The nature of photocounts arising in detectors exposed to highly coherent laser radiation is discussed. It is shown
that the spatial localization of a photon allowed in quantum
electrodynamics fails to account for the effect observed and
that the Coulomb instability of a low electron flux in a photodetector can be the explanation. With detectors utilizing non-free electrons, namely, electrons bound in atoms, ions,
molecules, etc., weak optical signals can be detected with laser
radiation without photocounts, in other words, at a suppressed
shot noise. A basic scheme for a laser detector using bound
electrons is suggested.