Supplemental Material for “In search of beyond mean-field signatures in heavy-ion fusion reactions”

R. T. deSouza 0000-0001-5835-677X [email protected] Department of Chemistry and Center for Exploration of Energy and Matter, Indiana University, Bloomington, Indiana 47408, USA K. Godbey 0000-0003-0622-3646 [email protected] FRIB Laboratory, Michigan State University, East Lansing, Michigan 48824, USA S. Hudan 0000-0002-9722-2245 [email protected] Department of Chemistry and Center for Exploration of Energy and Matter, Indiana University Bloomington, Indiana 47408, USA W. Nazarewicz 0000-0002-8084-7425 [email protected] Department of Physics and Astronomy and FRIB Laboratory, Michigan State University, East Lansing, Michigan 48824, USA

Abstract

This supplemental material contains 2 illustrative videos of TDHF simulations and one supplemental figure.

S.I Animations of TDHF simulations

Video 1: Time evolution of the neutron localization function for the collision of ^16,17O + ¹²C at $E_{\rm c.m.}$ = 14 MeV and the incoming angular momentum $\ell=0\hbar$ as predicted by TDHF calculations.

Video 2: Time evolution of the neutron localization function for the collision of ^16,17O + ¹²C at $E_{\rm c.m.}$ = 14 MeV and the incoming angular momentum $\ell=11\hbar$ as predicted by TDHF calculations.

S.II DC-TDHF isovector potential

Refer to caption — Figure S1: The isovector part of the DC-TDHF potential for the ^16,17,18O $+^{12}$ C reactions discussed in the main text. For ¹⁷O, 200 random initial orientations of the deformed projectile were considered and are plotted as the light grey lines.