Density functional theory provides the most promising, and likely unique, microscopic framework to describe nuclear systems ranging from finite nuclei to neutron stars. Properly optimized energy density functionals define a new paradigm in nuclear theory where predictive capability is possible and uncertainty quantification is demanded. Moreover, density functional theory offers a consistent approach to the linear response of the nuclear ground state. In this paper, we review the fundamental role played by nuclear collective modes in uncovering novel excitations and in guiding the optimization of the density functional. Indeed, without collective excitations the determination of the density functional remains incomplete. Without collective excitations, the equation of state of neutron-rich matter continues to be poorly constrained. We conclude with a discussion of some of the remaining challenges in this field and propose a path forward to address these challenges. PACS Number(s): 21.60.Jz, 24.30.Cz, 21.65.Mn 1541003-1 Int. J. Mod. Phys. E 2015.24. Downloaded from www.worldscientific.com by FLINDERS UNIVERSITY LIBRARY on 10/04/15. For personal use only.
J. PiekarewiczBesides being a fundamental nuclear structure question, its answer is vital to understanding the equation of state (EOS) of infinite nuclear matter. Indeed, the EOS plays a critical role in elucidating the dynamics of heavy ion collisions, the structure of neutron stars and the mechanism of core-collapse supernovae. Nuclear collective excitations, or "giant resonances", encapsulate the dynamic response of the nuclear ground state to external perturbations. As such, they offer a unique view of the nucleus that is often not accessible otherwise. Because of their relevance to the EOS, this paper will be limited to the study of two collective modes: the isoscalar monopole and the isovector dipole resonances. 3 Whereas the former is mostly sensitive to the incompressibility of symmetric nuclear matter, the latter constraints the density dependence of the nuclear symmetry energy. 4 For the possible impact of other nuclear modes on the nuclear EOS see Refs. 5-8. The isoscalar monopole resonance measures the collective response of the nucleus to small density fluctuations. Pictorially, this collective excitation in which protons and neutrons oscillate in phase around the equilibrium density may be perceived as a nuclear "breathing" mode. Given that nuclear matter saturates, the pressure at saturation density vanishes. Thus, the isoscalar monopole resonance probes the curvature of the EOS at saturation density, or equivalently, the incompressibility of symmetric nuclear matter. However, because heavy nuclei are typically neutron rich (e.g., 208 Pb) their monopole response probes the incompressibility of asymmetric matter, which in turn is sensitive to the density dependence of the symmetry energy. 9 Unfortunately, access to the symmetry energy is hindered by the relatively low neutron-proton asymmetry of stable nuclei, so one looks forward to the measurement ...