The Wide Field Imager (WFI) is one of the two focal plane instruments foreseen on board the future Advanced Telescope for High ENergy Astrophysics (ATHENA) planned by ESA. It is a DEPFET-based detector working in the energy range between 0.2 and 12 keV and covering a field-of-view of 40 arcmin diameter. A major advantage of a DEPFET active sensor is that each pixel has integrated its own amplifier, so that no charge transfer between pixels is needed. Therefore, it could be speculated that a DEPFET is less susceptible to radiation damage than a CCD, as lattice defects from nuclear scattering by particles in the space environment, mainly protons, would degrade the detector performance decreasing the charge transfer efficiency. However, any other degradation of the performance that might be caused by solar and cosmic protons must be quantified by dedicated irradiation tests in laboratory. For the non-X-ray-background (NXB) assessment conducted so far, we assumed that a bulk shielding providing a proton cut-off at ∼100 MeV was appropriate. The reasoning behind that is simply that below ∼100 MeV the non-ionising energy loss (NIEL) of protons in silicon increases with decreasing energy, while it tends to flatten above ∼100 MeV, as shown in Fig. 1. The drawback of a shielding surrounding the detector is the production of secondary emission in its environment from the interaction of omnidirectional energetic cosmic particles. This secondary emission is indeed mostly responsible for the generation of NXB. Therefore, it is crucial to conduct a trade-off analysis aimed to identify materials and geometries able to guarantee an adequate proton stopping power and, at the same time, minimize the induced NXB. In this paper, we review the assessment study conducted for the WFI in the former phase A. The new assessment has recently started after mission reformulation, and the results previously achieved in the framework of the WFI Background Working Group constitute the basis to continue the investigation, aimed at improving further the camera design and the methods of NXB reduction.
Orbital soft protons that reach the detector region of astronomical X-ray observatories can seriously degrade the instrumental performance. Firstly, they pose a non-reducible background component and, secondly, they might induce permanent damage in the sensors. A reliable performance estimation and risk assessment for new X-ray missions is only possible when radiation transport simulations are based on and validated against experimental scattering data.
In order to address this need for experimental data, we conducted measurement campaigns at various accelerator facilities and at different energies below 1 MeV in the past decade. Targets ranged from classic gold-coated nickel shells as used for the optics of XMM-Newton and eROSITA to the latest silicon pore optics (SPO) samples coated with iridium as foreseen for Athena.
The latest measurements with SPO samples were taken with a completely new experimental design at considerably lower energies than before, ranging from 20 keV to 50 keV, and with an MCP detector that features two dimensional position resolution. Therefore, this data is even more relevant for background studies and features a much finer angular coverage. Furthermore, the data yield hints that a significant fraction of scattered protons undergoes charge exchange and, thus, is not affected by a magnetic diverter.
In this contribution, we give an overview of the different proton experiments and their results and present our new low-energy setup together with some preliminary results.
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