0 en meV entre les premiers niveaux purement vibrationnels (?=0,1,2 avec j=0) avec l'état fondamental (?=0, j=0) et éléments de matrice du moment dipolaire en Debye pour les états correspondants ,
0 en meV entre les premiers niveaux purement vibrationnels (?=0,1,2,3 avec j=0) avec l'état fondamental (?=0, j=0) et éléments de matrice du moment dipolaire en Debye pour les états correspondants. Approche d'incorporation, p.104 ,
4 Energies des états liés obtenues par dynamique quantique pour les différents potentiels. Les énergies des niveaux purement vibrationnels que l'on peut identifier sont désignées par 2 nombres quantiques, ? pour la vibration selon l'axe Z et j pour la rotation associée à l'angle, p.134 ,
0 en meV entre les premiers niveaux purement vibrationnels (?=0,1,2 avec j=0) avec l'état fondamental (?=0, j=0) et éléments de matrice du moment dipolaire en Debye pour les états correspondants, p.135 ,
0 en meV entre les premiers niveaux purement vibrationnels (?=0,1,2 avec j=0) avec l'état fondamental (?=0, j=0) et éléments de matrice du moment dipolaire en Debye pour les états correspondants, p.135 ,
0 en meV entre les premiers niveaux purement vibrationnels (?=0,1,2 avec j=0) avec l'état fondamental (?=0, j=0) et éléments de matrice du moment dipolaire en Debye pour les états correspondants. Approche d'incorporation, p.135 ,
0 en meV entre les premiers niveaux purement vibrationnels (?=0,1,2,3 avec j=0) avec l'état fondamental (?=0, j=0) et éléments de matrice du moment dipolaire en Debye pour les états correspondants, p.143 ,
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