concept

Wigner function

The Wigner function is a quasiprobability distribution representing quantum states in phase space.
37 related articles · 2 formulas

Description

The Wigner function represents a quantum state in phase space (the space of coordinates and momenta). It is a quasiprobability distribution: integrating over momenta yields the probability for coordinates, and vice versa. However, unlike true probability, it can take negative values. Negative regions indicate quantum correlations and non-classicality, serving as a resource in quantum computing. The map of the Wigner function, even with negative peaks, remains the most detailed snapshot of quantum reality.

History

Proposed by Hungarian-American physicist Eugene Wigner in 1932 as a bridge between quantum and classical statistical mechanics. Later, it became a key tool in quantum optics and quantum information. Experimental measurement of the Wigner function became possible with the development of homodyne tomography in the 1990s.

How it works

The Wigner function for a pure state with wave function \(\psi(x)\) is defined as \\(W(x,p) = \frac{1}{\pi \hbar} \int_{-\infty}^{\infty} \psi^*(x+y) \psi(x-y) e^{2i p y / \hbar} dy\\). For mixed states, it is analogous with the density matrix. The Heisenberg uncertainty principle manifests itself in constraints on the possible shapes of the distribution. Negativity is a direct consequence of the superposition principle and cannot be eliminated by any classical mixing.

In practice

The Wigner function aids in developing quantum computers—it reveals errors in qubits and allows for precise tomographic images of quantum states.

Fun fact

The negativity of the Wigner function is a precise indicator that a quantum state cannot be efficiently simulated on a classical computer (quantum supremacy).

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Formulas

$$\delta = \int |W(X,P)|\, dX dP - 1$$
Measures nonclassicality via Wigner function negativity.
What is in the formula
WvariableWigner function of the quantum state — Wigner function
Xvariableposition quadrature variable — position metre
Pvariablemomentum quadrature variable — momentum kilogram metre per second
∫ dX dPoperatorintegration over the full phase space — double integral
| |operatorabsolute value of the Wigner function — absolute value
δ=\int|w(x,p)|dxdp-1 · 2505.01942v2
$$k(r) = rac{\sigma^2 2^{1-\nu}}{\Gamma(\nu)} \left( \frac{\sqrt{2\nu} r}{l} \right)^\nu K_\nu \left( \frac{\sqrt{2\nu} r}{l} \right)$$
A covariance function for Gaussian processes with smoothness parameter ν.
What is in the formula
rvariabledistance between two points — distance metre
νvariablesmoothness parameter
lvariablelength scale parameter — length metre
σvariablevariance amplitude — variance square metre
ΓoperatorGamma function, generalizes factorial — gamma function
K_νoperatorModified Bessel function of the second kind of order ν — modified bessel function second kind
k_ν(r)=σ_f^2\frac{2^{1-ν}}{\gamma(ν)}(\frac{\sqrt{2ν}r}{l_f})^νk_ν(\frac{\sqrt{2ν}r}{l_f}) · 2601.06656

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