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Cohen-Tannoudji, à paraître dans le numéro spécial d'Applied Physics B sur "Optics and Interferometry with atoms ,
Sa grande profondeur (jusqu'à plusieurs Kelvins) nous permet de atomes avec une surface, le piégeage d'isotopes rares, des expériences de recherche de moment dipolaire anormal sur des fontaines atomiques, sans oublier la réalisation d'horloges à césium de plus grande précision ,
23 a) Mouvement d'un atome à deux niveaux dans une onde lumineuse, p.23 ,
29 a) Le régime final, p.30 ,
57 a) La cellule à faible pression de vapeur de césium, p.57 ,
67 03B1) Le laser principal, p.67 ,
71 a) Fonctionnement de la diode laser libre, p.71 ,
77 03B1) Description du montage, p.77 ,
96 03B1) Mise en place de la sonde étroite, p.96 ,
98 calcul de l'état stationnaire à l'ordre zéro ..... 100 perturbation l'onde sonde ,
110 a) Variation avec la pression de la vapeur de césium dans la cellule ..... 110 b) Variation avec l'intensité des faisceaux piège, p.112 ,
127 a) Origine du déséquilibre, p.127 ,
135 a) Expression de la force, p.135 ,
151 a) Etat stationnaire pour un atome immobile, 151 03B1) Champ laser ..... 153 ,
155 03B1) Passage dans le référentiel tournant, p.155 ,
159 a) Effet d'un champ constant, p.159 ,
164 03B1) Expression de la force, p.164 ,
172 03B3) Traitement quantique, p.175 ,
179 a) Expressions de la densité et de la taille. Ordres de grandeur, 179 03B1) Régime n ~ n c ..... 179 ,
183 03B1) Modification du didpositif expérimental, p.183 ,
195 a) Comparaison piège-mélasse ,
227 03B1) Variation avec l'intensité laser piège, p.227 ,
234 a) Idée de l'interprétation, p.234 ,
238 03B1) Ordre zéro -Notations, p.239 ,
244 03B1) Signal entre la sonde et le laser piège, p.244 ,
251 a) Signal entre la pompe annexe et la sonde, p.251 ,
269 a) Mélange à quatre ondes vers l'arrière, p.269 ,
Mélange à quatre ondes vers l'avant -Signal hyper, p.275 ,
285 a) Commodité d'utilisation, p.285 ,
289 a) Généralités sur le piège dipolaire, p.289 ,