Advacam, Prague, Czech Republic. Nuclear Physics Institute, Czech Academy of Sciences, Prague, Czech Republic
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1 Resolving Power of Pixel Detector Timepix for Wide-Range Electron, Proton and Ion Detection Carlos Granja 1,2, Jan Jakubek 1, M. Sommer 2, O. Ploc 2 D. Chvatil 2, P. Krist 2, V. Zach 2, J. Stursa 2, V. Olsansky 2, T. Matlocha 2 Satoshi Kodaira 3, Maria Martiskova 4 1 Advacam, Prague, Czech Republic 2 Nuclear Physics Institute, Czech Academy of Sciences, Prague, Czech Republic 3 National Institute of Radiological Sciences NIRS, HIMAC, Chiba, Japan 4 German Cancer Research Center DKFZ, HIT, Heidelberg, Germany ADVACAM IBWS Workshop, Karlovy Vary, Carlos Granja, Advacam
2 Resolving Power of Pixel Detector Timepix for Wide-Range Electron, Proton and Ion Detection Motivation + Goals + Challenges + Status Timepix detectors being used to detect and characterize mixed radiation fields such as those found in outer space, near Earth, deep space, upper atmosphere, ion beam radiotherapy Response/calibration needed Particular value by the detector resolving power in terms of particle-type, spectral- (energy loss) and direction/tracking. The challenge is to provide resolving power with high sensitivity and wide dynamic range in terms of particle types, stopping power and direction with a single compact device Experimental study, tests and calibration of a single Timepix (300 µm Silicon): evaluation of detection response in defined fields of various radiations (electrons, protons, ions) in wide range of fluxes, energies and incident directions Use of Timepix in space Applications: Radiation dosimetry (quantum imaging dosimetry, LET spectra, on line response) Radiation monitoring (miniaturization, integration) Characterization of radiation fields (photon counting, per-px spectrometry, wide range) Science/research Space weather Focal plane X-ray imager Micro-tracker/directional camera Gamma-ray Compton camera Neutron detection Deployments of Timepix in space/orbit Applications: NASA - ISS-REM-TPX 2012, IEAP CTU ESA - Proba-V/SATRAM-TPX spacecraft payload 2013, IEAP CTU NASA BIRD-TPX Orion EFT NASA ISS HERA-TPX 2016 NASA ISS EPT TPX telescope 2017 Science/research CZ - X-ray focal plane detector/x-ray telescope on board Czech VZLUSAT-1 cubesat 2016, VZLU/RIGAKU/FEL- IEAP CTU Educational GB TechDemoSat1 ADVACAM IBWS Workshop, Karlovy Vary, Carlos Granja, Advacam 4/19/2018 2
3 A. Chilingarian, Yerevan Phys. Inst./CRREAT Prof. G. Reitz, O. Ploc, C. Granja*, et al., CRREAT-UJF Research area/subjects Atmospheric phenomena & ionizing radiation Sources, variation, characterization of primary & secondary cosmic rays Radiation instrumentation/methodology Experiments/projects/deployment Atmospheric balloons UAV/drones, remote/terrain vehicles DLR aircraft flights Dosimetry experiments on board ISS Satellite borne payloads/experiments Return satellite capsule High-altitude radiation stations Biological satellite BION-M1, return capsule LEO orbit, IBMP RAS Moscow 3
4 Cyklotron accelerator Electron microtron accelerator NPI-CAS, Rez near Prague ADVACAM Oy Event name Presentation title 4/19/ Electron Microtron Accelerator
5 6-35 MeV protons minipix LIULIN Detectors/setup Cyklotron (UJF AV/CANAM) 2x stack TPX telescope WidePIX3D: 4x TPX telescope Directional cosmic ray/muon detector WidePIX3D: 4x TPX telescope Electron Microtron TEPC 7-25 MeV electrons WidePIX3D: 4x TPX telescope Detectors/setup minipix CdTe modupix LIULIN minipix Electron Microtron Accelerator (UJF AV) 60 Co/ 137 Cs irradiator (ODZ-UJF AV) 16 May
6 WidePIX3D Highly integrated (contact geometry) WidePIX3D 4xTPX tracker Physics/radiation research at accelerator research facilities 4x TPX Electron Microtron accelerator Nuclear Physics Institute, Prague, Czech Academy of Sciences Electron beam Microtron Palm-top miniaturized particle telescope Lead shielding (radiation, EMI) Electron beam Mono-energetic electrons 7-25 MeV - LEO orbit - radiation belts Electron beam NPI-CAS, Rez near Prague Electron Microtron Accelerator 25 Aprill
7 600 ns Y-position [pixels] y-axis 3D charged particle tracking Widepix3D 4xTimepix miniaturized Tracker TPX 3 TPX 4 TPX 1 TPX 2 Spatial + Time correlated detection Color value = Time of interaction 0 0 x-axis MeV electrons (NPI Microtron) 512 Color value = pixel layer ordering TPX 3 TPX TPX 1 TPX 2 1 TPX 3 TPX TPX 1 TPX X-position [pixels] 250 7
8 protons: varying E + unfiltered data Medium-energy protons Cyclotron accelerator, NPI- CAS, Rez near Prague Space weather Solar wind, plasma Ionizing radiation Magnetic field/magnetosphere Timepix/miniPIX Timepix + HIMAC: 4He beam + background Liulin Timepix/miniPIX Proton beam Timepix chip Timepix/miniPIX Incident beam 8
9 Quantum imaging detection, spectrometry, tracking Energetic charged particles: relativistic ions, secondary reaction/fragmentation products 490 MeV/u 28 Al ions 85 MeV/u 28 Al ions & secondary reaction products Relativistic ions HIMAC ion synchrotron accelerator, NIRS, Chiba, Japan Timepix/miniPIX Medipix spin-off Energetic (penetrating) charged particles: Deposited energy Position of interaction de/dx LET, stopping power Direction (limited angular resolution) Micro-scale particle tracking + high-resolution pattern recognition of single charged particles C. Granja, CRREAT/NPI-CAS, Prague
10 ADVACAM Oy Event name Presentation title 4/19/
11 Single particle detection and spectrometry Cluster analysis + Pattern recognition: Heavy charged particles: protons, ions C. Granja, IEAP CTU Prague 2014 Unwanted events, background, X- rays, scattered particles Low-energy protons VdG accelerator, IEAP CTU Prague 200 kev protons 1.6 MeV protons Charged particles: Deposited energy Position of interaction Pixelated cluster morphology / pattern recognition analysis: Shape, cluster area: A Summed energy, cluster volume: E Largest pixel energy, cluster height: H E = 24.4 MeV A = 137 px H = 921 kev E = 30.7 MeV A = 147 px H = 2.6 MeV E = 23.8 MeV A = 142 px H = 861 kev Light ions /products from nuclear reaction 24 MeV Li ions on Be target 9 Be( 7 Li, 8 Li) E = 5.0 MeV A = 52 px H = 1.3 MeV E = 2.9MeV A = 62 px H = 116 kev E = 10.9 MeV A = 392 px H = 332 kev E = 11.8 MeV A = 110 px H = 380 kev 23.8 MeV 5.6 MeV H 3.5 MeV A E E = 5.6 MeV A = 71 px H = 362 kev E = 9.5MeV A = 6 px H = 2.2 MeV E = 20.8 MeV A = 141 px H = 525 kev E = 3.5MeV A = 66 px H = 118 kev 16 May MeV 11
12 Detection Response of Timepix: Micro-scale tracks Pattern recognition + cluster analysis parameters + (physics) degrees of freedom Energetic (penetrating) charged particles: Deposited energy Position of interaction de/dx LET, stopping power Direction (ang res 5-10⁰) Pattern recognition and micro-scale tracking of single charged particles Degrees of freedom: Particle type Particle energy, stopping power Particle direction = Azimuth angle b = Elevation angle ADVACAM IBWS Workshop, Karlovy Vary, Carlos Granja, Advacam 4/19/
13 Response of cluster analysis parameters: Varying ion energy 4 He beam: MeV/u: all particles Area [# px] 144 MeV/ u SINGLE-PARAMETER ANALYSIS 61 MeV/ u 48 MeV/ u 31 MeV/ u 21 MeV/ u Energy (volume) [kev] Height [kev] Track length [um] LET [kev/um] ADVACAM Oy Event name Presentation title 4/19/
14 Response of cluster analysis parameters: Varying ion energy 4 He beam: MeV/u: all particles SINGLE-PARAMETER ANALYSIS Area [# px] Energy (volume) [kev] Height [kev] Track length [um] LET [kev/um] ADVACAM IBWS Workshop, Karlovy Vary, Carlos Granja, Advacam 4/19/
15 TWO-PARAMETER ANALYSIS Electrons, protons, ions: all particles 4 energies 2 energies protons bckg/unwan ted events bckg/unwan ted events ADVACAM Oy Event name Presentation title 4/19/
16 TWO-PARAMETER ANALYSIS Electrons, protons, ions: all particles 25 MeV p electrons 490 MeV 28Si 48 MeV p MeV 12C ADVACAM IBWS ADVACAM Workshop, Oy Karlovy Event Vary, name Presentation Carlos title Granja, Advacam 4/19/
17 Timepix: detection response/resolving power Particle types/species, spectral range, direction Classification of radiation events in the Timepix detector. The proposed event types are listed with the proposed range of selected values of cluster parameters. # Event CAP 1 CAP 2 CAP 3 1 X-rays, L.E. e s, P. energetic e s, μ s H < L.E. p s 140 < H < L.E. light ions 800 < H < L.E. heavy ions 2500 < H 5 E. e s, μ s 0 < LET < E. p s 1.85 < LET < E. light ions 4.0 < LET < 42 8 E. heavy ions, HZE 42 < LET L.E. = low energy, E = energetic, P. = Perpendicular, CAP = cluster analysis parameter A = area [# px], R = roundness [a.u.], H = height [kev/px], LET = linear energy transfer [kev/μm] e = electrons, μ = muons, p = protons ADVACAM IBWS Workshop, Karlovy Vary, Carlos Granja, Advacam 4/19/
18 composite detector C. Granja, L. Mikulickova, V. Marsikova, A. Inneman, D. Doubravova, R. Pavlica, A. Marek, et al. Composite materials for radiation shielding Evaluation + proton beam + mixed field characterization secondary radiation Set of various composite materials Proton/light ion cyclotron at NPI Rez F G proton beam B C proton beam B C F G proton beam Nuclear Physics Institute of the CAS public research institution CRREAT, ODZ-UJF-CAS Carlos Granja 18
19 acq t = 100 ms Monoenergetic, size/parallel beam proton field at 3 energies: 4 samples + open beam open beam sample A sample C sample G sample H 30.9 MeV 19.6 MeV 7.9 MeV 19
20 sample C open beam C. Granja, L. Mikulickova, V. Marsikova, A. Inneman, D. Doubravova, R. Pavlica, A. Marek, et al. Composite materials for radiation shielding Particle flux and spectral (energy loss) characterization Count rate [#/s]: 30.9 MeV protons Count rate [#/s]: 19.6 MeV protons Count rate [#/s]: 7.9 MeV protons A B C D E F G H K open 50 0 A B C D E F G H K open A B C D E F G H K open all p non-p all p non-p all p non-p 20
21 Back-up slides ADVACAM Oy Event name Presentation title 4/19/
22 ADVACAM Oy Event name Presentation title 4/19/
23 ADVACAM Timepix ADVACAM in Space, Oy Event CERN, name Presentation Carlos title Granja, Advacam 4/19/
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