This contribution reviews the present status on the available constraints to the nuclear
equation of state (EoS) around saturation density from nuclear structure calculations on …

The compression-mode giant resonances, namely the isoscalar giant monopole and
isoscalar giant dipole modes, are examples of collective nuclear motion. Their main interest …

We present results of centroid energies ECEN, of the isoscalar (T= 0) and isovector (T= 1)
giant resonances of multipolarities L= 0–3 in 40, 48Ca, 68Ni, 90Zr, 116Sn, 144Sm, and …

Abstract “Why are the tin isotopes soft?” has remained, for the past decade, an open
problem in nuclear structure physics: models which reproduce the isoscalar giant monopole …

Background: Two recent studies of the evolution of the isoscalar giant monopole resonance
(ISGMR) within the calcium isotope chain report conflicting results. One study suggests that …

Recent data on isoscalar giant monopole resonance (ISGMR) in the calcium isotopes 40,
44, 48 Ca have suggested that K τ, the asymmetry term in the nuclear incompressibility, has …

The recent RCNP (α, α′) data on the Isoscalar Giant Monopole Resonance (ISGMR) and
Isoscalar Giant Quadrupole Resonance (ISGQR) in 92, 94, 96, 98,100 Mo are analyzed …

Abstract “Background-free” spectra of inelastic α-particle scattering have been measured at
a beam energy of 385 MeV in 90, 92 Zr and 92 Mo at extremely forward angles, including 0° …

The isoscalar giant monopole, dipole, and quadrupole strength distributions have been
deduced in Zr 90, 92 and Mo 92 from “background-free” spectra of inelastic α-particle …

Isoscalar giant resonances in Zr 90, 92, 94 have been studied with inelastic scattering of 240
MeV α particles at small angles including 0∘. A significant fraction of the energy-weighted …