X iv : n uc l - th / 9 80 50 15 v 1 6 M ay 1 99 8 Pairing and symmetry energy in N ≃ Z nuclei

X iv : n uc l - th / 9 80 50 07 v 1 4 M ay 1 99 8 Neutrino capture by r - process waiting - point nuclei

We use the Quasiparticle Random Phase Approximation to include the effects of low-lying Gamow-Teller and first forbidden strength in neutrino capture by very neutron-rich nuclei with N = 50, 82, or 126. For electron neutrinos in what is currently considered the most likely r-process site the capture cross sections are two or more times previous estimates. We briefly discuss the reliability of o...

ar X iv : n uc l - th / 9 90 60 01 v 2 3 J un 1 99 9 February 9 , 2008 Proton - neutron interactions in N ≈ Z nuclei

Proton-neutron (p − n) interactions and their various aspects in N ≈ Z nuclei of g 9/2-and f 7/2 subshell are studied using a schematic model interaction with four force parameters proposed recently. It is shown that the model interaction well reproduces observed physical quantities: the double differences of binding energies, symmetry energy, Wigner energy, odd-even mass difference and separat...

ar X iv : n uc l - th / 9 80 50 53 v 1 2 9 M ay 1 99 8 g - factor of a tightly bound electron

We study the hyperfine splitting of an electron in hydrogen-like 209 Bi 82+. It is found that the hfs energy splitting can be explained well by considering the g-factor reduction due to the binding effect of a bound electron. We determine for the first time the experimental value of the magnetic moment of a tightly bound electron.

ar X iv : n uc l - th / 9 90 50 49 v 2 2 6 M ay 1 99 9 η - and η ′ - meson production in the reaction pn → dM near threshold

ar X iv : n uc l - th / 9 90 50 49 v 1 2 1 M ay 1 99 9 η - and η ′ - meson production in the reaction pn → dM near threshold