124 research outputs found

    Quantum Monte Carlo calculations of A=9,10A=9,10 nuclei

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    We report on quantum Monte Carlo calculations of the ground and low-lying excited states of A=9,10A=9,10 nuclei using realistic Hamiltonians containing the Argonne v18v_{18} two-nucleon potential alone or with one of several three-nucleon potentials, including Urbana IX and three of the new Illinois models. The calculations begin with correlated many-body wave functions that have an α\alpha-like core and multiple p-shell nucleons, LSLS-coupled to the appropriate (Jπ;T)(J^{\pi};T) quantum numbers for the state of interest. After optimization, these variational trial functions are used as input to a Green's function Monte Carlo calculation of the energy, using a constrained path algorithm. We find that the Hamiltonians that include Illinois three-nucleon potentials reproduce ten states in 9^9Li, 9^9Be, 10^{10}Be, and 10^{10}B with an rms deviation as little as 900 keV. In particular, we obtain the correct 3+^+ ground state for 10^{10}B, whereas the Argonne v18v_{18} alone or with Urbana IX predicts a 1+^+ ground state. In addition, we calculate isovector and isotensor energy differences, electromagnetic moments, and one- and two-body density distributions.Comment: 28 pages, 12 tables, 7 figure

    Mass splittings of nuclear isotopes in chiral soliton approach

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    The differences of the masses of nuclear isotopes with atomic numbers between \~10 and ~30 can be described within the chiral soliton approach in satisfactory agreement with data. Rescaling of the model is necessary for this purpose - decrease of the Skyrme constant by about 30%, providing the "nuclear variant" of the model. The asymmetric term in Weizsaecker-Bethe- Bacher mass formula for nuclei can be obtained as the isospin dependent quantum correction to the nucleus energy. Some predictions for the binding energies of neutron rich nuclides are made in this way, from, e.g. Be-16 and B-19 to Ne-31 and Na-32. Neutron rich nuclides with high values of isospin are unstable relative to strong interactions. The SK4 (Skyrme) variant of the model, as well as SK6 variant (6-th order term in chiral derivatives in the lagrangian as solitons stabilizer) are considered, and the rational map approximation is used to describe multiskyrmions.Comment: 16 pages, 10 tables, 2 figures. Figures are added and few misprints are removed. Submitted to Phys. Atom. Nucl. (Yad. Fiz.

    Measurement of alpha and neutron decay widths of excited states of C-14

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    The 12C 16O,14O 14C reaction was studied at a beam energy of 234 MeV. The 14O ejectile was detected by a Q3D spectrometer at forward angles. The energies and angles of the excited 14C recoil break up fragments were measured in coincidence with the 14O ejectile using a double sided silicon strip detector array at backward angles. A complete kinematic reconstruction of the reaction was performed to reconstruct the 14C rightarrow 10Be and 14C rightarrow 13 n decay channels and the branching ratios and widths of these decays were calculated. Theoretical decay branches were calculated using barrier penetrability factors and were compared to the measured ratios to provide information on the spins, parities, and configurations of the states. Neutron emission was found to be favored for the 11.73, 12.96, 14.87,16.72, and 18.6 MeV states. The 14.87, 18.6, and 21.4 MeV states were found to have a considerable width for decay and are candidates for the three bodied molecular cluster structure of 14

    6th International School-seminar on Heavy-ion Physics

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