Quantum states of light characterized by a Gaussian Wigner function, including coherent and squeezed states.Gaussian states are a special class of quantum states of light (and other bosonic systems) whose Wigner function—a quasi-probability distribution that visualizes the state in phase space—has a Gaussian shape. This family includes the vacuum state, coherent states (the closest quantum analog to classical light waves), and squeezed states, where quantum noise is reduced in one quadrature at the expense of increased noise in the other. They are the workhorses of continuous-variable quantum optics and quantum information, because they are both experimentally accessible and theoretically tractable.
The concept emerged from the 1930s work of Eugene Wigner on quantum corrections to classical statistical mechanics, but the explicit classification of Gaussian states in quantum optics was developed in the 1980s and 1990s, notably by researchers like Klaus Vogel and Helmut Risken, and later formalized in the context of quantum information by Samuel Braunstein and others.
The Wigner function of a Gaussian state is fully described by its first and second moments—the mean position and momentum, and their covariance matrix. This simplicity means that many operations, such as beam splitters, phase shifts, and squeezers, act linearly on these moments, making calculations straightforward. Measurements like homodyne detection, which project onto quadrature amplitudes, also preserve the Gaussian character, allowing for efficient classical simulation of many Gaussian processes unless non-Gaussian operations (e.g., photon counting) are introduced.
Gaussian states are used in quantum cryptography, quantum teleportation, and gravitational-wave detectors, where squeezed light reduces measurement noise.
The vacuum state itself is a Gaussian state, and its zero-point fluctuations are a direct consequence of the Heisenberg uncertainty principle.



















