
Quantum optomechanics studies the interaction between light and mechanical motion at the quantum level.Quantum optomechanics is the study of the interaction between electromagnetic radiation (light) and mechanical motion of macroscopic or mesoscopic objects, where quantum effects become relevant. In this regime, the position and momentum of a mechanical oscillator are subject to quantum fluctuations, and light can be used to cool, control, and measure these motions at the quantum level. This field bridges quantum physics and mechanics, allowing researchers to explore the quantum-classical boundary, test fundamental physics, and develop ultra-sensitive sensors and quantum information interfaces.
The theoretical foundations were laid in the 1970s by Vladimir Braginsky, who predicted quantum limits on measurements of mechanical motion. The field gained momentum in the 2000s with advances in micro-fabrication and cryogenics, leading to the first ground-state cooling of a mechanical oscillator in 2010 by several groups.
The core mechanism is radiation pressure: photons carry momentum, and when they reflect off a movable mirror or a tiny mechanical resonator, they exert a force that changes the object's motion. In a typical optomechanical setup, a laser cavity is formed between a fixed mirror and a movable one (or a micro-mechanical membrane). The light intensity in the cavity depends on the mirror's position, and the mirror's position depends on the light pressure, creating a coupled system. By tuning the laser frequency, researchers can either amplify or damp the mechanical motion — the latter is called 'laser cooling' and can bring the oscillator to its quantum ground state. At that point, the mechanical object's behavior is governed by quantum mechanics, and its motion can be entangled with light.
Quantum optomechanics is used to develop ultra-sensitive force and displacement sensors, including detectors for dark matter candidates, and to create interfaces between optical and mechanical quantum systems for quantum computing and communication.
Optomechanical systems have been cooled to temperatures where the mechanical oscillator's motion is dominated by quantum fluctuations, with an average phonon number less than one — meaning it spends most of its time in the quantum ground state.
| G | variable | optomechanical gain |
| Q_m | variable | mechanical quality factor — quality factor |
| P | variable | optical power — power watt |
| G_n | variable | optical response function (complex) |
| M | variable | effective mass of mechanical mode — mass kilogram |
| ω_m | variable | mechanical angular frequency — angular frequency radian per second |
| Re | operator | extracts the real component of a complex number — real part |











