Table 1 Set of parameters used to reproduce spectra and \(g^{(2)}\left( t \right)\) functions, as shown in Fig. 4.
From: Complex plasmon-exciton dynamics revealed through quantum dot light emission in a nanocavity
\(\hbar {\upkappa}\) | 400 meV | Intrinsic plasmon decay rate |
\(\hbar {\upgamma}_{{\mathrm{gB}}}\) | 0.1 \(\upmu {\mathrm{eV}}\) | Intrinsic decay rate of the bright exciton |
\(\hbar {\upgamma}_{{\mathrm{gD}}}\) | \(0.005\,\upmu {\mathrm{eV}}\) | Intrinsic decay rate of the dark exciton |
\(\hbar {\upgamma}_{{\mathrm{DB}}}^0\) | 0.2 \(\upmu {\mathrm{eV}}\) | Rate of energy transfer between the dark and the bright exciton |
\(\hbar {\upgamma}_{{\mathrm{BB}}}\) | 130 meV | Pure dephasing of the bright exciton |
\(\hbar {\upgamma}_{{\mathrm{DD}}}\) | 50 meV | Pure dephasing of the dark exciton (broadening of the dark-exciton line) |
\(\hbar {\upgamma}_{{\mathrm{Bg}}}\) | 1 n\({\mathrm{eV}}\) | Incoherent pumping of the bright exciton |
\(\hbar {\upgamma}_{{\mathrm{Dg}}}\) | 5 n\({\mathrm{eV}}\) | Incoherent pumping of the dark exciton |
\(\hbar {\mathrm{g}}_{\mathrm{B}}\) | 100 meV | Coupling between plasmon and the bright exciton |
\(\hbar {\mathrm{g}}_{\mathrm{D}}\) | 35 \(\upmu {\mathrm{eV}}\) | Coupling between plasmon and the dark exciton |
\(\hbar {\upomega}_{{\mathrm{pl}}}\) | 1.93 \({\mathrm{eV}}\) | Plasmon energy |
\(\hbar {\upomega}_{\mathrm{D}}\) | 1.95 \({\mathrm{eV}}\) | Emission energy of the dark exciton |
\(\hbar {\upomega}_{\mathrm{B}}\) | 2.00 \({\mathrm{eV}}\) | Emission energy of the bright exciton |
