Nuclear “pasta” formation

AS Schneider, CJ Horowitz, J Hughto, DK Berry - Physical Review C—Nuclear …, 2013 - APS
Physical Review C—Nuclear Physics, 2013APS
The formation of complex nonuniform phases of nuclear matter, known as nuclear pasta, is
studied with molecular dynamics (MD) simulations containing 51200 nucleons. A
phenomenological nuclear interaction is used that reproduces the saturation binding energy
and density of nuclear matter. Systems are prepared at an initial density of 0.10 fm− 3 and
then the density is decreased by expanding the simulation volume at different rates to
densities of 0.01 fm− 3 or less. An originally uniform system of nuclear matter is observed to …
The formation of complex nonuniform phases of nuclear matter, known as nuclear pasta, is studied with molecular dynamics (MD) simulations containing 51200 nucleons. A phenomenological nuclear interaction is used that reproduces the saturation binding energy and density of nuclear matter. Systems are prepared at an initial density of and then the density is decreased by expanding the simulation volume at different rates to densities of or less. An originally uniform system of nuclear matter is observed to form spherical bubbles (“swiss cheese”), hollow tubes, flat plates (“lasagna”), thin rods (“spaghetti”) and, finally, nearly spherical nuclei with decreasing density. We explicitly observe nucleation mechanisms, with decreasing density, for these different pasta phase transitions. Topological quantities known as Minkowski functionals are obtained to characterize the pasta shapes. Different pasta shapes are observed depending on the expansion rate. This indicates nonequilibrium effects. We use this to determine the best ways to obtain lower energy states of the pasta system from MD simulations and to place constraints on the equilibration time of the system.
American Physical Society