English

Three-body model for the two-neutron decay of $^{16}$Be

Nuclear Theory 2017-03-14 v1

Abstract

While diproton decay was first theorized in 1960 and first measured in 2002, it was first observed only in 2012. The measurement of 14^{14}Be in coincidence with two neutrons suggests that 16^{16}Be does decay through the simultaneous emission of two strongly correlated neutrons. In this work, we construct a full three-body model of 16^{16}Be (as 14^{14}Be + n + n) in order to investigate its configuration in the continuum and in particular the structure of its ground state. In order to describe the three-body system, effective n-14^{14}Be potentials were constructed, constrained by the experimental information on 15^{15}Be. The hyperspherical R-matrix method was used to solve the three-body scattering problem, and the resonance energy of 16^{16}Be was extracted from a phase shift analysis. In order to reproduce the experimental resonance energy of 16^{16}Be within this three-body model, a three-body interaction was needed. For extracting the width of the ground state of 16^{16}Be, we use the full width at half maximum of the derivative of the three-body phase shifts and the width of the three-body elastic scattering cross section. Our results confirm a dineutron structure for 16^{16}Be, dependent on the internal structure of the subsystem 15^{15}Be.

Keywords

Cite

@article{arxiv.1611.00604,
  title  = {Three-body model for the two-neutron decay of $^{16}$Be},
  author = {A. E. Lovell and F. M. Nunes and I. J. Thompson},
  journal= {arXiv preprint arXiv:1611.00604},
  year   = {2017}
}

Comments

13 pages, 9 figures, submitted to Phys. Rev. C