Post on 18-Jan-2016
transcript
MICOSa CHERNE collaboration
in applied research involving industry
François Tondeur, Lara Marwaha, Isabelle Gerardy, Jonathan Baré
ISIB José Rodenas, Sergio Gallardo
UPV
MICOSminiaturisation of the Compton
spectrometer
• PRINCIPLE
Measurement on the scattered X-ray beam to avoid detector saturation
The Compton spectrometer in the 1990’s
• Matscheko et al RTI Electronics
A big, heavy device adapted to a Ge detector
The Compton spectrometerin CHERNE
• UP Valencia: Gallardo, Rodenas, Verdu Monte Carlo simulation of the Compton scattering technique applied to characterize diagnostic X-ray spectra
• U. Bologna: Fernandez, Scot, Baré et alReconstruction of the X-ray tube spectrum from a scattering measurement
• ISIB Bruxelles: Marwaha, Tondeur et alpresent work
MICOS
• Development of a small portable device for routine spectrometric controls of X-
ray generators• 4-year FIRST project supported by the
Walloon region 2008-2012• Industrial cooperation with Balteau
NDT and Canberra Benelux• Academic collaboration with UP
Valencia
MICOS partnership
• Project coordinated by ISIB, and executed at ISIB lab of nuclear and radiation physicsresearch fellow: Lara Marwaha (ex-FHA)
• UPV: training of the research fellow to MC simulation and to the « old » spectrometer
• Balteau: manufacturer of the shielding + sales in the industrial sector
• Canberra: provided detectors for the project + sales in the medical sector
MICOS main steps
• Design of a simplified shielding
• Tests of detectors and choice of a detector
• MC simulation and validation
• Choice of the methodology for unfolding
Shielding design• 3 options according
to energy : maximum 150, 300 or 450 keV
• Design with MC simulation
• Steel/lead/copper for 150 kV and 300 kV
• 450 kV: W cover above the 300 kV device
Choice of the detector
• Limited choice of « pen-type » detectors diam.<20 mm, reasonable cost
• Tested : CZT, CdTe, NaI• CZT- CdTe: not easy to simulate with MC
(problems with dead layers, variability from one detector to another, response depending on electronics settings…)
• Choice: NaI – easy to simulate with MC
Monte Carlo simulation• Geometrical model validated with
radioactive sources: 241Am, 109Cd, 57Co, 137Cs
thickness of front
window fitted to
experimental data
• Response matrix of 150 keV prototype calculated with 1 keV interval
Deconvolution• A specific algorithm similar to GRAVEL
gives good results in few iterationssensitive to good energy calibration
MICOS going on
• 300/450 keV prototype soon manufacturedsimulation-validation-unfolding-testing
• Back to CZT/CdTe improve the geometrical model and the
simulation of the response
• Students from CHERNE welcome for a master thesis
Thank you