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. 2021 Oct 28;217(8):80. doi: 10.1007/s11214-021-00855-2

Fig. 12.

Fig. 12

(a) Energy deposit in a single MED pixel as a function of incident electron energy, calculated with the full Geant4 model. The main channel boundaries (cuts on the energy deposit) are labeled, along with non-ideal contributions to the energy deposit (bounce, collimator, pixel edges – see text). (b) The response of the individual PHA channels that constitute the main channel delineated in panel (a), showing the maximum energy resolution and separation achievable by the sensor