concept

coherent state

A coherent state is a quantum state of light or matter with well-defined phase, used in precision generation, noise reduction, and quantum imaging.
22 related articles · 1 formulas · 1 who worked here

Description

A coherent state is a family of quantum states of the harmonic oscillator (e.g., an electromagnetic field mode) that minimize the Heisenberg uncertainty relation. Mathematically, it is an eigenfunction of the annihilation operator a, a|α⟩ = α|α⟩, where the complex number α specifies the mean amplitude and phase. Expanding in number (Fock) states reveals a Poissonian photon statistics: the probability of detecting exactly n photons is e^{-|α|²} |α|^{2n}/n!. The average energy is ħω|α|². Such states do not spread over time and preserve the shape of the wave packet, which is why they often serve as a bridge between quantum and classical descriptions.

History

Schrödinger (1926) first formulated the concept of non-spreading wave packets for the oscillator. In 1963–65, Glauber, Sudarshan, and Klauder independently rediscovered coherent states in the context of quantum optics, showing that they describe ideal laser radiation. Glauber received the 2005 Nobel Prize for this work. In subsequent decades, coherent states found applications in atomic physics (coherent population trapping), condensed matter physics (Bose-Einstein condensates), and quantum information.

How it works

Generation of coherent states is achieved by a classical current interacting with the quantum field. The Schrödinger equation with the interaction Hamiltonian H_int = iħ(ϵ a† − ϵ* a) yields the evolution of the displacement operator, creating a coherent state from the vacuum. The stability under time evolution is due to the preservation of quadrature variances. However, interaction with a thermal bath leads to loss of coherence (damping)—the average photon number decreases exponentially, but the state remains coherent. This robustness is used in laser interferometry: even after traveling long distances, the interference pattern is determined by the phase α.

In practice

Without coherent states, there would be no lasers, optical interferometers, and holograms—it is a fundamental tool of modern optics.

Fun fact

When reflecting coherent light from an ordinary mirror, it remains coherent—losses only reduce α. That's why laser pointers work even after hundreds of kilometers in optical fiber.

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Formulas

$$|\text{cat}\rangle = \frac{1}{\sqrt{2}}(|\alpha\rangle + |-\alpha\rangle)$$
Quantum superposition of two coherent states.
What is in the formula
|cat⟩variablecat state vector — quantum state
|α⟩variablecoherent state with amplitude α — coherent state
|−α⟩variablecoherent state with amplitude −α — coherent state

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