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The master equation of the damped harmonic oscillator is
<br /> \frac{d}{dt}\rho_S(t)<br /> =<br /> -i\omega_0<br /> [a^\dagger a,\rho_S(t)]<br /> +<br /> \gamma_0(\bar n+1)<br /> \{<br /> a\rho_S(t) a^\dagger<br /> -\frac{1}{2}<br /> a^\dagger a \rho_S(t)<br /> -\frac{1}{2}<br /> \rho_S(t) a^\dagger a<br /> \}<br /> +<br /> \gamma_0\bar n<br /> \{<br /> a^\dagger<br /> \rho_S(t)<br /> a<br /> -\frac{1}{2}<br /> a a^\dagger \rho_S(t)<br /> -\frac{1}{2}<br /> \rho_S(t)<br /> a<br /> a^\dagger<br /> \}<br /> \equiv<br /> \mathcal{L}\rho_S(t).<br />
Is there any method to analytically find out some eigenvalues, like the smallest three eigenvalues, of the liouvillian?
I am an engineering graduate, but now a rookie in physics.
Thanks for any advices.
<br /> \frac{d}{dt}\rho_S(t)<br /> =<br /> -i\omega_0<br /> [a^\dagger a,\rho_S(t)]<br /> +<br /> \gamma_0(\bar n+1)<br /> \{<br /> a\rho_S(t) a^\dagger<br /> -\frac{1}{2}<br /> a^\dagger a \rho_S(t)<br /> -\frac{1}{2}<br /> \rho_S(t) a^\dagger a<br /> \}<br /> +<br /> \gamma_0\bar n<br /> \{<br /> a^\dagger<br /> \rho_S(t)<br /> a<br /> -\frac{1}{2}<br /> a a^\dagger \rho_S(t)<br /> -\frac{1}{2}<br /> \rho_S(t)<br /> a<br /> a^\dagger<br /> \}<br /> \equiv<br /> \mathcal{L}\rho_S(t).<br />
Is there any method to analytically find out some eigenvalues, like the smallest three eigenvalues, of the liouvillian?
I am an engineering graduate, but now a rookie in physics.
Thanks for any advices.