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Physics-Uspekhi

Photocounts and laser detection of weak optical signals

Vladimir P Bykov

Published May 31, 2005• 2 citations
Publisher

Abstract

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.

DOI
10.1070/pu2005v048n05abeh002103

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Photocounts and laser detection of weak optical signals

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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.
The physical nature of photocounts, i.e. current splashes in outer circuit of receiver at detection of weak optical signals is studied. It is shown, that the basic features of photocounts can be explained if to take into consideration the Coulomb instability of weak electronic flow, appearing in the detector under influence of accepted radiation. Many other particle mani- festations of electrons can be explained by this way. The laser scheme of detection of weak coherent radiation, essentially using laser radiation pumping, is offered. Thereat electrons, bound in atoms, ions or molecules, are used as an active element of device, but not free electrons, as it is usual. The stabilization of electrons by strong Coulomb field of the atom, ion or molecule nuclea does not allow to manifest their Coulomb instability. As a result photocounts, otherwise, Schottky noises are strongly put down at de- tection of weak signals. The detection of light is one of the most fundamental physical processes playing the important role as in nature, so in technique. For example, in na- ture this process provides a possibility of sight and, hence, to know the sur- rounding world. In technique the numerous photodetectors allow to make quantitative the process of detection of optical signals and to expand a spec- trum of accepted radiations.
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.
Modern concepts of the physical phenomenon described by the term “photon”, which was introduced simultaneously with the acceptance of quantum concepts in physics, are presented. Since that time, this term is a necessary component of each discussion about the physical meaning of quantum mechanics. These discussions are generally carried out within the concepts that are 50 or even 100 years old. At the same time, new fields of science have arisen and been developed in the last century: quantum mechanics and quantum electrodynamics, nonlinear optics, theory of dynamic chaos, etc. The experimental potential has been significantly increased, especially when highly coherent lasers were developed. As a result, the difficult problems of quantum mechanics have become aggravated and enriched. In this paper, we discuss two different approaches to gaining insight into the photon nature, which differ radically. An especially urgent problem is the difference in the estimates of the length of light states that are put into correspondence with photons: laser photons are many orders of magnitude longer than the photons put into correspondence with photocounts. Correspondingly, the spectrum of photocounts is many orders of magnitude wider than the lasing spectrum. The author believes that a photocount cannot be put into correspondence with a photon, because the former is a manifestation of the Coulomb nonlinearity of photodetector. The final solution of the question of the photon nature is expected to be obtained experimentally.
Any single on-off photocounter, which can only detect the presence or absence of photons without discriminating their number, is not capable of identifying nonclassical nature of light. This limitation arises because any photocounting statistics obtained with such a detector can be easily reproduced with coherent states of a light mode. We show that a simple modification of an on-off detector -- introducing controlled attenuation as a tunable setting -- enables such detectors to reveal nonclassical properties of radiation fields.