Baseline drift is a change with time in the non-signal level of a measurement readout. For a photodetector, write the measured electric current as
where is the changing baseline and represents fluctuations around that level. Detector baseline subtraction using one fixed value can leave a time-dependent residual even when it correctly removes the initial offset.
If a detection time gate uses a constant baseline estimate , its baseline contribution to the charge error is
A proposed control brackets the signal in time with signal-absent measurements. For baseline values at equally spaced times and , estimate the central baseline by
This reproduces the central value exactly for a baseline linear in time. If that linearity holds across a gate centred at , its integrated baseline is also exactly .
For an original example, choose baseline readings and before and after the signal, with linear drift between them. The central baseline is . A centred gate of width contains of baseline charge. Subtracting only the earlier reading removes and leaves a false positive contribution of .
Bracketing is not an unconditional drift correction. For , the two-point estimate of the central level is , so curvature introduces an error. Random baseline-readout errors also contribute measurement uncertainty. Taking reference readings close to the signal limits some drift effects, but does not remove a source-correlated artifact or compensate for all changes in the measurement conditions.
A real gated-integrator implementation alternates signal-present and signal-absent triggers and reverses the latter contribution before averaging. The manufacturer's stated purpose is active baseline subtraction.[ref] Its effectiveness depends on whether the signal-absent readings represent the baseline during the signal. Plotting those readings against time, as well as reporting their average, can distinguish a changing zero from uncorrelated measurement noise.

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