HIGHLIGHTS
SUMMARY
Low Temperature Detectors (LTDs) are one of the most suitable detectors for experiments demanding a very high energy resolution for energies up to MeV. Both the two filtering techniques require that the processed pulses are acquired in record windows whose length is determined by the detector characteristic time profile in such a way that, within their record windows, pulses can fully recover. The standard filter (H ) is derived, as, by maximizing the signal-to-noise ratio (ρ) of the processed pulse: ∞ iωtmax dω 2 -∞ H (iω)S(ω)e 2 ∞ ρ ∝ 2 -∞ N (ω)|H (iω)| d . . .
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