e-LINAC Beam Facility Characterization For Its Use For Space - - PowerPoint PPT Presentation

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e-LINAC Beam Facility Characterization For Its Use For Space - - PowerPoint PPT Presentation

e-LINAC Beam Facility Characterization For Its Use For Space Detectors Performance Studies E. Pilicer (INFN-Perugia, Italy) B. Alpat, M. Menichelli, L. Servoli (INFN-Perugia, Italy) D. Caraffini, F. Renzi (Maprad-Perugia, Italy) M. Italiani,


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SLIDE 1

7th Geant4 Space Users Workshop, 18-20 August, 2010

e-LINAC Beam Facility Characterization For Its Use For Space Detectors Performance Studies

  • E. Pilicer (INFN-Perugia, Italy)
  • B. Alpat, M. Menichelli, L. Servoli (INFN-Perugia, Italy)
  • D. Caraffini, F. Renzi (Maprad-Perugia, Italy)
  • M. Italiani, E. Buono, M. Casale, M. Muti (Terni Hospital, Italy)
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SLIDE 2

7th Geant4 Space Users Workshop, 18-20 August, 2010

  • Motivation
  • Beam & Dose profiles
  • Available energy & Flux @ detector surface
  • Conclusions

Outline

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SLIDE 3

7th Geant4 Space Users Workshop, 18-20 August, 2010

The goal is to use of AOT’s e-Linac for Space Detectors‘ Performance testing To do this we need full Monte Carlo (MC) description of irradiation system as well as a Beam Monitoring Detector system (BMDS)

Motivation

Flux

Provided by Terni Hospital Provided by Maprad

MC (Geant4) Beam Profile Energy Fluence Advanced Markus Chamber Beam Profile Dose Profile Double Sided Silicon Detector Beam Profile Charge Flux Plastic Scintillator+SiPM Energy Data (BMDS)

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SLIDE 4

7th Geant4 Space Users Workshop, 18-20 August, 2010

Source to Surface Distance SSD (100 - 200 cm) Advanced Markus Chamber

PTW-34045

Linac head DUT Applicator shield

Entrance window thickness 0.03 mm Sensitive volume 20 mm3

e-

Simulated Accelerator Head

Terni Hospital e-Linac

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SLIDE 5

7th Geant4 Space Users Workshop, 18-20 August, 2010

Physics Lists & Applied Cuts

Two kinds of physics list classes are available; G4VUserPhysicsList for relatively simple physics lists G4VModularPhysicsList for detailed physics lists Recommended Built-in Physics used G4EmStandardPhysics_option1 G4EmStandardPhysics_option2 G4EmStandardPhysics_option3 G4EmPenelopePhysics G4EmLivermorePhysic Particle production thresholds (Cuts) = 0.1 and 1 mm StepSize (Steps) = 1 and 100 mm Generated primaries → mono-energetic electrons with no beam divergency (energy range 4-20 MeV)

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/process/eLoss/binsDEDX 480 /process/eLoss/binsLambda 480

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SLIDE 6

7th Geant4 Space Users Workshop, 18-20 August, 2010

Beam Profiles

Beam profile width from FWHM

Sample plots @ 100 cm with option3 15 MeV (mono-choromatic, no beam divergence)

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SLIDE 7

7th Geant4 Space Users Workshop, 18-20 August, 2010

Beam Profile Widths

Primary: mono-energetic, 6 MeV, no beam divergence

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SLIDE 8

7th Geant4 Space Users Workshop, 18-20 August, 2010

Beam Profile Widths

Primary: mono-energetic, 15 MeV, no beam divergence

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SLIDE 9

7th Geant4 Space Users Workshop, 18-20 August, 2010

Beam Profile Widths

Beam Profile Width Percent Deviation = ((MC-Data)/Data)x100 @ 6 MeV e-Beam Deviation starts after 130 cm for all Physics lists @ 15 MeV e-Beam G4EmPenelope better agreement

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SLIDE 10

7th Geant4 Space Users Workshop, 18-20 August, 2010

Primary: mono-energetic, 6 MeV, no beam divergence

Dose & Energy

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SLIDE 11

7th Geant4 Space Users Workshop, 18-20 August, 2010

Dose & Energy

Primary: mono-energetic, 15 MeV, no beam divergence

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SLIDE 12

7th Geant4 Space Users Workshop, 18-20 August, 2010

Kinetic energy @ SSD=130cm For cuts=0.1mm and step=1mm For primaries; Fit Gauss & Sigma

Available Energy @ Detector Surface

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SLIDE 13

7th Geant4 Space Users Workshop, 18-20 August, 2010

Available Energy @ Detector Surface

Kinetic energy distributions for 15 MeV primary

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SLIDE 14

7th Geant4 Space Users Workshop, 18-20 August, 2010

Available Energy @ Detector Surface

Fluctuations in kinetic energy for 15 MeV primary

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SLIDE 15

7th Geant4 Space Users Workshop, 18-20 August, 2010

Steps to obtain flux

  • Convert Energy [MeV] to Dose [Gy]
  • Conversion factor [CF] = DoseGeant4 / DoseExperimental
  • Flux = CF x DetectorSurfaceHits / DetectorSurface / Time

15 MeV 6 MeV

Flux @ Detector Surface

[particles] / [cm2] / [second]

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SLIDE 16

7th Geant4 Space Users Workshop, 18-20 August, 2010

Flux @ Detector Surface

From fits one can estimate @ a given distance;

  • Flux
  • Kinetic energy
  • σ in Kinetic energy

cuts=0.1mm step=1mm

~50x103 particle/cm2/sec @ 300cm

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SLIDE 17

7th Geant4 Space Users Workshop, 18-20 August, 2010

Double Sided Silicon Detector (DSSD)

Double sided silicon detector

  • 35x35 mm2 and 1.5 mm thick
  • 64 channel on p and n sides with

readout pitch of 500 µm Sr-90 source Ar-20MeV/n

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SLIDE 18

7th Geant4 Space Users Workshop, 18-20 August, 2010

  • Beam & Dose profiles from Advanced Markus Chamber used

in AOT e-Linac is compared with full Geant4 simulations

  • Measured Beam & Dose profiles are in better agreement with MC

by using cuts=0.1 and step=1mm with G4EmPenelopePhysics

  • To reach the same number of simulated events longer computation

time is required for G4EmPenelopePhysics and G4EmLivermorePhysics

  • In e-Linac facility we can obtain uniform energy distributions at

almost all distances and deliver to DUT surface electron fluxes (from few particles/cm2/sec at about 550 cm up to 106 particles/cm2/sec at 100 cm)

Conclusions 1/2

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SLIDE 19

7th Geant4 Space Users Workshop, 18-20 August, 2010

  • The distances larger than 200 cm requires to turn e-Linac head

for horizontal irradiation (horizontally max available working distance is about 700 cm)

  • In addition to instrumentation available at AOT we plan to develop

The DSSD and Plastic Scintillator+SiPM detector developments for further comparison and validation studies

  • e-Linac at Terni Hospital is a promising site for detector

performance testing with electrons of energies ranging from 4-to-20 MeV

Conclusions 2/2

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