“…The direct methods used for measuring the macroscopic delayed-neutron characteristics from neutroninduced fission of heavy elements are based on irradiating the investigated sample by neutrons and subsequently measuring the appropriate delayed-neutron observables: the time dependence of delayed-neutron activities or the delayed-neutron energy spectrum. Neutron sources used for this purpose are mainly the neutron flux in nuclear reactors [207][208][209][210][211][212][213][214], critical assemblies [13,215,216], or electrostatic accelerator-based nuclear reactions: Li(p,n), T(p,n), T(d,n), D(d,n) [217][218][219][220][221][222][223]. All experimental methods are based on the assumption that the delayed-neutron activity arising from the irradiation of the fissionable sample can be represented by the linear superposition of the exponential decay modes, each with its own decay constant…”