“…calculated by the convolution of the ''chopper function'' C(t), which is given by the geometry of the experiment, the Maxwellian flight time distribution between chopper and crystal M 1 (t) and the flight time distribution between crystal and ion source M 2 (t) [16,58], shows a good correspondence to the experimental pulse without the necessity to introduce an additional surface function. This can be seen also when the above experimental pulse is compared with a pulse I 0 (t) with a definitely immeasurable time delay recorded at a high crystal temperature.…”