The Lindblad equation describes the time evolution of the density matrix for open quantum systems.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).
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.
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.
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.
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.
| ρ | variable | density matrix of the open quantum system — density matrix |
| t | variable | time — time second |
| H | variable | Hamiltonian of the system — hamiltonian joule |
| L_n | variable | Lindblad operators (jump operators) for each dissipation channel — lindblad operator |
| i | constant | imaginary unit, square root of -1 — imaginary unit = 1 |
| ħ | constant | Planck constant divided by 2π — reduced planck constant = 1.054571817e-34 joule second |
| d/dt | operator | derivative with respect to time — time derivative |
| [H, ρ] | operator | commutator of H and ρ — commutator |
| {L_n† L_n, ρ} | operator | anticommutator of L_n† L_n and ρ — anticommutator |
| ∑_n | operator | sum over all dissipation channels — sum over channels |
| \mathbf{y} | variable | output vector — vector |
| \mathbf{x} | variable | input vector — vector |
| \mathbf{A} | variable | linear transformation matrix — matrix |
| ε'' | variable | Imaginary part of the dielectric function (dielectric loss) — dielectric function |
| ω | variable | Angular frequency of the applied electromagnetic field — angular frequency radian per second |
| ω_0 | variable | Resonance angular frequency of the oscillator — angular frequency radian per second |
| γ | variable | Damping rate of the oscillator — angular frequency radian per second |
| ω_p | variable | Plasma frequency, related to the density of oscillators — angular frequency radian per second |
| N | variable | column density — column density per square metre |
| EW | variable | equivalent width — equivalent width metre |
| f | variable | oscillator strength — oscillator strength |
| λ | variable | wavelength — wavelength metre |
| concentration | variable | local concentration of the diffusing species — concentration mole per cubic metre |
| t | variable | time — time second |
| flux | variable | diffusive flux vector — diffusive flux mole per square metre per second |
| d/dt | operator | rate of change with respect to time — time derivative |
| divergence | operator | measures the net outflow of a vector field per unit volume — divergence operator |
| Δv | variable | Change in velocity of the rocket — velocity metre per second |
| v_e | variable | Effective exhaust velocity — velocity metre per second |
| m_0 | variable | Initial total mass (rocket + propellant) — mass kilogram |
| m_f | variable | Final total mass (after propellant expended) — mass kilogram |
| ln | operator | Natural logarithm of the mass ratio — natural logarithm |









