study of calorimeter performance using the lc full simulator
DESCRIPTION
Study of Calorimeter performance using the LC full simulator. The 8th ACFA Workshop Yoshihiro Yamaguchi (Tsukuba U.). M. -C. Chang (RCNS, Tohoku U.) K. Fujii (KEK) T. Fujikawa (RCNS, Tohoku U.) S. Kim (Tsukuba U.) H. Matsunaga (Tsukuba U.) A. Miyamoto (KEK) T. Nagamine (RCA, Tohoku U.). - PowerPoint PPT PresentationTRANSCRIPT
Study of Calorimeter Study of Calorimeter performance using the LC full performance using the LC full
simulatorsimulator
The 8th ACFA WorkshopYoshihiro Yamaguchi (Tsukuba U.)
M. -C. Chang (RCNS, Tohoku U.)K. Fujii (KEK)T. Fujikawa (RCNS, Tohoku U.)S. Kim (Tsukuba U.)H. Matsunaga (Tsukuba U.)A. Miyamoto (KEK)T. Nagamine (RCA, Tohoku U.)
H. Ono (Niigata U.)A. L. C. Sanchez (Niigata U.)T. Takeshita (Shinshu U.)A. Yamaguchi (Tsukuba U.)S. Yamamoto (Graduate U.)T. Yoshioka (ICEPP, Tokyo U.)…
2005/07/12 The 8th ACFA Workshop 2
ContentsContentsIntroductionCalorimeter geometryAmount of materialsEM CAL PerformanceHD CAL PerformanceFine segmented Cell Study of Digital calorimeterSummary & Future plan
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SolenoidSolenoid
TPCTPC
ITIT
Standard Geometry (GLD)Standard Geometry (GLD)
Muon/IronMuon/Iron
Hadron CalorimeterHadron Calorimeter
EM CalorimeterEM Calorimeter VTXVTX
Forward CalForward Cal
Jupiter is Full simulator and MC truth generatorBased on Geant4
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Calorimeter in JupiterCalorimeter in Jupiter
Perform an analysis with ideal geometry to know ultimate performance.
Each tower with one HD tower (12cm12cm) and 33 EM tower (4cm4cm) is pointing to an interaction point.
No crack between towers.
Tower geometry and material can be modified easily.
Implement realistic geometry in the next step.
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Parameter List
EM + HDHDCal 130Layers: 6.1 0
EMCal 38Layers: 27X0
Lead 8mm
Scinti. 2mm
Lead 4mmDivide 33
12cm
Scinti. 1mm
Cut CalorimeterTower
12cm
Endcap Inner R = 40cm Barrel Tower Front R = 210cm Endcap Tower Front R = 270cm
Calorimeter geometryCalorimeter geometry
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Amount of MaterialsAmount of Materials
Radiation Length = 0.05 ~ 0.2 X0
(5.4X0 at cos = 0) Nuclear Interaction
Length = 0.02 ~ 0.1 0
(2.8 0 at cos = 0)
Radiation Length andNuclear Interaction Lengthmeasured from interactionpoint to CAL front.
X0
X00
0
cos cos
cos cos
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Event DisplayEvent Display (single electron)
1GeV electron incident angle to CAL is very small due to a magnetic field.
1GeV EM shower stops in the early depths in EM CAL.
1GeV1GeV
TPC
EMCAL
HDCAL
10GeV10GeV
TPC
EMCAL
HDCAL
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EM CAL Performance (electron)EM CAL Performance (electron)
Worse resolution and non-linearity at 1GeV is due to shower stopping at the early depth of EM CAL.
Energy [GeV]
En
erg
y D
ep
os
it [
Ge
V]
LinearityLinearity
De
via
tio
n [
%]
Energy [GeV]
Deviation from LinearityDeviation from Linearity
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HD CAL Performance (pion)HD CAL Performance (pion)
Large non-linearity in the low energy region. Under investigation.
Deviation from LinearityDeviation from LinearityLinearity (QGSP)Linearity (QGSP)
Energy [GeV]
En
erg
y D
epo
sit
[GeV
]
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HD CAL Performance (pion)HD CAL Performance (pion)
QGSP :
LHEP :
No Sol : (QGSP)
Front Cal : (QGSP)
Beam Test:
sto = 40.61.1 %con = 7.10.3 %
sto = 38.01.2 %con = 9.00.8 %
sto = 39.31.2 %con = 8.40.6 %
sto = 44.91.4 %con = 4.30.4 %
sto = 46.330.35 %con = 0.90.4 %
Beam test from NIMA 487 (2002) 291-307Configuration is 8mm lead and 2mm sinti.No EM Detector
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Fine segmented CellFine segmented Cell
Set new CAL geometry EM CAL divided 1212, Cell size = 0.83 ~ 0.92cm HD CAL divided 1212, Cell size = 0.92 ~ 1.4cm
Use Hadron PhysicsList: QGSP To study coarser segmentation, we sum the
energy deposits in adjacent cells.
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Event Display (single pion)Event Display (single pion) pink -> electronblue -> muonyellow -> photonred -> piblack -> K0Lgreen -> protonpurple -> neutrongray -> other
TPC
EMCAL
HDCAL
Cell Size = 1cmx1cm
TPC
EMCAL
HDCAL
Cell Size=EM 4cmx4cm, HD=12cmx12cm
Incident particle: - 100GeV Exact hits of TPC and merged hits of CAL are displayed. Color shows which particle makes hit.
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Digital calorimeterDigital calorimeter
Incident particle: -, 2 ~ 200GeV, 500event Select - punching through EM CAL as a MIP. Non-linearity observed in # of hits. Large constant term in energy resolution.
Energy [GeV]
Mea
sure
d h
its
# of hits
10GeV10GeV
LinearityLinearity
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Definition of hitDefinition of hit
Blue cell is 1 hitRed cell is 2 hits
# of hits in a cellF
ract
ion
of
# o
f h
its
in a
cel
l [%
] 1cm1cm: single hit ~100 % 2cm2cm: single hit ~70% Large difference between 1cm 1cm
and 2cm2cm. Segmentation should be < 2cm2cm.
1 particle 2 particles
# of hits in a cell” is defined by the # of original particles incident onto the calorimeter which cause the cell hit.
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Summary & Future planSummary & Future plan
HD cal simulation does not reproduce beam test results. Discrepancy is observed in the resolution constant term. Large non-linearity in the low energy region.
Need more extensive study. Cell size less than 2cm2cm is favorable for PFA.
We plan to study the calorimeter clustering with digital calorimeter.
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Buck up
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Jupiter/Satellites ConceptsJupiter/Satellites Concepts
JUPITERJLC Unified
Particle Interactionand
Tracking EmulatoR
IO Input/Outputmodule set
URANUSLEDA
Monte-Calro Exact hits ToIntermediate Simulated output
Unified Reconstructionand
ANalysis Utility Set
Library Extention for
Data AnalysisMETIS
Satellites
JSF/ROOT basedFramework
Geant4 basedSimulator
MC truth generator Event Reconstruction
Tools for simulation For real data
Used Geant4.7.0.p01 and root.4.03.04Used Geant4.7.0.p01 and root.4.03.04
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HD CAL PerformanceHD CAL Performance
QGSP :
LHEP :
LCPhysics :
No Sol : (QGSP)
Front Cal : (QGSP)
Beam Test:
sto = 40.61.1 %con = 7.100.29 %
sto = 38.01.2 %con = 9.020.79 %
sto = 25.71.3 %con = 17.420.43 %
sto = 39.31.2 %con = 8.370.55 %
sto = 44.91.4 %con = 4.290.38 %
sto = 46.330.35 %con = 0.840.38 %
Beam test from NIMA 487 (2002) 291-307Configuration is 10mm lead and 2.5mm sinti.
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Definition of hitDefinition of hit “# of hits in a cell” is defined by the # of original particles
incident onto the calorimeter which cause the cell hit.
1 particle 2 particles
Blue cell is 1 hitRed cell is 2 hits
Scintillator