CMS HCAL Test Beam Results and Comparison CMS HCAL Test Beam Results - - PowerPoint PPT Presentation

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CMS HCAL Test Beam Results and Comparison CMS HCAL Test Beam Results - - PowerPoint PPT Presentation

CMS HCAL Test Beam Results and Comparison CMS HCAL Test Beam Results and Comparison with GEANT 4 Simulation with GEANT 4 Simulation Jordan Damgov Jordan Damgov on behalf of the on behalf of the CMS HCAL Collaboration CMS HCAL Collaboration


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SLIDE 1

CMS HCAL Test Beam Results and Comparison CMS HCAL Test Beam Results and Comparison with GEANT 4 Simulation with GEANT 4 Simulation

Jordan Damgov Jordan Damgov

  • n behalf of the
  • n behalf of the

CMS HCAL Collaboration CMS HCAL Collaboration

CALOR '06 CALOR '06 Chicago June 5-9, 2006 Chicago June 5-9, 2006

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SLIDE 2

CMS Calorimeter system CMS Calorimeter system

Wedge, 20o

ECAL HCAL

Sampling calorimeter Scintillator Brass (70%Cu,30%Zn) 17 Layers

ECAL: PbWO4 crystals

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

See Julie Whitmore's talk for details

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SLIDE 3

The test beam setup is designed to preserve the interaction point-like geometry of CMS.

HB HE HO

Table

Beam

Interaction point like geometry Interaction point like geometry

IP=Pivot

EC

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 4

HB2 HB1 ECAL HE HO

“Magnet”

beam

Test beam setup Test beam setup

2 Hadron barrel wedges 1 Hadron endcap wedge Hadron outer calorimeter 7x7 crystals ECAL Material for Magnet Movable table in η-φ plane

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 5

BEAM

Light guides to PMTs

View from top

7x7 crystals=14x14 cm

HO

VM

HB1 HB2 Beam

Al

ECAL and HO ECAL and HO

ECAL is readout by PMTs. Light guides are attached to the front face of the crystals.

ECAL

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 6

ECAL H C A L B a r r e l HCAL Endcap

Trigger counters Wire Chambers

H C A L O u t e r C a l

  • r

i m e t e r

GEANT4 simulation GEANT4 simulation

M a g n e t C

  • i

l

  • Detailed HCAL geometry

with HB1&HB2 read-out schema.

  • ECAL – PbWO4 crystals, Al box

and Al block behind ECAL.

  • Beam line - trigger

counters and wire chambers

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 7

GEANT4 physics models validation GEANT4 physics models validation

Physics lists tested against the test beam data :

  • LHEP: LEP/HEP parametrized models for inelastic scattering.
  • QGSP: Quark Gluon String model for the “Punch-through”

interactions.

  • QGSC: QGSP + Chiral invariant phase-space decay.
  • FTFP: diffractive string excitation similar to that in FRITOF and

Lund

In this comparison is used Geant 4.6.2.p02 Parametrized: LHEP-3.7 Model based: QGSP-2.8

QGSC-2.9 and FTFP-2.8 produce very similar to QGSP-2.8 results.

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 8

80 GeV/c SCI_VLE CK2 CK3 WC A,B,C

HCAL HCAL ECAL ECAL

V3,V6 VM

P-ID: Cerenkov counter (CK2) - electron Cerenkov counter (CK3) - pion / kaon / proton Scintillators (V3, V6, VM) – muon tagging

VLE tag against punchthrough muon

Wire Chambers (WC A,B,C): single hit to reject interaction in beam line

S1-S4

Beam trigger counters

Available beam tunes: pions 2-300 GeV muons 80/150 GeV electrons 9-100 GeV

Beam line with particle identification 2-300 GeV/c Beam line with particle identification 2-300 GeV/c

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 9

Beam contamination and cleaning Beam contamination and cleaning

Beam cleaning:

  • The particle Id counters are used for beam with

momentum from 2 to 15 GeV

  • Calorimeter based cuts: use the particle Id

capabilities of the calorimeters. High energy muons a tagged by the muon veto counters with 99% efficiency. Low energy muons form pion decay are evaluated to be less then 1.5% for 9 GeV and below. Beam contamination before the clean up:

Pbeam mu el- [GeV] [%] [%] 300 0.7 150 2 100 2 50 2.5 30 3.5 7 15 11 35 10 7 70 9 1.5 6 7 3.5 10 5 5.5 6 3 30 30 2 85 7

VLE beam line

+ interaction in the beam line 2 and 3 GeV are not used

e-

pi- 30GeV

µ

Electrons are clearly identify by ECAL/HCAL energy deposition.

Any remaining uncertainty in the beam contamination and interaction in the beam line is added to the systematics of the measurement.

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ECAL [GeV] HCAL [GeV]

Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 10

Uniformity calibration and Energy Scale Uniformity calibration and Energy Scale

forward backward

signal

Wire source

Scintillator

The uniformity calibration is done with Co60,

per-tower and per-layer

Energy scale:

ECAL: 100 GeV e- HCAL: 50 GeV pi- with MIP in ECAL.

Reconstructed energy: Erec=a*EECAL+b*EHCAL

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

See Mayda Velasco's talk

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SLIDE 11

Energy spectra ECAL+HCAL: data vs GEANT4 Energy spectra ECAL+HCAL: data vs GEANT4

300 GeV 50 GeV 10 GeV 5 GeV 7 GeV

Good agreement between data and GEANT4 prediction.

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 12

Calorimeter response to pions Calorimeter response to pions

Important for Jets

ECAL+HCAL

GEANT4 models correctly the calorimeter response to pions in broad energy

  • range. Correct representation of the single hadron response at low energy is

important for simulation of the calorimeter response to jets.

Some discontinuity is observed at 7-10 GeV in the GEANT4 prediction. 12 12

Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

100 10 5 3 30

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SLIDE 13

HCAL alone: MIP in ECAL is required. HO is not used in this measurement to compensate the HB leakage on the back

HCAL alone

HCAL alone response to pions HCAL alone response to pions

10 100 300 30

LHEP models better the high energy calorimeter response. QGSP has less leakage

  • n the back

due to shorter shower.

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 14

Proton over pion response ratio Proton over pion response ratio

Significant difference in the calorimeter response to protons with respect to pions is observed in the data and is well represented in the GEANT4 simulation.

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

Protons have 15% Protons have 15% lower response then lower response then pions at this pions at this energies. energies. We will remeasure We will remeasure it this summer with it this summer with improved particle Id. improved particle Id.

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SLIDE 15

Longitudinal shower profile measurement Longitudinal shower profile measurement

Electromagnetic shower profile in HCAL

Very good agreement between test beam data and GEANT4 prediction.

Modified read-out: redesigned optical decoding units to allow longitudinal shower measurement

e- 100 GeV beam HB2 Optically masked out

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 16

pi 5 GeV

LHEP and QGSP show good agreement with test beam data at low and intermediate energies.

pi 30 GeV pi 10 GeV

Longitudinal shower profile measurement (cont.) Longitudinal shower profile measurement (cont.)

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SLIDE 17

MIP in ECAL MIP in L0

QGSP physics list has shorter shower profile for incident particles with high momentum.

QGSP LHEP

Longitudinal shower profile measurement (cont.) Longitudinal shower profile measurement (cont.)

pi 300 GeV

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

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SLIDE 18

HCAL - ECAL response to very low energy pion beam HCAL - ECAL response to very low energy pion beam

ECAL response is higher in GEANT4 at low energy: geometry or physics or ...?

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

5 GeV 7 GeV 7 GeV 5 GeV

TB TB G4 G4

5 GeV

TB

5 GeV

G4

ECAL [GeV]

ECAL [GeV]

ECAL [GeV]

ECAL [GeV] HCAL [GeV] HCAL [GeV] HCAL [GeV] HCAL [GeV] ECAL [GeV] ECAL [GeV]

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SLIDE 19

Cluster-based response compensation Cluster-based response compensation

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results

Dan Green 70% Stochastic 8% Constant σ/E E [GeV] Uses test beam data to fit the intrinsic electron to hadron response (e/h) and the average neutral fraction f0 of the ECAL and HCAL as a function of the raw total calorimeter energy, E + H. Fractional energy resolution for pions.

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SLIDE 20

Conclusions and Outlook Conclusions and Outlook

Calorimeter response for momentum range 5-300 GeV/c was measured with test beam in 2004. GEANT4 is in good overall agreement with the data LHEP shows best agreement We observed small discrepancy in the following quantities : 1)Longitudinal shower shape for 150-300 GeV/c pions, modeled by QGSP physics list 2)Discontinuity in the calorimeter response in 7-10 GeV/c range 3)ECAL response to very low energy pion beam is higher in the GEANT4 simulation .

We plan to repeat the measurements this summer with ECAL production super-module and improved particle Id.

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Jordan Damgov CALOR06 – CMS HCAL Test Beam Results