A scheme is proposed for detecting optical signals in which electrons bound in atoms, molecules, or ions are used as a sensitive element rather than free electrons, as in conventional detectors (photoelements, photomultipliers, etc.). It is shown that such a scheme has a high sensitivity and a reduced shot-noise level.
Detection of light is one of the most fundamental physical processes playing a very important role in both nature and technology. In nature, this process underlies vision, thus providing an opportunity to perceive the world around us. Numerous photodetectors in technology allow the quantification of the detection of optical signals, expanding the spectrum of detected radiation. The problem of detecting optical signals by optical methods themselves was first formulated apparently by Bloembergen [1]. However, this idea has not been adequately developed. In paper [2] it was shown that the signal-to-noise ratio could be improved by using nonlinear radiation detectors in which the signal transformation begins from an absorption transition. It was shown in papers [3] that photocounts appear in conventional photodetectors due to the strong Coulomb instability of a weak electron current produced in the detector by a signal being detected. This suggests that in detectors, instead of free electrons, the electrons that are bound in atoms, ions, or molecules can be used, where they are well stabilized by a strong Coulomb field of nuclei. Below a possible scheme for detecting weak optical signals by laser means is described. At present microcavities are created which can be used in the Bloembergen scheme, providing the passage from spontaneous to stimulated effect, thereby substantially improving the scheme.
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.
A system of unexcited three-level atoms, located in a nonresonant laser field, was examined. One of the excited levels in the system becomes populated under the influence of a weak optical signal, as a result of which the atoms resonate with the laser field. A consequence of this is intense scattering of the laser radiation and particularly excitation of the hitherto unexcited modes of the cavity in which the system of atoms is located. The system considered thus possesses states which are specially sensitive to external agencies and therefore sensitive optical-radiation detectors can be based on these states.