Shell-model studies relevant for the low-energy Coulomb excitation in Zn isotopesSpringer Science and Business Media LLC - Tập 59 - Trang 1-13 - 2023
I. Ahmed, R. Kumar, K. Hadyńska-Klȩk, C. Qi
The low-lying nuclear structure of even-even Zn isotopes ranging from
$$^{62}$$
Zn to
$$^{70}$$
Zn has been comprehensively examined through large scale shell model calculations. These calculations ...... hiện toàn bộ
PrefaceSpringer Science and Business Media LLC - - 2005
C. J. Gross, W. Nazarewicz, K. P. Rykaczewski
Energies and radii of light nuclei around unitaritySpringer Science and Business Media LLC - Tập 56 - Trang 1-15 - 2020
Sebastian König
Light nuclei fall within a regime of universal physics governed by the fact that the two-nucleon scattering lengths are large compared to the typical nuclear interaction range set by one-pion exchange. This places nuclear physics near the so-called unitarity limit in which the scattering lengths are exactly infinite. Effective field theory provides a powerful theoretical framework to capture this ...... hiện toàn bộ
Hadron production in elementary nucleon–nucleon reactions from low to ultra-relativistic energiesSpringer Science and Business Media LLC - Tập 56 - Trang 1-19 - 2020
V. Kireyeu, I. Grishmanovskii, V. Kolesnikov, V. Voronyuk, E. Bratkovskaya
We study the hadron production in
$$p+p$$
,
$$p+n$$
and
$$n+n$$
reactions within the microscopic Parton–Hadron-Dynamics (PHSD) transport approach in comparison to PYTHIA 8.2. We discuss the details of the “PHSD tune” of the Lund string model (realized by event generators FRITIOF and PYTHIA) in the vacuum (as in
$$N+N$$
collisions) as well as its in-medium modifications relevant for heav...... hiện toàn bộ
Absolute E1 and E2 transition rates in 110CdSpringer Science and Business Media LLC - Tập 2 - Trang 269-273 - 1998
L.K. Kostov, W. Andrejtscheff, L.G. Kostova, L. Käubler, H. Prade, R. Schwengner
The lifetimes of several states in 110Cd have been determined by means of the generalized centroid-shift method. The reaction 108Pd(α,2n) has been used and the following results were obtained: T1/2(2879 keV) = 0.60 ± 0.10 ns, T1/2(3029 keV) = 0.30 ± 0.10 ns, T1/2(3056 keV) = 2.25 ± 0.10 ns, T1/2(3611 keV) = 0.45 ± 0.10 ns. Electric dipole and quadrupole transitions are discussed in terms of octup...... hiện toàn bộ