[19], où la corrélation concerne souvent des paires de spins 1/2. Ici la corrélation non locale est entre l'atome et le champ. Les deux états atomiques internes |f> et | e & # x 3 E ,
nous allons envoyer un second atome pour sonder l, p.102 ,
Il permet ainsi de faire une distinction entre l'état non classique précédent et l'état où le champ est dans un mélange statistique représenté par la matrice densité ,
Par contre s'il est dans l'état |e>, il induit deux effets. Le premier est de faire entrer dans la cavité un champ 03B1e -i0394T , où T est l'intervalle de temps qui sépare les instants d'arrivée du premier et du second atome à la cavité, la phase 0394 T est due au fait que la source évolue avec une fréquence différente de celle de la cavité. Le second effet de l'atome est de produire un déphasage 0394 t int sur un champ qui existerait déjà à l ,
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stocké dans une cavité supraconductrice de très grand facteur de qualité constituent un système simple, bien isolé de son environnement et permettant d'étudier l'interaction rayonnement-matiére. Dans ce mémoire nous présentons une expérience réalisé dans une situation où l'atome et le champ sont en résonance. Le signal de Rabi correspondant à l'évolution de la population atomique présente des composantes de Fourier dont les fréquences sont proportionnelles aux racines carrées des entiers successifs ; ceci met directement en évidence la quantification du champ dans la cavité. Nous montrons également que l'analyse des signaux permet de remonter aux propriétés statistiques du champ. Enfin, en analysant l'interaction non résonante de l'atome avec la cavité, nous montrons que dans un futur proche, il sera possible de préparer des superpositions quantiques d'états du champ présentant des différences mésoscopiques, Ces états sont de type "chat de Schrödinger". L'étude de la décohérence de ces états en fonction du nombre de photons que contient le champ permet d'explorer la frontière qui existe entre le monde quantique et le monde classique ,
Atome à deux niveaux ,