“…The background, b, can assume values at some E out that are even larger than the signal one wants to measure [9]. This is especially true at E out < 100 keV [13,38,42,52,66]. Background can arise from γs in γ-sensitive neutron detectors, beam contaminations (e.g., secondary-neutron group, protons or charged particles in the beam), wrap-around neutrons (dependent on spacing between source-neutron pulses), from pile-up of incident neutrons, room-return, random coincidences, α-particles from the sample, etc.…”