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

TL;DR

This paper develops a three-body model to analyze the structure and decay of $^{16}$Be, confirming a dineutron configuration and providing insights into its resonance energy and decay width.

Contribution

It introduces a full three-body model for $^{16}$Be using hyperspherical R-matrix methods, constrained by experimental data, to investigate its resonance properties and structure.

Findings

Confirmed a dineutron structure for $^{16}$Be

Reproduced the experimental resonance energy with a three-body interaction

Provided estimates for the decay width of $^{16}$Be

Abstract

While diproton decay was first theorized in 1960 and first measured in 2002, it was first observed only in 2012. The measurement of $^{14}$Be in coincidence with two neutrons suggests that $^{16}$Be does decay through the simultaneous emission of two strongly correlated neutrons. In this work, we construct a full three-body model of $^{16}$Be (as $^{14}$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-$^{14}$Be potentials were constructed, constrained by the experimental information on $^{15}$Be. The hyperspherical R-matrix method was used to solve the three-body scattering problem, and the resonance energy of $^{16}$Be was extracted from a phase shift analysis. In order to reproduce the experimental resonance energy of $^{16}$Be within this three-body model, a three-body interaction was needed. For extracting the width of the ground state of $^{16}$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 $^{16}$Be, dependent on the internal structure of the subsystem $^{15}$Be.