Quadrupole moment of the 8+ yrast state in Kr84
R. Schwengner, D. L. Balabanski, G. Neyens, N. Benouaret, D. Borremans, N. Coulier, M. De Rydt, G. Georgiev, S. Mallion, Georgi Rainovski, Gencho Y. Rusev, S. Teughels, K. Vyvey
Abstract
R. Schwengner, D. L. Balabanski, G. Neyens, N. Benouaret, D. Borremans, N. Coulier, M. De Rydt, G. Georgiev, S. Mallion, Georgi Rainovski, Gencho Y. Rusev, S. Teughels, K. Vyvey
Abstract
The quadrupole moment of the ${8}^{+}$ yrast state in $^{84}\mathrm{Kr}$ was measured using the level-mixing spectroscopy technique to be $Q=$ 36(4) $e$ fm${}^{2}$. The result is compared with predictions of the shell model using common sets of effective charges. The comparison of experimental quadrupole moments with calculated values for 8${}^{+}$ states in Kr, Sr and Zr isotopes with $N=$ 48, 50 and for $9/{2}^{+}$ states in isotopes with $N=$ 47, 49 suggests a modification of the effective charges used in this region.
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The quadrupole moment of the ${8}^{+}$ yrast state in $^{84}\mathrm{Kr}$ was measured using the level-mixing spectroscopy technique to be $Q=$ 36(4) $e$ fm${}^{2}$. The result is compared with predictions of the shell model using common sets of effective charges. The comparison of experimental quadrupole moments with calculated values for 8${}^{+}$ states in Kr, Sr and Zr isotopes with $N=$ 48, 50 and for $9/{2}^{+}$ states in isotopes with $N=$ 47, 49 suggests a modification of the effective charges used in this region.
Key concepts: Yrast, Quadrupole, Atomic physics, Physics, Isotope, SHELL model, Mixing (physics), Nuclear physics