Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Philosophical Transactions of the Royal Society A Mathematical Physical and Engineering Sciences

Non-classicality and the effect of one photon

Christopher C. Gerry, Richard J. Birrittella, Paul M. Alsing, Jihane Mimih, P. L. Knight

Published Dec 24, 2024• 3 citations
Publisher

Abstract

The quantum interference effects of mixing the most non-classical states of light, number states, with the most classical-like of pure field states, the coherent state, are investigated. We demonstrate how the non-classicality of a single photon when mixed with a coherent field can transform the statistical properties of the output and further demonstrate that the entanglement of the output is independent of the coherent state amplitude.This article is part of the theme issue 'The quantum theory of light'.

DOI
10.1098/rsta.2023.0331

Related papers

Non-classical interference between independent sources

John G. Rarity, P. R. Tapster, R. Loudon

When a one-photon state is mixed with a (separate) weak coherent state at a beamsplitter the probability for detecting one photon in each beamsplitter output approaches zero due to destructive interference. We demonstrate this non-classical interference effect using pulse-gated single photons and weak mode-locked laser pulses.

arXiv:quant-ph/9702032•Journal of Optics B Quantum and Semiclassical Optics•Jun 30, 2005•119 citations

Entanglement and Superradiance in the Light of Non-Classical and Classical Photon Sources

Ralph Wiegner

In the present thesis we investigate spatial and temporal intensity correlations which are created by statistically independent or by entangled light sources. Even though this classification may appear quite technical, the diverseness of the statistical properties of the considered photon sources naturally brings into our focus two different lines of research. In the first part of this thesis we will quantitatively study the non-classical and potentially entangled character of light fields which originate from a variety of different statistically independent light sources. To this end quantum correlations between light fields are analyzed which either stem from non-classical single-photon emitters (like ensembles of uncorrelated atoms) or from a mixture of non-classical and classical photon sources (like lasers with uncorrelated fluctuating initial phase). In the second part of this thesis we study correlations between initially entangled lightsources, namely localized atoms which share an entangled state. In the course of the investigations we physically reinterpret in particular the so called superradiance effect in a quantum-path formalism: superradiance denotes an enhanced mean radiated intensity in a particular direction, i.e., a focussing of the photons scattered by an atomic gas. This effect is commonly explained by a successive synchronization of the dipole moments of all participating atoms leading to a photon emission predominantly in one direction. For more than 60 years this focussing has been physically interpreted as a cooperative effect depending on the dipole-dipole interaction between the atoms. In contrast, we will show that it is rather a quantum-interference effect which is caused by non-synchronized and potentially widely separated entangled atoms.

•Jan 1, 2012•0 citations

Quantum Theory of Interference Effects Produced by Independent Light Beams

L. Mandeļ

The conditions are examined under which interference effects should be observable in the superposition of two light beams derived from independent sources. The quantum-mechanical description of these effects differs from the classical description principally in that it is necessarily based on expectation values of the light intensity at one or more space-time points. It is shown that pure states of the radiation field which are not energy states give rise to interference effects, but in that case the two beams cannot meaningfully be described as statistically independent. For a realistic description mixed states have to be introduced, when the expectation value of the intensity gives no indication of interference effects. On the other hand, the intensity correlation at two space-time points is a periodic function of the separation of the points and indicates the presence of transient interference effects. The effects become readily observable only when the average photon occupation number of each cell of phase space is appreciably greater than 1, and this explains why laser beams were needed for the experimental observations. It is pointed out that, even in these experiments, each photon may be regarded as interfering only with itself.

Physical Review•Apr 6, 1964•54 citations

Non-Classical States of the Electromagnetic Field

L. Mandeļ

A number of general features of non-classical states of light are reviewed. The phenomena of photon antibunching and sub-Poissonian photon statistics are then treated in more detail, including the experimental observations. Quantum effects in spontaneous parametric down-conversion are discussed, and recent experiments dealing with the time intervals between down-converted photons, with the intensity dependence of the cross-correlation function, and with the detection of a localized one-photon state are described. Finally, some quantum effects in the interference of light are discussed.

Physica Scripta•Jan 1, 1986•282 citations

Photon interference and correlation effects produced by independent quantum sources

L. Mandeļ

Interference effects produced by independent quantum sources are investigated, when the state of the field is not describable as a simple mixture of coherent states. The results of classical and quantum-mechanical calculations are compared. Whereas correlation effects are predicted both classically and quantum mechanically when the sources have random phases, there are important differences when the number of atoms is small. In particular, when each source consists of just one atom, the joint probability of detecting two photons at two different points in the receiving plane is found to vanish when the distance between them is an odd number of half fringes. Finally it is shown that when the number of atoms of each source is subject to Poisson fluctuations, one recovers the solution given by classical optics for thermal light, no matter how weak the sources may be on the average.

Physical Review A•Aug 1, 1983•183 citations

Effects of photon statistics in wave mixing on a single qubit

W. V. Pogosov, A. Yu. Dmitriev, O. V. Astafiev

We theoretically consider wave mixing under the irradiation of a single qubit by two photon fields. The first signal is a classical monochromatic drive, while the second one is a nonclassical light. Particularly, we address two examples of a nonclassical light: (i) a broadband squeezed light and (ii) a periodically excited quantum superposition of Fock states with 0 and 1 photons. The mixing of classical and nonclassical photon fields gives rise to side peaks due to the elastic multiphoton scattering. We show that a side peaks structure is distinct from the situation when two classical fields are mixed. The most striking feature is that some peaks are absent. The analysis of peak amplitudes can be used to probe photon statistics in the nonclassical mode.

arXiv:2107.10769•Physical Review A•Aug 5, 2021•8 citations
The quantum interference effects of mixing the most non-classical states of light, number states, with the most classical-like of pure field states, the coherent state, are investigated. We demonstrate how the non-classicality of a single photon when mixed with a coherent field can transform the statistical properties of the output and further demonstrate that the entanglement of the output is independent of the coherent state amplitude.This article is part of the theme issue 'The quantum theory of light'.
In the present thesis we investigate spatial and temporal intensity correlations which are created by statistically independent or by entangled light sources. Even though this classification may appear quite technical, the diverseness of the statistical properties of the considered photon sources naturally brings into our focus two different lines of research. In the first part of this thesis we will quantitatively study the non-classical and potentially entangled character of light fields which originate from a variety of different statistically independent light sources. To this end quantum correlations between light fields are analyzed which either stem from non-classical single-photon emitters (like ensembles of uncorrelated atoms) or from a mixture of non-classical and classical photon sources (like lasers with uncorrelated fluctuating initial phase). In the second part of this thesis we study correlations between initially entangled lightsources, namely localized atoms which share an entangled state. In the course of the investigations we physically reinterpret in particular the so called superradiance effect in a quantum-path formalism: superradiance denotes an enhanced mean radiated intensity in a particular direction, i.e., a focussing of the photons scattered by an atomic gas. This effect is commonly explained by a successive synchronization of the dipole moments of all participating atoms leading to a photon emission predominantly in one direction. For more than 60 years this focussing has been physically interpreted as a cooperative effect depending on the dipole-dipole interaction between the atoms. In contrast, we will show that it is rather a quantum-interference effect which is caused by non-synchronized and potentially widely separated entangled atoms.
The conditions are examined under which interference effects should be observable in the superposition of two light beams derived from independent sources. The quantum-mechanical description of these effects differs from the classical description principally in that it is necessarily based on expectation values of the light intensity at one or more space-time points. It is shown that pure states of the radiation field which are not energy states give rise to interference effects, but in that case the two beams cannot meaningfully be described as statistically independent. For a realistic description mixed states have to be introduced, when the expectation value of the intensity gives no indication of interference effects. On the other hand, the intensity correlation at two space-time points is a periodic function of the separation of the points and indicates the presence of transient interference effects. The effects become readily observable only when the average photon occupation number of each cell of phase space is appreciably greater than 1, and this explains why laser beams were needed for the experimental observations. It is pointed out that, even in these experiments, each photon may be regarded as interfering only with itself.
A number of general features of non-classical states of light are reviewed. The phenomena of photon antibunching and sub-Poissonian photon statistics are then treated in more detail, including the experimental observations. Quantum effects in spontaneous parametric down-conversion are discussed, and recent experiments dealing with the time intervals between down-converted photons, with the intensity dependence of the cross-correlation function, and with the detection of a localized one-photon state are described. Finally, some quantum effects in the interference of light are discussed.
Interference effects produced by independent quantum sources are investigated, when the state of the field is not describable as a simple mixture of coherent states. The results of classical and quantum-mechanical calculations are compared. Whereas correlation effects are predicted both classically and quantum mechanically when the sources have random phases, there are important differences when the number of atoms is small. In particular, when each source consists of just one atom, the joint probability of detecting two photons at two different points in the receiving plane is found to vanish when the distance between them is an odd number of half fringes. Finally it is shown that when the number of atoms of each source is subject to Poisson fluctuations, one recovers the solution given by classical optics for thermal light, no matter how weak the sources may be on the average.
We theoretically consider wave mixing under the irradiation of a single qubit by two photon fields. The first signal is a classical monochromatic drive, while the second one is a nonclassical light. Particularly, we address two examples of a nonclassical light: (i) a broadband squeezed light and (ii) a periodically excited quantum superposition of Fock states with 0 and 1 photons. The mixing of classical and nonclassical photon fields gives rise to side peaks due to the elastic multiphoton scattering. We show that a side peaks structure is distinct from the situation when two classical fields are mixed. The most striking feature is that some peaks are absent. The analysis of peak amplitudes can be used to probe photon statistics in the nonclassical mode.