Abstract

Abstract We use a microscopic multicluster model to investigate the structure of $^{10}{\rm Be}$ and of $^{11}{\rm Be}$. These nuclei are described by $\alpha +\alpha+n+n$ and $\alpha +\alpha+n+n+n$ configurations, respectively, within the Generator Coordinate Method (GCM). The 4- and 5-body models raise the problem of a large number of generator coordinates (6 for $^{10}{\rm Be}$ and 9 for $^{11}{\rm Be}$), which requires specific treatment. We address this issue by using the Stochastic Variational Method (SVM), which is based on an optimal choice of the basis functions, generated randomly. The model provides good energy spectra for low-lying states of both nuclei. We also compute rms radii and densities, as well as electromagnetic transition probabilities. We analyze the structure of $^{10}{\rm Be}$ and of $^{11}{\rm Be}$ by considering energy curves, where one of the generator coordinates is fixed during the minimization procedure.

Highlights

  • We aim to investigate the 10Be and 11Be isotopes within the α + α + n + n and α + α + n + n + n Generator Coordinate Method (GCM)

  • The main goal of this paper is to investigate the 10Be and 11Be nuclei within a microscopic multicluster model

  • We have confirmed that the Stochastic Variational Method (SVM) provides an excellent framework to address this issue

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Summary

Introduction

About 50 years ago, the seminal paper of Ikeda and his collaborators [1] showed that α-clustering is expected near the α threshold of 4N nuclei. This conjecture leads to the famous Ikeda diagram and was remarkably confirmed by theory and by experiment. A typical example is 6He, which requires three-body models to accurately describe the halo neutrons. Accurate bases require large numbers of functions This problem can be efficiently addressed by the Stochastic Variational Method (SVM), where a random choice of the basis sets is performed, which permits optimizing the basis [20, 21].

Wave functions
Brief description of the SVM
The 10Be nucleus
The 11Be nucleus
Conclusion
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