(→Known mistakes in our work) |
(→Known errors in our work) |
||
| Line 2: | Line 2: | ||
== Erratum == | == Erratum == | ||
| + | |||
| + | === Generation of a two-photon state from a quantum dot in a microcavity, [http://iopscience.iop.org/1367-2630/13/11/113014/ New J. Phys. 13, 113014 (2011)] === | ||
| + | |||
| + | In page 8, last paragraph the equation $$L_\mathrm{I}+L_\mathrm{II}\approx2\langle a^{\dagger2}a^2\rangle$$ should read $$L_\mathrm{I}+L_\mathrm{II}\approx2\int_0^{\infty}dt\,\langle a^{\dagger2}a^2\rangle(t)$$ as the dynamics are always time integrated. | ||
=== Regimes of strong light-matter coupling under incoherent excitation, [http://pra.aps.org/abstract/PRA/v84/i4/e043816 Phys. Rev. A 84, 043816 (2011)] === | === Regimes of strong light-matter coupling under incoherent excitation, [http://pra.aps.org/abstract/PRA/v84/i4/e043816 Phys. Rev. A 84, 043816 (2011)] === | ||
Contents |
In page 8, last paragraph the equation $$L_\mathrm{I}+L_\mathrm{II}\approx2\langle a^{\dagger2}a^2\rangle$$ should read $$L_\mathrm{I}+L_\mathrm{II}\approx2\int_0^{\infty}dt\,\langle a^{\dagger2}a^2\rangle(t)$$ as the dynamics are always time integrated.
An $i$ is missing in Eq. (10c), so these coefficient should read:
$$L_{\pm}+iK_\pm=\frac{\frac{8\Omega_\mathrm{L}^2}{\gamma_\sigma(\gamma_\sigma+\gamma_\phi)}\big[1 \pm i \frac{5\gamma_\sigma-\gamma_\phi}{4 R_\mathrm{L}}\big]-\frac{\gamma_\sigma-\gamma_\phi}{\gamma_\sigma+\gamma_\phi}\big[1\pm i\frac{\gamma_\sigma-\gamma_\phi}{4R_\mathrm{L}}\big]}{4\big(1+\frac{8 \Omega_\mathrm{L}^2}{\gamma_\sigma(\gamma_\sigma+\gamma_\phi)}\big)}$$