# Free decompression of white dwarf or neutron star matter — what do we end up with?

Suppose that we somehow produced or obtained a small amount of neutron star matter or white dwarf matter compressed to nearly the degeneracy limit and released it into free space uncompressed by gravitational fields or surrounding matter.

That it would explode with nuclear force is well known. What I ask, is, how precisely is it known what it would explode into, and what that would be? Would you get exclusively light nucleii, or heavier ones?

If it is just neutronic matter - i.e. mostly neutrons with a small fraction of protons and electrons to maintain "$$\beta$$ equilibrium", then to first order, all that would happen is the particles would expand very quickly (relativistically) to low densities and the free neutrons would decay into protons, electrons and anti-neutrinos over the course of an hour.
A slow expansion would be more interesting, because you would in a sense be working your way up through density regimes occupied by the neutron star crust. If you could arrange such an expansion, whereby nuclear statistical equilibrium was maintained, then you start with nuclear pasta, move on to very heavy, very neutron-rich nuclei, then lighter (but still $$A>100$$) neutron-rich nuclei and finally end up with "normal" iron-peak nuclei. At the same time, as the material become less neutron-rich it must create lots of anti-neutrinos and electrons.