fit 0.09061 h Entries 17223 Mean 0.9863 RMS 0.1142 Mean of the fit 0.9929 Sigma of the fit 0.09878

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 3

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SLIDE 4

Linearity and Resolution at Point D

Plots show the linearity and the resolution for 40 GeV ≤ π ≤ 200 GeV, data and MC, at Point D. Full (open) red circles are data (MC) at EM-scale. Full (open) black triangles are data (MC) after weighting + OOC + DM corrections Linearity at point D:

  • There is a difference between

data (π) and MC at 40 and 60 GeV. At higher energies the calibrated data are in fairly good agreement with the MC

(MeV)

π

E 40 60 80 100 120 140 160 180 200

3

10 ×

π

/E

reco

E 0.5 0.6 0.7 0.8 0.9 1 1.1

Resolution at point D:

  • The MC gives an overall better

resolution than the data, both at EM-scale and after calibration corrections

(MeV)

π

E 40 60 80 100 120 140 160 180 200

3

10 × /E σ 0.06 0.08 0.1 0.12 0.14 0.16 0.18 0.2 0.22 0.24

We know the noise in the data is higher than in the MC. We also know that the lateral shower shape of Geant 4 QGSP doesn’t describe data

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 4

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SLIDE 5

Energy Density Moment at Points D and H

Plots show the energy density cluster moment: log10(

  • cells

Ecell Vcell ∗Ecell

  • cells Ecell

) for 200 GeVπ at Point D (left plot) and H (right plot)

))

3

> (MeV/mm ρ (<

10

log

  • 4
  • 3.5
  • 3
  • 2.5
  • 2
  • 1.5
  • 1
  • 0.5

0.005 0.01 0.015 0.02 0.025 0.03 0.035 0.04 0.045

200 GeV π Point D, Data MC

))

3

> (MeV/mm ρ (<

10

log

  • 4
  • 3.5
  • 3
  • 2.5
  • 2
  • 1.5
  • 1
  • 0.5

0.01 0.02 0.03 0.04 0.05 0.06

200 GeV π Point H, Data MC

At both points D and H the MC has slightly higher energy density than the data, we can say it reasonable describes the data The energy density moment is used in the calibration procedure for separation of hadronic from electromagnetic showers

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 5

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SLIDE 6

Second Radial Moment at Points D and H

Plots below show the sqrt of the second radial moment (lateral spread) for 200 GeVπ at points D (left plot) and H (right plot)

(mm)) >

2

<r 20 40 60 80 100 120 140 160 180 200 0.005 0.01 0.015 0.02 0.025 0.03 0.035 0.04 0.045

200 GeV π Point D, Data MC

(mm)) >

2

<r 20 40 60 80 100 120 140 160 180 200 0.02 0.04 0.06 0.08 0.1 0.12

200 GeV π Point H, Data MC

Even though there is a shift to the right, at point H the MC describes the data. At point D the MC fails to describe the data The shower model used in MC physics list doesn’t describe the data well

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 6

slide-7
SLIDE 7

Outlook

We have started to validate the ATLAS Hadronic Calibration procedure using the LAr End-Cap Beam Tests data In the studies shown in this presentation we see that the MC Geant 4 8.3 QGSP EMV has problems to describe the data We need and we are working to have a proper beam tests MC simulation Once a test-beam MC simulation is available, further improvements for the hadronic calibration procedure (EM-scale, weighting, OOC and dead material correction) can be done These are the first validation results with LAr end-cap beam tests data obtained so far

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 7

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SLIDE 8

BACKUP SLIDES

slide-9
SLIDE 9

Hadronic Calib. Performance: πs at Point H

Plots below show Ereco/Eπ for π in Point H for EM-scale (red); weighted (green); weighted + OOC (blue); weighted + OOC + DM (black). Data point H: 60 GeVπ

  • Mean improves in every step, the

resolution becomes worse

  • Final deviation from

Ereco/Eπ = 1 is 6.03%

π

/E

reco

E

0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 1.3 1.4 1.5 50 100 150 200 250 300

h_em Entries 9570 Mean 0.7124 RMS 0.1138 Mean of the fit 0.694 Sigma of the fit 0.1256 h_w Entries 9570 Mean 0.7345 RMS 0.1167 Mean of the fit 0.7223 Sigma of the fit 0.125 h_ooc Entries 9570 Mean 0.8596 RMS 0.1401 Mean of the fit 0.8564 Sigma of the fit 0.1396 h Entries 9570 Mean 0.9397 RMS 0.1688 Mean of the fit 0.9347 Sigma of the fit 0.166

Data point H: 200 GeVπ

  • Mean and resolution improve in

every step of the corrections

  • Final deviation from the

Ereco/Eπ = 1 is ≈ 7.21%

π

/E

reco

E

0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 1.3 1.4 1.5 100 200 300 400 500 600 700

h_em Entries 17163 Mean 0.7787 RMS 0.09803 Mean of the fit 0.7798 Sigma of the fit 0.0956 h_w Entries 17163 Mean 0.8126 RMS 0.1028 Mean of the fit 0.8173 Sigma of the fit 0.09749 h_ooc Entries 17163 Mean 0.8787 RMS 0.1133 Mean of the fit 0.8865 Sigma of the fit 0.1031 h Entries 17163 Mean 0.9202 RMS 0.1213 Mean of the fit 0.9279 Sigma of the fit 0.1082

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 9

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SLIDE 10

Linearity and Resolution at Point H

Plots show the linearity and the resolution for data and MC at Point H. Full (open) red circles are data (MC) at EM-scale. Full (open) black triangles are data (MC) after weighting + OOC + DM corrections Linearity at point H:

  • The calibrated data (for

E > 40 GeV) show a fairly good agreement with the MC

(MeV)

π

E 40 60 80 100 120 140 160 180 200

3

10 ×

π

/E

reco

E 0.5 0.6 0.7 0.8 0.9 1 1.1

Resolution at point H:

  • In the low energy region the data

have a better resolution than the

  • MC. In the higher energy bins the

MC performs better. The dead material correction are problematic in this region for both data and MC.

(MeV)

π

E 40 60 80 100 120 140 160 180 200

3

10 × /E σ 0.05 0.1 0.15 0.2 0.25 0.3

Teresa Barillari, MPI M¨ unchen Calor 2008 Pavia, 26 - 30 May 2008 10