état fondamental X 3 03A3 -g ont été tirées de [ 25 ]. Ces valeurs maintenant précises et fiables permettent de "placer ,
B0) est fixée par la tête de bande On définit et on ajuste ensuite T(B1) et T(P1) par rapport à cette nouvelle origine ,
ajustés séparément, puisque seule une combinaison de ces 2 paramètres rend compte de la perturbation près de (B 0 + g, p.55 ,
2022 les valeurs diagonales restent très proches de 1 : 2022 les valeurs non diagonales sont effectivement faibles ; les plus importantes correspondent à v 1 -v 0 = ±1 et sont inférieures à 0, p.16 ,
Les corrections à g 01 et P impliquent en effet des termes croisés : provenant de l'interaction entre l'état 3 03A3 considéré et tous les états 3 03A0 . Les corrections observées nécessitent des termes dont l'ordre de grandeur estApproximation Methods in Quantum Mechanics, 1969. ,
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