1973
DOI: 10.1103/physrevc.8.629
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Structure, Directional-Correlation, and Doppler-Shift Lifetime Measurements inCu61via

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Cited by 31 publications
(4 citation statements)
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“…On the other hand, the small errors of/-forbidden matrix elements mean that an overall agreement between theory and experiment depends sharply on these matrix elements. The data used in the fit are shown in Table2 together with three theoretical results: the calculation with the effective M1 matrix elements determined in this work From [35] b From [36] c From [13] d From [10] Deduced from data in [21,22,37] f From [34] (theory I), the Koops parameters (theory II), and the bare-nucleon g-factors (theory III [30] d From [10] e From [26] f From [34] shows that the effects of proton excitations from a 56Ni core become less important in Zn, Ga, and Ge than Ni and Cu. The experimental data used in the fit and theoretical values calculated with ev= 1.56 e and e, = 1.03 e are compared in Table 3.…”
Section: Determination Of Effective Operatorsmentioning
confidence: 99%
“…On the other hand, the small errors of/-forbidden matrix elements mean that an overall agreement between theory and experiment depends sharply on these matrix elements. The data used in the fit are shown in Table2 together with three theoretical results: the calculation with the effective M1 matrix elements determined in this work From [35] b From [36] c From [13] d From [10] Deduced from data in [21,22,37] f From [34] (theory I), the Koops parameters (theory II), and the bare-nucleon g-factors (theory III [30] d From [10] e From [26] f From [34] shows that the effects of proton excitations from a 56Ni core become less important in Zn, Ga, and Ge than Ni and Cu. The experimental data used in the fit and theoretical values calculated with ev= 1.56 e and e, = 1.03 e are compared in Table 3.…”
Section: Determination Of Effective Operatorsmentioning
confidence: 99%
“…Pour ces raisons, nous avons prefere adopter une forme plus g6n6rale [5][6][7][8][9][10][11][12][13][14][15][16][17][18][19][20][21][22] que celle de 1'Hamiltonien vibrationnel de Bohr et Mottelson [21], ou les etats du coeur sont introduits simplement par les elements de matrice. Pourtant, les noyaux de nickel etant presque vibrationnels, nous avons formellement retenu pour le c0153ur la description vibrationnelle, sp6cifiant le nombre de phonons, et nous avons aussi garde le parametre du couplage en accord avec le parametre k de 1'Hamiltonien de Bohr et Mottelson (k rr 40 MeV).…”
Section: Figunclassified
“…Les niveaux d'6nergie obtenus sont compares aux niveaux experimentaux dans les figures 2 et 3 et dans le tableau II. Pour les six premiers 6tats 1'accord est excellent : dans 61CU les niveaux se correspondent a mieux qu'a 25 keV pres (5 %) et dans 63Cu a mieux qu'a 128 keV (9 %). Pour les quatre 6tats suivants, la sequence des niveaux calcules diffère de la sequence experimentale.…”
Section: Niveaux D'energie Et Fonctions D'onde -unclassified
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