
Techniques for manipulating light at the quantum level, including extraction from vacuum and molecular emission.Quantum light control refers to the set of techniques for manipulating light at the level of individual photons, where the quantum nature of the electromagnetic field becomes directly observable. This includes generating single photons on demand, squeezing light to reduce noise in one observable at the cost of increasing it in another, and even extracting photons from the vacuum — the quantum ground state of the field. It also covers controlling how molecules emit light, such as shaping the emission spectrum or direction through cavity quantum electrodynamics.
The theoretical foundations were laid in the 1960s and 1970s, with Roy Glauber formalizing quantum coherence and the first squeezed light produced in 1985 by Richard Slusher and colleagues at Bell Labs. The dynamical Casimir effect was first observed experimentally in 2011 by Chris Wilson and collaborators.
At the heart of quantum light control is the ability to prepare and measure specific quantum states of the electromagnetic field. Single-photon sources use quantum emitters like atoms, quantum dots, or defect centers in crystals that emit one photon at a time. Squeezed light is produced by nonlinear optical crystals that correlate photon pairs, reducing quantum fluctuations in one quadrature. Vacuum emission can be stimulated by rapidly changing boundary conditions — the dynamical Casimir effect — where moving mirrors or superconducting circuits convert virtual photons into real ones. Cavity QED uses high-finesse optical cavities to enhance or suppress spontaneous emission, giving experimenters control over how and when a molecule releases its energy as light.
Quantum light control underpins quantum cryptography, quantum key distribution, and photonic quantum computing, where single photons serve as flying qubits, and squeezed light enhances the sensitivity of gravitational-wave detectors like LIGO.
The vacuum is not truly empty — it teems with virtual photons that can be coaxed into real ones by rapidly changing the speed of a mirror, an effect first predicted by Gerald Moore in 1970.
| L | variable | Luminosity (total power emitted) — luminosity watt |
| R | variable | Radius of the emitting region — radius metre |
| n | variable | Number density of particles — number density per cubic metre |
| γ | variable | Lorentz factor of the particles — lorentz factor |
| m | variable | Particle rest mass — mass kilogram |
| c | constant | Speed of light in vacuum, the maximum speed for any particle. — speed of light = 299792458 metre per second |
| dN/dE | variable | Differential number of particles per energy interval — particle spectrum joule per joule |
| E | variable | Particle energy — energy joule |
| alpha | variable | Spectral index of the power law |
| E_cut | variable | Cutoff energy — energy joule |



