radiation levels in cbm radiation effects ifluka (fluka c++ interface to cbmroot) fluka geometry...
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Radiation levels in CBMRadiation levels in CBM
• Radiation effects• iFluka (Fluka C++ interface to CbmRoot)• Fluka Geometry Models• Results• Conclusion
Radiation Damage EffectsRadiation Damage Effects
Total Ionizing Dose DisplacementDamage
Single Event Error
hard SEE soft SEE
clock
data input line
data in register
expected data in register
© T. Wijnands
2
MATERIAL CAUSE RADIATIONEFFECT
Semiconductors Electron-hole pair dose ionizationPhoton interaction photon
absorption Lattice displacement nucleon collision
Polymers Main and side chain rupture dose ionizationcross-linking degradation “ “gas evolution, radical productiondose rate
Ceramics Lattice displacements nucleon collision
trapped charge carriers dose ionizationcolor centers “ “
Metals Lattice displacements nucleon collision
nuclear reactions producing clusters “ “
voids and bubbles “ “
Radiation Effects – Rough Classification
© Lockheed Martin3
Semiconductors
Polymers
Ceramics
Metals and alloys
1E3 1E4 1E5 1E6 1E7 1E8 1E9 1E10 1E11 1E12 1E13 rad1E12 1E13 1E14 1E15 1E16 1E17 1E18 1E19 1E20 1E21 1E22 n/cm2
- no damage- mild to severe damage
- destruction
CBM
Radiation Damage to Materials/Electronics
Dose & Displacement Damage
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iFluka MotivationsiFluka Motivations
• Non intrusive interface • Fluka used in analogue or biased mode• C++ programming using FairRoot Class
Library– Generators ( Urqmd, etc ... )– Field maps definition– Standardized IO using Fairroot file structure– Parameters containers
iFluka DesigniFluka Design
FairRoot
iFluka FeaturesiFluka Features
• Fluka version 2006.3b• C++ FairRoot interface to native Fluka
– Enable usage of FairRoot class library directly• precise field maps info (CbmFieldMap)• external generators ( CbmUrqmdGenerator etc ..)• etc ...
– FairRoot IO supported• All Root IO +• Stack info: (CbmMCTrack)• Detector scoring info stored using CbmMCPoint
• General Fluka mesh normalization routine– directly linked with Fluka executable– Energy density -> Total Ionizing Dose (rad)– Fluence -> 1 MeV n-eq– etc ..
Radiation study settingsRadiation study settings
– Geometry models: • CBM cave ( based on technical drawings + modifs )• Magnets ( Muon + Active ) • MUCH ( compact design ) taken from CbmRoot• (1%) Au target
– Primary sources:• DPMJET-III (delta rays + beam / beam dump )• UrQmd (Au-Au mbias collisions @ 25 AGeV)
– Secondaries (transport):• Delta –rays: 50 KeV, hadrons 100 KeV• Low-energy neutrons library activated
FLUKA Geometry of the CBM Cave
Field Active Muon Field
Cave Global Diagnosis ( TID)Cave Global Diagnosis ( TID)
No Much
MUCH
Cave Global Diagnosis (fluence)Cave Global Diagnosis (fluence)
No MUCH
MUCH
Global Diagnosis Xsection X=0Global Diagnosis Xsection X=0
Fluence TID
MUCH
MUCH induced radiation MUCH induced radiation
Scoring planes Scoring planes
Much scoring planes
MDV+STS Scoring planes
Details : MVD @ z=5cm (TID)Details : MVD @ z=5cm (TID)MUCH no MUCH
Xsection X=0
Details : STS1 @ z= 30 cm (TID)Details : STS1 @ z= 30 cm (TID)MUCH no MUCH
Details : STS8 @ z= 100 cm (TID)Details : STS8 @ z= 100 cm (TID)MUCH no MUCH
Details : MVD @ z= 5 cm (Fluence)Details : MVD @ z= 5 cm (Fluence)MUCH no MUCH
Details : STS1 @ z= 30 cm (fluence)Details : STS1 @ z= 30 cm (fluence)MUCH no MUCH
Details : STS4 @ z= 50 cm (fluence)Details : STS4 @ z= 50 cm (fluence)MUCH no MUCH
Details : STS8 @ z= 100 cm (fluence)Details : STS8 @ z= 100 cm (fluence)MUCH no MUCH
Details : Much1 @ z= 130 cm (fluence)Details : Much1 @ z= 130 cm (fluence)MUCH no MUCH
Comparisons with other MCsComparisons with other MCs
MVD0 (TID) MVD0 Fluence
Radiation studies ( CBM-Wiki)Radiation studies ( CBM-Wiki)
Main Page Results tables
ConclusionConclusion
• MUCH option (study with Active Field Magnet)– Impact in Tracker region ( 30 cm < Z < 100 cm )– TID increases moderately with Z– Fluence increases x10 up to x100 with Z
• Soon effects due to Muon Magnet
• Results cross-checked with other MC´s
• Study of beam dump effect (PSD)• beam dump design
• Needed : feedback from detector groups
BACKUPSBACKUPS
Much : Energy densityMuch : Energy density
Much: Charged particles fluenceMuch: Charged particles fluence
Much: neutrons particles fluenceMuch: neutrons particles fluence
ConclusionConclusion
• iFluka ready to be used for radiation level
studies• On going work:
– More detailed Geometry– run time conversion to ROOT format for all
Fluka estimators– Normalization routine in C++– Comparison with TFluka (Validation)
( Collaboration with ALICE )
CBM radiation environmentCBM radiation environment
• Detectors– MVD + STS– MUCH
• Estimators:– Energy density ( GeV/cm3/primary )– Fluence ( 1 Mev n equivalent : n-equiv/cm2/primary)
GeometryGeometry
Scoring planes Scoring planes
Much scoring planes
MDV+STS Scoring planes
MVDs energy densityMVDs energy density
STS Energy density (1) STS Energy density (1) Sts 1 Sts 2
Sts 3 Sts 4
Sts energy density Sts energy density
STS 5STS 6
STS 7STS 8
MUCH energy densityMUCH energy densityMUCH 1 MUCH2
MUCH 3 MUCH 4
MUCH energy densityMUCH energy density
MUCH 5 MUCH 6
MVDs Charged particles fluenceMVDs Charged particles fluence
MVD 1 MVD 2
STS charged particles fluenceSTS charged particles fluenceSTS 1 STS 2
STS 3 STS 4
Sts charged particles fluenceSts charged particles fluenceSTS 5 STS 6
STS 7STS 8
MUCH charged particles fluenceMUCH charged particles fluenceMUCH 1 MUCH 2
MUCH 3 MUCH 4
Much charged particles fluenceMuch charged particles fluence
MUCH 5 MUCH 6
MVDs neutrons fluenceMVDs neutrons fluence
MVD 1 MVD 2
Sts neutrons fluenceSts neutrons fluenceSTS 1 STS 2
STS 3STS 4
Sts neutrons fluenceSts neutrons fluenceSTS 5 STS 6
STS 7 STS 8
MUCH neutrons fluenceMUCH neutrons fluenceMUCH 1 MUCH 2
MUCH 3 MUCH 4
MUCH neutrons fluenceMUCH neutrons fluence
MUCH 5 MUCH 6
ConclusionConclusion
• iFluka used to estimate fluences for MVD , STS and MUCH
• Need to overlay results from UrQmd with DPM (beam dump)
• Need more input from detector groups
• Compare with real data ( TRD ... ) and other MC ?
NIEL (1)NIEL (1)
• Displacement damage on Si lattice proportional to non ionizing energy transfer (NIEL) ( n, p, π+/-,e).
• To characterize the damage efficiency of a particle at E – Use of the normalized damage function D(E)/D(1Mev)– Tables taken from A.Vasilescu and G. Lindstroem
( http://sesam.desy.de/menbers/gunnar/Si-func.htm)
• Normalization of hadron fluence Φ :
Φ (1 MeV n-eq) = ∫ (D(E)/D(1 MeV)) Φ(E) dE
with D(1 MeV) = 95 MeV mb.
• Φ (1 MeV n-eq) : equivalent 1 MeV-n fluence
producing the same bulk damage
NIEL (2)NIEL (2)
CBM Cave GeometryCBM Cave Geometry
ZY view XZ view
The electronics caveThe electronics cave