In a programmable two-slit setup with scanned point source and fixed detector, source-plane nulls defined by vanishing coherent transfer amplitude yield a null-mask loss that obeys the visibility-distinguishability relation, realizing reciprocal detector-conditioned complementarity.
Wen, Hybrid second-order coherence in a time- reversed Young’s experiment (2026)
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Detector-Conditioned Source-Space Nulls and Null-Mask Loss in a Programmable Two-Slit Interferometer
In a programmable two-slit setup with scanned point source and fixed detector, source-plane nulls defined by vanishing coherent transfer amplitude yield a null-mask loss that obeys the visibility-distinguishability relation, realizing reciprocal detector-conditioned complementarity.