论文标题

$^{25} $ f的核心由$^{25} $ f(-1p)$^{24} $ o反应

The Core of $^{25}$F studied by the $^{25}$F(-1p)$^{24}$O reaction

论文作者

Crawford, H. L., Jones, M. D., Macchiavelli, A. O., Fallon, P., Bazin, D., Bender, P. C., Brown, B. A., Campbell, C. M., Clark, R. M., Cromaz, M., Elman, B., Gade, A., Holt, J. D., Janssens, R. V. F., Lee, I. Y., Longfellow, B., Paschalis, S., Petri, M., Richard, A. L., Salathe, M., Tostevin, J. A., Weisshaar, D.

论文摘要

$^{25} $ f($ 5/2^+)(-1p)^{24} $ o反应在NSCL上使用S800光谱仪进行了研究。与壳型预期相比,地基态至地面过渡的实验光谱因子表明,质子$ d_ {5/2} $强度的大量耗竭。我们的结果支持Tang \ textit {等}报告的发现,从$(p,2p)$反应的RIBF中的研究中。如果$^{25} $ f和$^{24} $ o地面 - 如果$^{24} $ O在$^{25} $ f中充当强大且刚性的双重核心,则$^{24} $ o地面态的重叠率要小得多。我们在$ d_ {5/2} $质子的粒子振动耦合(PVC)的框架内解释结果,该结果与有效核心的Quadrupole Phonon耦合。这种方法通过需要有效的$^{24} $ o*核心,以$ \hbarΩ_2$ = 3.2 meV和a $ b(e2)〜2.7 $ w.u.,比裸露的$^{24} $ O。 Nilsson变形的平均场和PVC模型似乎都捕获了$^{25} $ f的有效核心的性质,这表明附加的质子倾向于以这种方式略微使免费的,双重的魔术$^{24} $偏振,以使其变为略微变形或Quadrupole振动器。

The $^{25}$F($5/2^+) (-1p) ^{24}$O reaction was studied at the NSCL using the S800 spectrometer. The experimental spectroscopic factor for the ground-state to ground-state transition indicates a substantial depletion of the proton $d_{5/2}$ strength compared to shell-model expectations. Our result supports the findings reported by Tang \textit{et al.}, from their study of the $(p,2p)$ reaction at RIBF. The overlap between the $^{25}$F and $^{24}$O ground-states is considerably less than anticipated if $^{24}$O acted as a robust and rigid doubly-magic core in $^{25}$F. We interpret the results within the framework of the Particle-Vibration Coupling (PVC) of a $d_{5/2}$ proton coupled to a quadrupole phonon of an effective core. This approach provides a good description of the experimental data by requiring an effective $^{24}$O* core with a phonon energy of $\hbarω_2$= 3.2 MeV, and a $B(E2) ~ 2.7$ W.u., softer and more collective than a bare $^{24}$O. Both the Nilsson deformed mean field and the PVC models appear to capture the properties of the effective core of $^{25}$F, suggesting that the additional proton tends to polarize the free, doubly magic $^{24}$O in such a way that it becomes either slightly deformed or a quadrupole vibrator.

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