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Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager
Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager
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Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager
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Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager
Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager

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Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager
Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager
Paper

Low temperature proton irradiation with DEPFETs for Athena's Wide Field Imager

2024
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Overview
The Wide Field Imager (WFI), one of two instruments on ESA's next large X-ray mission Athena, is designed for imaging spectroscopy of X-rays in the range of 0.2 to 15 keV with a large field of view and high count rate capability. The focal plane consists of back-illuminated DEPFET (Depleted p-channel field effect transistor) sensors that have a high radiation tolerance and provide a near Fano-limited energy resolution. To achieve this, a very low noise readout is required, about 3 electrons ENC at beginning of life is foreseen. This makes the device very susceptible to any radiation induced worsening of the readout noise. The main mechanism of degradation will be the increase of dark current due to displacement damage caused primarily by high energy protons. To study the expected performance degradation, a prototype detector module with fully representative pixel layout and fabrication technology was irradiated with 62.4 MeV protons at the accelerator facility MedAustron in Wiener Neustadt. A total dose equivalent to 3.3 \\(\\textstyle{10^{9}}\\) 10-MeV protons/\\(\\mathrm{cm^{2}}\\) was applied in two steps. During, in-between and after the irradiations the detector remained at the operating temperature of 213 K and was fully biased and operated. Data was recorded to analyze the signal of all incident particles. We report on the increase of dark current after the irradiation and present the current related damage rate at 213 K. The effect of low temperature annealing at 213 K , 236 K, 253 K, 273 K, and 289 K is presented.