Radiation Test Challenges with High-Energy Electrons

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Radiation Test Challenges with High-Energy Electrons CALIFES Workshop 2016 10-12 October, CERN Radiation Tests Session Rubén García Alía (ruben.garcia.alia@cern.ch) Markus Brugger Roberto Corsini Wilfrid Farabolini Maris Tali 10th October 2016

Radiation Test Challenges with High-Energy Electrons Outline Introduction JUICE mission and Jovian environment Electron induced radiation effects: DD and TID Electron facility overview VESPER test requests and possible HEP applications Summary 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Outline Introduction JUICE mission and Jovian environment Electron induced radiation effects: DD and TID Electron facility overview VESPER test requests and possible HEP applications Summary 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Context and Overview CERN/ESA meeting in December 2014 to discuss about the potential use of CALIFES for electron radiation testing applications Since then: 2015: proof of concept through first tests with well-known detectors 2016: improvements in beam line and instrumentation for dedicated dosimetry Further tests, both internal and external 2014 2016 10th October 2016 Radiation Test Challenges with High-Energy Electrons

(High-energy) electrons at NSREC 2016 International conference on radiation effects on electronics Increasing interest in the community, mainly driven by the future Jovian missions Examples of presented studies on electron effects: “Gamma and Electron NIEL Dependence of Irradiated GaAs” M. El Allam et al. (PC-2) “Low-Energy Electron Irradiation of NAND Flash Memories” M. J. Gadlage et al. (D-2) “Heavy Ion, Proton and Electron Single-Event Effect Measurements of a Commercial Samsung NAND Flash Memory” F. Irom et al (W-44) “Shielding a MCP Detector for a Spaceborne Mass Spectrometer Against the Harsh Jupiter Radiation Environment” M. Tujet et al (J-3) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Outline Introduction JUICE mission and Jovian environment Electron induced radiation effects: DD and TID Electron facility overview VESPER test requests and possible HEP applications Summary 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons JUICE ESA Mission JUpiter ICy moons Explorer: first L-class launch slot in ESA’s Comic Vision Programme, foreseen for 2022 Objective: investigation of Jupiter and its icy moons, Callisto, Ganymede and Europa Mission overview: Launch in June 2022 with Ariane 5 Interplanetary transfer about 7.5 years Scientific measurements around Europa (35 days), Jupiter high latitude phase (6 months), eccentric orbit around Ganymede (4 months), circular phase at 500 km (5 months) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Jovian Radiation Environment Jupiter is by far the strongest magnetic trap in the solar system >5 MeV electron fluxes at Jupiter: 1-2 orders of magnitude higher than at other planets E. Roussos, RADECS 2016 Topical Day 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Outline Introduction JUICE mission and Jovian environment Electron induced radiation effects: DD and TID Electron facility overview VESPER test requests and possible HEP applications Summary 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation effects on electronics next presentation this presentation Displacement Damage Single Event Effects Total Ionizing Dose 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Displacement Damage (DD) Semiconductor materials (Si, GaAs…) are usually crystalline and interactions of energetic particles with it can lead to a disruption in the lattice, degrading the electrical performances of the device 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons DD by electrons NIEL scaling hypothesis: proportionality between Non Ionizing Energy Loss and resulting damage effects How well does this hold for high energy electrons and state-of-the-art technologies? C. Poivey and G. Hopkinson, “Displacement Damage Mechanisms and Effects” , presentation at EPFL Space Center (2009) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Electron hardness factor For silicon, relationship between displacement damage cross section and NIEL is 100 MeVmb = 2.144 keVcm2/g Hardness factor k = Dparticle(E)/Dneutron(1 MeV), where Dneutron(1 MeV) = 95 MeVmb 10th October 2016 Radiation Test Challenges with High-Energy Electrons

DD in Jovian environment Trapped electrons in the Jovian environment will dominate the overall mission displacement damage E.g. for 20 mm Al shielding, the 10 MeV proton equivalent fluence from electrons for DD is ~6·1011 cm-2 and clearly dominates the total contribution JUICE environment specification, JS-14-09 (2015) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

TID in Jovian environment Trapped electrons are expected to clearly dominate the TID Unlike in the case of the Earth trapped electron belts, due to the larger energies, shielding is less efficient Almost 1 kGy for 20 mm Al shielding (design baseline) JUICE environment specification, JS-14-09 (2015) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

60Co TID tests for EEE components in Jupiter 60Co is traditionally used to characterize electronic component TID performance In general, it represents a worst-case condition with respect to radiation environment due to the larger fraction of unrecombined holes/electrons Input from A. Zadeh (TEC-QEC, ESA) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

60Co TID tests for EEE components in Jupiter For the LM124, the data indicates increased electron irradiation induced parameter degradation compared to 60Co tests. Electron 12MeV at ~6.7rad/s. HSM (Portugal) Electron >10MeV at RADEF (Finland). 60Co gamma at ~6.7rad/s. CTN (Portugal) 60Co gamma at ~0.08rad/s. ESTEC (The Netherlands) Input from A. Zadeh (TEC-QEC, ESA) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Outline Introduction JUICE mission and Jovian environment Electron induced radiation effects: DD and TID Electron facility overview VESPER test requests and possible HEP applications Summary 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Facilities: CLINAC@RADEF Example of medical linac accelerator CLINAC electron accelerator installed at RADEF facility Aimed to be used for irradiation studies of semiconductor materials and devices Extraction energies from 6 to 20 MeV Maximum dose rate: 600 Gy/h Pulse distance of 5.5 ms (RF frequency of 180 Hz), pulse width of 5 um Dosimetry: ionization chamber, 2D array detector (PTW Octavius) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Facilities: piM1 beam line@PSI Secondary particles produced on thick carbon target from energetic proton beam Selection of particle charge/momentum and guides to test areas Electron flux/energies ranging from 1.5·103 e/cm2/s at 20 MeV to 2·106 e/cm2/s at 345 MeV Beam contamination with heavier particles (protons, pions) above 115 MeV/c 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Facilities: VESPER@CALIFES Developments in beam line, optics, instrumentation and dosimetry for radiation testing 200 MeV electrons, with a large range of possible intensities First external test campaign: Flash memories from University of Padova/ESA More information in next presentation (“VESPER status and outlook”, Maris Tali) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Outline Introduction JUICE mission and Jovian environment Electron induced radiation effects: DD and TID Electron facility overview VESPER test requests and possible HEP applications Summary 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Example of test request for VESPER SEE tests from ESA and CNES (e.g. deep sub-micron CMOS technology) Study the degradation of triple junction solar cells for space applications Electron energy between 75 and 200 MeV Fluence between 1012 and 1015 e/cm2 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Possible interest from HEP community Electronics for detectors: possible use of high intensity electron beam for high dose applications (though effects such as e.g. high dose rate would need to be analysed) Electromagnetic calorimetry: radiation effects in scintillating materials Testing and calibrating dosimeter samples and radiation monitors Input from F. Ravotti (CERN EP-DT-DD) 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Outline Introduction JUICE mission and Jovian environment Electron induced radiation effects: DD and TID Electron facility overview VESPER test requests and possible HEP applications Summary 10th October 2016 Radiation Test Challenges with High-Energy Electrons

Radiation Test Challenges with High-Energy Electrons Summary Trapped electrons will dominate the DD and TID in the Jovian environment Therefore, it is important to evaluate whether standard test approaches (e.g. protons for DD, 60Co for TID) are representative of the high energy electron induced damage in state-of-the-art technologies The availability of a 200 MeV electron radiation facility is a key asset for performing such a study, as medical linacs used for radiation effects testing typically have energies one order of magnitude below 10th October 2016 Radiation Test Challenges with High-Energy Electrons