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Lindblad equation

The Lindblad equation or master equation in the Lindblad form is the most general type of master equation allowed by Quantum mechanics to describe non-unitary (dissipative) evolution of the density matrix ρ (such as ensuring normalisation and hermiticity of ρ). It reads:

\dot\rho=-{i\over\hbar}[H,\rho]-{1\over\hbar}\sum_{n,m}h_{n,m}\big(\rho L_m L_n+L_m L_n\rho-2L_n\rho L_m\Big)+\mathrm{h.c.}

where ρ is the density matrix, H is the hamiltonian part, Lm are operators defined by the system to model as are the constants hn,m.

The most common Lindblad equation is that describing the damping of a quantum harmonic oscillator, it has L0 = a, L_1=a^{\dagger}, h_{0,1}=-(\gamma/2)(\bar n+1), h_{1,0}=-(\gamma/2)\bar n with all others hn,m = 0. Here \bar n is the mean number of excitations in the reservoir damping the oscillator and γ is the decay rate.

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