Résumé
The effective LEF αe is obtained by computing over the entire comb spectrum the mean square of α(ν)such as αe = s 1ν 1 Z comb dν0α2(ν0), (1) with 1ν the width of the comb spectrum, while ν0 is the frequency of the radiation emitted by the laser. Therefore, assuming a QD as a two-level atomic system and that the center of the emitted comb spectrum matches the center frequency of the QD transition, integration of Eq. (1) leads to 1ν = 2√30αe (2) with 0 the homogeneous broadening of the QD transition. The factor two was missing in [1].
| langue originale | Anglais |
|---|---|
| Pages (de - à) | 856 |
| Nombre de pages | 1 |
| journal | Optics Letters |
| Volume | 45 |
| Numéro de publication | 4 |
| Les DOIs |
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| état | Publié - 15 févr. 2020 |
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