ar X iv : n uc l - th / 9 80 50 45 v 1 2 3 M ay 1 99 8 1 Structure Effects on Coulomb Dissociation of 8 B

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 1 2 1 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 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 - ex / 9 80 30 12 v 1 2 6 M ar 1 99 8 Measurement of E 2 transitions in the Coulomb dissociation of 8 B

In an effort to understand the implications of Coulomb dissociation experiments for the determination of the 7 Be(p,γ) 8 B reaction rate, longitudinal momentum distributions of 7 Be fragments produced in the Coulomb dissoci-ation of 44 and 81 MeV/nucleon 8 B beams on a Pb target were measured. These distributions are characterized by asymmetries interpreted as the result of interference between...

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...