207 E.2 Probabilité qu'une impulsion contienne au moins 1 photon . . . . . 209 E.3 Probabilité qu'une impulsion contienne 1 et 1 seul photon, 211 E.5 Efficacité de collection imparfaite . . . . . . . . . . . . . . . . . . . . . 211 ,
A grand attendue sur la courbe d'autocorrélation en intensité. La méthode utilisée repose sur le principe des « fonctions d'onde stochastiques nous savons qu'il existe une probabilité p 2 , non nulle, d'avoir deux photons par impulsion. En outre, nous connaissons une relation entre p 2 et la probabilité p 1 d'avoir une impulsion avec un seul photon (formule 5.23 du chapitre 5) Toutefois, nous ne connaissons ni p 1 , ni p 2 . Nous allons tenter de calculer ces deux paramètres, à partir d'une approche « fonction d'onde stochastique » encore appelée méthode des « fonctions d'onde Monte Carlo » [145, 146]. Nous considérerons à nouveau un atome à deux niveaux (|f , fondamental et |a, excité) couplé simultanément au champ laser de notre source impulsionnelle et aux différents modes du vide du champ électromagnétique quantifié. L'interaction atome-laser, à l'origine du processus d'absorption et d'émission stimulée ,
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