How a Magnesium Nucleus Grows a Neutron Coat express

Original: "Neutron radii and semi-phenomenological treatment of neutron distributions for Mg isotopes"
arXiv:2608.09429v2 · 2026-08-10 · CC BY 4.0 · 1 min
In some magnesium isotopes, neutrons extend beyond the nucleus, forming a diffuse halo.

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The atomic nucleus is usually pictured as a dense ball where protons and neutrons are mixed together. But in some isotopes, neutrons can stick out far beyond this ball, forming a diffuse shell — a neutron halo. This is especially common in nuclei with many more neutrons than protons.

Physicists took magnesium isotopes — from light magnesium-24 to heavy magnesium-38—and calculated how they scatter off carbon at an energy of 240 MeV per nucleon. By measuring how often the nuclei graze each other, they could determine the radius of the neutron cloud. It turned out that in magnesium-37, one neutron is so weakly bound that it forms a single halo.

A neutron halo is like a comet's fuzzy tail: the main nucleus is dense, while around it is a barely visible cloud of one or two neutrons.

Then the team applied the same approach to magnesium-40, which had not been studied before. The calculations showed that two neutrons are so loosely attached that they form a double halo. Such nuclei live for fractions of a second, but they are the perfect testing ground for our understanding of nuclear forces.

The double halo in magnesium-40 is a rare case where two neutrons pair up and together venture beyond the dense core. It's like two climbers roping together on the very edge of a cliff.

Original abstract

as written by the authors arXiv:2608.09429v2

Involving the charge radii of \rm Mg isotopes, as calculated using the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc), we have extracted the neutron radii of $$^{24-38}$$\rm Mg isotopes by studying their reaction cross sections ($$\sigma_{R}$$) from $$^{12}$$\rm C at 240 MeV/nucleon within the framework of Glauber model. The calculations use (i) descriptions of nuclei in terms of the Slater determinant involving harmonic oscillator single-particle wave functions (SDHO), and (ii) two-parameter Fermi (2pF) shape of density distribution, with the aim to assess the density dependence of neutron skin in $$^{24-38}$$\rm Mg isotopes. To understand the asymptotic behavior (spread) of neutron distribution, we propose to introduce the use of core+n ($$S_{n}S_{2n}$$) description for stable as well as unstable isotopes; $$S_{n}$$ ($$S_{2n}$$) is the one-neutron (two-neutron) separation energy of the considered isotope. The core+n (core+2n) is treated semi-phenomenologically. In this work, the core+n is employed for $$^{25-38}$$\rm Mg isotopes, and is subjected to reproduce the same neutron radius of the given isotope, as we obtained from $$\sigma_{R}$$ calculations. To validate the core+n description, we have revisited the reaction cross sections of $$^{25-38}$$\rm Mg isotopes. The results are found to agree well with the experimental values. Moreover, the core+n neutron distributions clearly demonstrate the one-neutron halo structure of $$^{37}$$\rm Mg. These findings motivated us to use the core+2n description for the neutron distribution of $$^{40}$$\rm Mg in predicting its neutron radius, and $$\sigma_{R}$$ from $$^{12}$$\rm C at 240 and 1000 MeV/nucleon. The trend of the neutron radius and $$\sigma_{R}$$ suggests that $$^{40}$$\rm Mg exhibits two-neutron halo like structure.

Magnesium-40 exists for less than a millisecond, but in that time it manages to display a double neutron halo, a state that never occurs in stable nuclei.

Scientists
Enrico FermiPaul DiracDavid DeutschErwin SchrödingerJohn Stewart BellLouis de Broglie
Concepts
halo nuclei neutron mass charge radius neutron skin nuclear magnetic resonance nuclear reactor carbon 13 deuteron crust NMR spectroscopy neutron star structure solar neutrino neutron star interior structure