Cited by 908Semiconductor Quantum Structures and DevicesQuantum optics and atomic interactionsStrong Light-Matter Interactions

The DOI matches its Crossref record; 213 of the 213 references it cites were found in a registry or an index; none of the 155 sources its claims cite is checked for support yet.

Single-photon sources

Open access
Lounis, Brahim, Orrit, Michel·2005·Reports on Progress in Physics

Abstract

The concept of the photon , central to Einstein's explanation of the photoelectric effect, is exactly 100 years old. Yet, while photons have been detected individually for more than 50 years, devices producing individual photons on demand have only appeared in the last few years. New concepts for single-photon sources, or 'photon guns', have originated from recent progress in the optical detection, characterization and manipulation of single quantum objects. Single emitters usually deliver photons one at a time. This so-called antibunching of emitted photons can arise from various mechanisms, but ensures that the probability of obtaining two or more photons at the same time remains negligible. We briefly recall basic concepts in quantum optics and discuss potential applications of single-photon states to optical processing of quantum information: cryptography, computing and communication. A photon gun's properties are significantly improved by coupling it to a resonant cavity mode, either in the Purcell or strong-coupling regimes. We briefly recall early production of single photons with atomic beams, and the operation principles of macroscopic parametric sources, which are used in an overwhelming majority of quantum-optical experiments. We then review the photophysical and spectroscopic properties and compare the advantages and weaknesses of various single nanometre-scale objects used as single-photon sources: atoms or ions in the gas phase and, in condensed matter, organic molecules, defect centres, semiconductor nanocrystals and heterostructures. As new generations of sources are developed, coupling to cavities and nano-fabrication techniques lead to improved characteristics, delivery rates and spectral ranges. Judging from the brisk pace of recent progress, we expect single photons to soon proceed from demonstrations to applications and to bring with them the first practical uses of quantum information.

Overview

AI snapshot

Written from the paper’s full text.

TL;DR

This review surveys the physics, applications, and material platforms for on-demand single-photon sources, emphasizing antibunching from single quantum emitters and cavity coupling. It concludes that source choice depends on the application: room-temperature emitters suffice for number-state uses, while indistinguishable photons for quantum computation require atoms/ions or cryogenic solid-state emitters.

Key findings

  • An ideal single-photon source requires both perfect antibunching and deterministic preparation of the excited state; the emission quantum yield must be unity or close to it. Cavity coupling can enhance emission rates, collection, and spectral properties via Purcell or strong-coupling regimes.
  • For quantum key distribution, a single-photon source tolerates more channel loss than faint laser pulses: the security condition is \(T_{AB} > p_{\rm dark}/\eta_{\rm det}\) for a single-photon source versus \(T_{AB} > \sqrt{2p_{\rm dark}}/\eta_{\rm det}\) for attenuated laser pulses.
  • Parametric down-conversion remains the workhorse for quantum optics but gives Poissonian photon pairs; a typical rate is \(10^7\) pairs/s at 10 mW cw pump, with about 1% probability of two pairs in a 1 ns slot, yielding \(10^6\) single photons/s with 10% detection on one fiber.
  • Emitter comparison: atoms/ions give pure, indistinguishable photons but require complex UHV/trapping setups; molecules, colour centres, and nanocrystals can operate at room temperature but often have broad lines, dark states, or blinking; self-assembled quantum dots are bright and stable at low temperature, with one dot showing >80% photon indistinguishability in a Hong-Ou-Mandel experiment. Cavity examples include Purcell factor \(F_P \approx 5.8\), \(Q \sim 1000\), and \(\beta \approx 80\%\) in a micropost, and \(F_P \approx 6\), \(Q \sim 10^4\) in microdisc cavities.

Methods

  • Review article synthesizing quantum optics, cavity QED, and single-emitter photophysics; no new primary experiments are reported.
  • Compares source classes—atoms/ions, organic molecules, colour centres, semiconductor nanocrystals, self-assembled quantum dots, and heterostructures—using reported spectroscopic and photophysical properties.
  • Summarizes characteristic features in Table 2, described by the authors as estimates for rough comparison.

Limitations

  • Stated: many technical problems remain before single-photon sources become as standard and user-friendly as lasers; current setups must be downsized and simplified for routine use.
  • Stated: progress on sources cannot be separated from detector progress; higher collection/transmission efficiencies and higher detection yields are needed, especially for near-infrared communication wavelengths.
  • Evident from text: this is a review, not a primary study; Table 2 numbers are explicitly estimates, and several source limitations are platform-specific—atoms/ions require complex apparatus, molecules can photobleach or enter dark states, nanocrystals blink, and quantum dots typically require cryogenic temperatures and spectral filtering.

Model-written summary. Check it against the paper before relying on it.

Integrity signals

Registry

Crossref · 10.1088/0034-4885/68/5/r04

Cites

213 of 213 references verified0 citation errors · 0 not checkable

Statistics

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Verification

Claims the paper makes

106 Not checked yet · 87 Own interpretation · 86 No basis given · 1 Own method

Verify all 155 references — free account
  • It may state two separate claims as one. 86
  • Probably not a substantial claim. 73
142 of 142
  • The paper relies on this without support.

    Number-states of light, except the vacuum state, are unfamiliar and very hard to obtain in practice.

    “Except for the trivial vacuum-state (n = 0), number-states of light are unfamiliar and very hard to obtain in practice.”
  • The paper relies on this without support.

    The detection of weak absorption signals is in general hampered by photon noise.

    “The detection of weak absorption signals is in general hampered by photon noise, i.e. fluctuations of the number of photons.”
  • The paper relies on this without support.

    An eavesdropper can escape detection while attempting to extract information from a statistical mixture of number-states, but not from a well-prepared number-state.

    “An eavesdropper can escape detection while attempting to extract information from a statistical mixture of number-states, but not from a well-prepared number-state.”
  • The paper relies on this without support.

    Real photon-counting detectors have limitations such as dead-time and after-pulses.

    “Unfortunately, real photon-counting detectors have their limitations.”
  • The paper relies on this without support.

    For most room-temperature emitters, the coherence time is extremely short, often shorter than picoseconds.

    “For most room-temperature emitters, however, the coherence time is extremely short (often shorter than picoseconds).”
  • The paper relies on this without support.

    For most systems in condensed matter at room temperature, the dephasing time is by several orders of magnitude shorter than the excited state lifetime, so the linewidth is very far from being lifetime-limited.

    “For most systems in condensed matter at room temperature, the dephasing time is by several orders of magnitude shorter than the excited state lifetime, i.e. the linewidth is very far from being lifetime-limited.”
  • The paper relies on this without support.

    In both pseudorandom and physical random number generation approaches, systematic errors and perturbations lead to deviations from a truly random distribution of numbers.

    “In both approaches, systematic errors and perturbations lead to deviations from a truly random distribution of numbers.”
  • The authors state this as an assumption.

    The recorded photon pairs in Bell tests are an unbiased sample of the ensemble.

    “One always assumes that the recorded pairs are an unbiased sample of the ensemble.”
  • The authors state this as an assumption.

    Eve is supposed to possess perfect detectors and to be able to forward signals to Bob without any loss.

    “In particular, Eve is supposed to possess perfect detectors and to be able to forward signals to Bob without any loss.”
  • The authors state this as an assumption.

    Alice and Bob may only use current technology.

    “Alice and Bob, on the other hand, may only use current technology.”
  • The authors state this as an assumption.

    Eve has unlimited technological power within the laws of physics.

    “If we endow Eve with unlimited technological power within the laws of physics”
  • The authors state this as an assumption.

    The cavity mode density is a normalized Lorentzian with a width of ω 0 /Q.

    “Assuming a normalized Lorentzian mode density with a width of ω 0 /Q for the cavity”
  • The paper relies on this without support.

    Atoms are usually very stable under laser illumination and, unlike large molecules and semiconductor systems, do not present long-lived dark states (or can be recycled out of them).

    “Atoms are usually very stable under laser illumination.In contrast to large molecules and semiconductor systems, they do not present long-lived dark states (or if they do, they can be recycled out of them).”
  • The paper relies on this without support.

    The operation time of an atom-based single-photon source is limited by the dwell time of the atom in the cavity mode, up to seconds for a cold atom in a trap.

    “The operation time of an atom-based single-photon source is limited by the dwell time of the atom in the cavity mode, up to seconds for a cold atom in a trap.”
  • The paper relies on this without support.

    Some organic dyes and aromatic molecules emit fluorescence with a high quantum yield and were the first condensed-matter systems for which antibunching was demonstrated.

    “Some organic dyes and aromatic molecules emit fluorescence with a high quantum yield and were the first condensed-matter systems for which antibunching was demonstrated.”
  • The paper relies on this without support.

    Organic molecules less than a nanometre in size can present optical transitions in the visible or near-IR.

    “Organic molecules less than a nanometre in size can present optical transitions in the visible or near-IR.”
  • The paper relies on this without support.

    Compared with atoms, the eigenstates of molecules in condensed matter involve vibrations and phonons, in addition to electronic states.

    “As compared with those of atoms, the eigenstates of molecules in condensed matter involve vibrations and phonons, in addition to electronic states.”
  • The paper relies on this without support.

    Zero-phonon linewidths are often lifetime-limited at low temperatures.

    “Zero-phonon linewidths are often lifetime-limited at low temperatures.”
  • The paper relies on this without support.

    A typical Debye-Waller factor is 0.1, and it decreases quickly for temperatures higher than that of liquid helium, while the width of the ZPL increases steeply because of phonon-induced dephasing processes.

    “A typical value is 0.1, and it decreases quickly for temperatures higher than that of liquid helium, while the width of the ZPL increases steeply because of phonon-induced dephasing processes.”
  • The paper relies on this without support.

    Fluorescence is emitted from the lowest vibration state of the excited electronic state towards vibrational levels of the ground state, giving rise to vibrational fluorescence lines and phonon sidebands.

    “Fluorescence is emitted from the lowest vibration state of the excited electronic state towards vibrational levels of the ground state, giving rise to vibrational fluorescence lines (shifted to the red with respect to the ZPL by vibration frequencies, 100-3000 cm -1 ) and to phonon sidebands (width about 100 cm -1 ).”
  • The paper relies on this without support.

    The width of the other vibronic lines is limited by the lifetime of the vibrations, about a few picoseconds.

    “The width of the other vibronic lines is limited by the lifetime of the vibrations, about a few picoseconds.”
  • The paper relies on this without support.

    The molecular transition is a linear dipole with an oscillator strength of about unity, which corresponds to a spontaneous emission lifetime of a few nanoseconds and to a ZPL linewidth of about 30 MHz.

    “The molecular transition is a linear dipole with an oscillator strength of about unity, which corresponds to a spontaneous emission lifetime of a few nanoseconds and to a ZPL linewidth of about 30 MHz.”
  • The paper relies on this without support.

    III-V semiconductor heterostructures benefit from knowhow developed for electronic microlithography, by which whole emitting structures, including the resonant cavity, can be produced in one microfabrication process.

    “In the latter class of solid-state sources, III-V semiconductor heterostructures benefit from all the knowhow developed for electronic microlithography, by which whole emitting structures, including the resonant cavity, can be produced in one microfabrication process.”
  • The paper relies on this without support.

    A simple photon gun based on a single diamond nanocrystal with a single colour centre at the focus of a microscope objective already exists.

    “The simplest version of a photon gun, based on a single diamond nanocrystal with a single colour centre at the focus of a microscope objective, already exists today.”
  • The paper relies on this without support.

    Such simple devices were already employed in early demonstrations of QKD.

    “Such devices were already employed in early demonstrations of QKD.”
  • The paper relies on this without support.

    Silicon detectors almost reach unity yield in the red part of the spectrum.

    “While silicon detectors almost reach unity yield in the red part of the spectrum, efficient and dedicated detectors must be built for near-infrared communication wavelengths.”
  • The paper relies on this without support.

    Many quantum processing schemes rely on entangled pairs of particles.

    “Many quantum processing schemes rely on entangled pairs of particles.”
  • The paper relies on this without support.

    Large aggregates of molecules, for example J-aggregates, present enhanced fluorescence rates due to cooperative interference of the molecules in a coherence domain.

    “Large aggregates of molecules, for example J-aggregates, present enhanced fluorescence rates due to cooperative interference of the molecules in a coherence domain.”
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Citations

Cites

Show all 213 references

Research works printed but not linked: 11

  1. Alspector J, 1989, Adv. Neutral Inform. Process. Syst., 1, 741
  2. Bell J S, 1965, Physics (NY), 1, 195
  3. Bennett C H Brassard G, 1984, Proc. IEEE Int. Conf. on Computers, Systems and Signal Processing
  4. Bennett C H, 1985, IBM Tech. Discl. Bull., 28, 3153
  5. Cohen-Tannoudji C, 1992, Atom-Photon Interactions
  6. Drexhage K H, 1974, Progress in Optics, XII, 165
  7. Drummond P D, 1999, Quantum Squeezing
  8. Gammon D, 1996, Science, 87, 273
  9. Haroche S, 1992, Les Houches session LIII, ?Fundamental Systems in Quantum Optics?
  10. Loudon R, 1983, The Quantum Theory of Light
  11. Planck M, 1900, Verh. Deutsch. Phys. Ges., 2, 202

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Metadata

Authors
Lounis, B., & Orrit, M.
Affiliations
  • Université de Bordeaux (FR)
  • Leiden University (NL)
Venue
Reports on Progress in Physics
Published
2005-04-21
Volume
68
Issue
5
Pages
1129-1179
ISSN
  • 0034-4885 (ISSN-L)
  • 1361-6633
OpenAlex
W2058874525
Cited by
908
References
213
Citations by year
2026: 31 · 2025: 43 · 2024: 53 · 2023: 36 · 2022: 46 · 2021: 43 · 2020: 42 · 2019: 51 · 2018: 50 · 2017: 56 · 2016: 49 · 2015: 40 · 2014: 66 · 2013: 35 · 2012: 49
FWCI
14.70
Type
journal article
Language
en
Open access
Locations
  • Reports on Progress in Physics (publishedVersion)
  • HAL (submittedVersion)
  • Oskar-Bordeaux (Universite de Bordeaux) (submittedVersion)
Topics
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Semiconductor Quantum Structures and Devices
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Quantum optics and atomic interactions
  • Physical Sciences › Physics and Astronomy › Atomic and Molecular Physics, and Optics › Strong Light-Matter Interactions
Keywords
single-photon sources, photon antibunching, quantum optics, quantum information processing, quantum cryptography, quantum computing, quantum communication, cavity quantum electrodynamics, Purcell effect, strong coupling, parametric down-conversion, organic compounds, defect centers, quantum dots, heterostructures, nanoscale emitters

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