Geant4 simulations - Indico...2016/02/12 · at gunpoint N photons in the SiPMs (polished channel)...
Transcript of Geant4 simulations - Indico...2016/02/12 · at gunpoint N photons in the SiPMs (polished channel)...
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Geant4 simulationsPonomarenko Daniil
02.12.2016
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In this presentation:● Current model description:
○ Physics list;○ Materials;○ Geometry and optical surfaces.
● Evaluation of:○ N photons in the SiPM per event;○ Cherenkov/scintillation photons contribution;○ Regions where photons have been created;○ Photons energy distributions.
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Statistics: 5000 events
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Model description (physics list)● Basic part is “QGSP_BERT_HP”
○ All electromagnetic processes are on boat
● Optical Physics ○ WLS
■ fWLSProcess->UseTimeProfile("delta");○ Cherenkov
■ fCerenkovProcess->SetMaxNumPhotonsPerStep(300);■ fCerenkovProcess->SetTrackSecondariesFirst(true);
○ Scintillation ■ fScintProcess->SetScintillationYieldFactor(1.);■ fScintProcess->SetTrackSecondariesFirst(true);■ fScintProcess->SetScintillationExcitationRatio(0.0);
○ Absorption○ Rayleigh scattering○ MieHG scattering○ Boundary
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MSPhysicsList.hh
MSOpticalPhysics.hh
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Model description (Material HBP)
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● Absorption is preliminary.○ Have correct distributions, but conversion
from % to length is needed.
● Is emission zero?
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Model description (Material EJ-309)
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● Chemical formula is wrong.○ Affects on Cherenkov process. ○ We have concentration of atoms per cm3.
● Scintillation from the EJ-309 pasport.○ Resolution scale?
● Absorption is preliminary. ● Briks constant is preliminary.
○ What is correct value?
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Model description (Optical surface)
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Plate / Air
EJ-309 / Plate
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Model description (SiPM)
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● Flat 40% quantum efficiency.○ f( ) is used since Slide 18
● Reflection 0%● SiPM now is a small black hole.
○ Stop and kills all particles.
y
z
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Existing prototype
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Electron 2.23 MeV
● HBP plate○ 8*cm x 25*mm x 1.96*mm
○ Polished
● SiPM x4○ 0.1*mm x 1.*mm x 1.*mm○ No reflection○ Quantum efficiency 40%
● HBP material (0.5*mm) in front of SiPM
● Channel x4○ 79*mm x 0.5*mm x 1.*mm
○ Ground
● Gun (CH#2) counting from 0
z
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Photon generation processes (all photons in all volume)
Peak at:● ~2000 scintillation photons● ~60 Cherenkov photons
Even
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Even
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Gun (-3,5cm, 0.5mm, 0.2cm+plate_widthZ/2.)
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Photon generation (all photons in all volume)
We can setup scintillation profile more precisely.
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Even
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at gunpoint
N photons in the SiPMs per event (ground channel)
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● Same behaviour as in the experiment.
● Does channel surface is really “ground”?
Gun (-3,5cm, 0.5mm, 0.2cm+plate_widthZ/2.)
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Is problem in channel surface?
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Electron 2.23 MeV
● HBP plate○ 8*cm x 25*mm x 1.96*mm
○ Polished
● SiPM x4○ 0.1*mm x 1.*mm x 1.*mm○ No reflection○ Quantum efficiency 40%
● HBP material (0.5*mm) in front of SiPM
● Channel x4○ 79*mm x 0.5*mm x 1.*mm
○ Ground
No photons are escape.
● Gun (CH#2) counting from 0
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Is problem in channel surface?
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Electron 2.23 MeV
● HBP plate○ 8*cm x 25*mm x 1.96*mm
○ Polished
● SiPM x4○ 0.1*mm x 1.*mm x 1.*mm○ No reflection○ Quantum efficiency 40%
● HBP material (0.5*mm) in front of SiPM
● Channel x4○ 79*mm x 0.5*mm x 1.*mm
○ Polished
That’s what we want!
● Gun (CH#2) counting from 0
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Even
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at gunpoint
N photons in the SiPMs (polished channel)
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● Needs to take in account real SiPM quantum efficiency.
● We can tune the “roughness” of the channels surfaces.
Gun (-3,5cm, 0.5mm, 0.5cm+plate_widthZ/2.)
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Per channel contribution
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● Highest contribution from the fiered channel (MCh_2).
● There are no photon generation in the support channels.
Even
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Even
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at gunpoint
“MCh_#” - tag for main channels
“SCh_#” - tag for support channels
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Per process contribution
● Cerenkov photons coming from the plate and EJ-309!
● Scintillation photons comes from the fiered channel.
Even
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ents
Even
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ents at gunpoint
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Energy spectrum
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Energy spectrum mostly same for all SiPMs.
Here photon detection efficiency was flat and equal
to 40%.
Let's use correct one.
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Energy spectrum as f( )
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Maximum of EJ-309 emission spectrum is in the region between 400-450 nm. So, there are no big changes
even for Cherenkov spectrum.
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Even
tsN photons in the SiPMs (polished channel, fQE( ))
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● Real SiPM quantum efficiency doesn’t change distributions
a lot.● We can tune the “roughness”
of the channel's surface.
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Let’s shoot between channels!
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Electron 2.23 MeV
● HBP plate○ 8*cm x 25*mm x 1.96*mm
○ Polished
● SiPM x4○ 0.1*mm x 1.*mm x 1.*mm○ No reflection○ Quantum efficiency 40%
● HBP material (0.5*mm) in front of SiPM
● Channel x4○ 79*mm x 0.5*mm x 1.*mm
○ Ground/Polished
● Gun (between CH#2 and CH#3) counting from 0
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Photon generation processes (all photons in all volume)
● Compare with Slide 9● Total ~= Cherenkov
Even
ts
Even
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Gun (-3,5cm, 1.mm, 0.2cm+plate_widthZ/2.)
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N photons in the SiPMs
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Even
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Ground channel
Even
ts
Polished channel
Gun (-3,5cm, 0.5mm, 0.2cm+plate_widthZ/2.), between MCh2 and MCh3
● Compare with Slide 11 and Slide 14
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There was ideal gun...
What if we’ll set particle gun distance to the plate surface
from 0.2 cm to 2 cm?
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Photon generation processes (all photons in all volume)
● Higher probability to get event, where e- generates only cherenkov in the plate.
● Compare with Slide 9.
Even
ts
Even
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Gun (-3,5cm, 0.5mm, 2cm+plate_widthZ/2.)
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N photons in the SiPMs
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Even
ts
Even
ts
Ground channel
Polished channel
Gun (-3,5cm, 0.5mm, 2cm+plate_widthZ/2.)
● Higher probability to have events, where e-
generates only cherenkov in the plate (passes near the scintillation channel).
● Compare with Slide 11 and Slide 14
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TODO list● Check effects from the aluminium collimator.
○ Set random E and angular e- distributions.■ Some examples for Sr90?
● Add additional volumes and parts:○ simple trigger under the plate (box of scintillator EJ-309) ○ simple aluminium boxes around for reflection simulation from the
supporting constructions and ect.● Paste plate over with black duct tape.● Something else?
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Back Up Slides
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Talks history● 11.11.16 - intro to the Geant4 toolkit and what we can do.
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https://gitlab.cern.ch/microscint-experts/G4MicroScint29
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EJ-309 channel solo in the air
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● Channel○ 8*cm x 0.5*mm x 1.*mm
○ Polished○ EJ-309 scintillator
● SiPM○ 0.1*mm x 1.*mm x 1.*mm○ No reflection○ Quantum efficiency 40%
Not centered (-0.01*mm shift)
y
z
● Gun (center of CH)○ Position (0,0,0.3*cm)○ Electron 2.23 MeV
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EJ-309 channel solo in the air
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Even
ts
Even
ts
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EJ-309 channel solo in the air
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EJ-309 channel solo in the airEv
ents