equation

Lindblad equation

The Lindblad equation describes the time evolution of the density matrix for open quantum systems.
18 related articles · 6 formulas · 4 who worked here

Description

Proposed in 1976 by Göran Lindblad (independently of the group of Gorini, Kossakowski, and Sudarshan), the equation became a cornerstone of the theory of open quantum systems. Before it, scientists puzzled over how to include the inevitable influence of the environment on a quantum object—be it an atom, a photon, or a qubit—in calculations. The Lindblad equation adds to the standard quantum Schrödinger equation an additional term that acts like an invisible hand, erasing coherence (the coordination of quantum states).

History

In 1976, Swedish physicist Göran Lindblad published a work presenting a mathematically rigorous form for the generator of a quantum dynamical semigroup. Almost simultaneously, Vittorio Gorini, Andrzej Kossakowski, and George Sudarshan obtained an identical result. Previously, there were phenomenological equations (e.g., the Bloch equations), but they suffered from problems—they could lead to negative probabilities. Lindblad proved that his form is necessary and sufficient to obtain a completely positive mapping of the dynamics.

How it works

The equation is widely used in quantum optics, information science, and condensed matter theory. It models spontaneous emission of atoms, losses in resonators, decoherence of qubits in quantum processors, and even the stabilization of states through dissipation. Its range of validity is the Markovian assumption (the environment has no memory), which breaks down in strongly correlated systems requiring non-Markovian generalization.

In practice

Models of quantum computers are built on it to predict how quickly a qubit will be destroyed by environmental noise—without this, quantum computing would remain just a dream.

Fun fact

Paradoxically, the equation not only predicts the destruction of fragile quantum properties but also explains how stability can arise—for example, why laser light remains coherent even though the environment seems like it should spoil it.

Concept graph →

Formulas

$$\frac{d\rho}{dt} = -\frac{i}{\hbar}[H,\rho] + \sum_n \left( L_n \rho L_n^\dagger - \frac{1}{2} \{ L_n^\dagger L_n, \rho \} \right)$$
Describes open quantum system evolution with dissipation.
What is in the formula
ρvariabledensity matrix of the open quantum system — density matrix
tvariabletime — time second
HvariableHamiltonian of the system — hamiltonian joule
L_nvariableLindblad operators (jump operators) for each dissipation channel — lindblad operator
iconstantimaginary unit, square root of -1 — imaginary unit = 1
ħconstantPlanck constant divided by 2π — reduced planck constant = 1.054571817e-34 joule second
d/dtoperatorderivative with respect to time — time derivative
[H, ρ]operatorcommutator of H and ρ — commutator
{L_n† L_n, ρ}operatoranticommutator of L_n† L_n and ρ — anticommutator
∑_noperatorsum over all dissipation channels — sum over channels
\frac{dρ}{dt}=-\frac{i}{ħ}[h_0,ρ]+2γ(\barn+1)\mathcal{d}[b]ρ+2γ\barn\mathcal{d}[b^\dagger]ρ+2k\mathcal{d}[f(x)]ρ · 2505.01942v2
l_{{rot}}\hat{σ}=-\frac{1}{2ħ^2}\intd^3xd^3yd^{kl}_a(\vec{x},\vec{y})χ_{ki;lm}(\vec{x},\vec{y})[\hat{l}_i,[\hat{l}_m,\hat{σ}]] · 2605.12172v1
\frac{dρ}{dt}=-\frac{i}{ħ}[h,ρ]+\sum_k(l_kρl_k^\dagger-\frac{1}{2}\{l_k^\daggerl_k,ρ\}) · 2607.09247
$$\mathbf{y} = \mathbf{A} \mathbf{x}$$
Output is a linear transformation of input.
What is in the formula
\mathbf{y}variableoutput vector — vector
\mathbf{x}variableinput vector — vector
\mathbf{A}variablelinear transformation matrix — matrix
y=ax · 2607.13204
$$\varepsilon''(\omega) = \frac{\omega_p^2 \gamma \omega}{(\omega_0^2 - \omega^2)^2 + \gamma^2 \omega^2}$$
Describes the frequency-dependent dielectric loss in resonant materials.
What is in the formula
ε''variableImaginary part of the dielectric function (dielectric loss) — dielectric function
ωvariableAngular frequency of the applied electromagnetic field — angular frequency radian per second
ω_0variableResonance angular frequency of the oscillator — angular frequency radian per second
γvariableDamping rate of the oscillator — angular frequency radian per second
ω_pvariablePlasma frequency, related to the density of oscillators — angular frequency radian per second
\frac{\varepsilon''(ν)}{ν}=\frac{sν_0^2\gammaν}{(ν^2-ν_0^2)^2+\gamma^2ν^2}+b(ν) · 2607.14764
$$N = \frac{EW}{f \lambda^2}$$
Column density relates to equivalent width in optically thin limit.
What is in the formula
Nvariablecolumn density — column density per square metre
EWvariableequivalent width — equivalent width metre
fvariableoscillator strength — oscillator strength
λvariablewavelength — wavelength metre
n_{{nai}}=1.13*10^{20}\frac{ew}{f_{lu}λ_{lu}^2}{cm}^{-2} · 2607.20606v1
$$ rac{ ext{d} ext{concentration}}{ ext{d}t} = ext{divergence of flux}$$
Describes how concentration changes over time due to diffusion.
What is in the formula
concentrationvariablelocal concentration of the diffusing species — concentration mole per cubic metre
tvariabletime — time second
fluxvariablediffusive flux vector — diffusive flux mole per square metre per second
d/dtoperatorrate of change with respect to time — time derivative
divergenceoperatormeasures the net outflow of a vector field per unit volume — divergence operator
\partial_tφ\simeq\nabla*[\frac{(1-φ)^2φ}{n_0\zeta_0μ(φ)}\nabla\pi] · 2606.31786
$$\Delta v = v_e \ln\frac{m_0}{m_f}$$
The change in velocity equals exhaust velocity times log of mass ratio.
What is in the formula
ΔvvariableChange in velocity of the rocket — velocity metre per second
v_evariableEffective exhaust velocity — velocity metre per second
m_0variableInitial total mass (rocket + propellant) — mass kilogram
m_fvariableFinal total mass (after propellant expended) — mass kilogram
lnoperatorNatural logarithm of the mass ratio — natural logarithm
δv=i_{sp}g_0\ln\frac{m_0}{m_f} · 2607.02691
δv=i_{{sp}}g_0\ln\frac{m_0}{m_f} · 2607.02691v1

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