528 research outputs found

    Investigation of alpha-nuclear potential families from elastic scattering experiments

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    In this work we present the continuation of the reported analysis [1] of the experimentally measured angular distributions of the reaction Cd-106(alpha, alpha)Cd-106 at several different energies around the Coulomb barrier. The difficulties that arise in the study of Cd-106-alpha-nuclear potential and the so called Family Problem are addressed

    Elastic alpha-scattering of 112Sn and 124Sn at astrophysically relevant energies

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    The cross sections for the elastic scattering reactions {112,124}Sn(a,a){112,124}Sn at energies above and below the Coulomb barrier are presented and compared to predictions for global alpha-nucleus potentials. The high precision of the new data allows a study of the global alpha-nucleus potentials at both the proton and neutron-rich sides of an isotopic chain. In addition, local alpha-nucleus potentials have been extracted for both nuclei, and used to reproduce elastic scattering data at higher energies. Predictions from the capture cross section of the reaction 112Sn(a,g)116Te at astrophysically relevant energies are presented and compared to experimental data.Comment: 20 pages, 10 figures, accepted for publication in Phys. Rev.

    Total reaction cross sections from elastic alpha-nucleus scattering angular distributions around the Coulomb barrier

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    The total reaction cross section σreac\sigma_{\rm{reac}} is a valuable measure for the prediction of α\alpha-induced reaction cross sections within the statistical model and for the comparison of scattering of tightly bound projectiles to weakly bound and exotic projectiles. Here we provide the total reaction cross sections σreac\sigma_{\rm{reac}} derived from our previously published angular distributions of α\alpha-elastic scattering on 89^{89}Y, 92^{92}Mo, 112,124^{112,124}Sn, and 144^{144}Sm at energies around the Coulomb barrier.Comment: 4 pages, 2 figures, Phys. Rev. C, accepted as Brief Repor

    High precision 89^{89}Y(α\alpha,α\alpha)89^{89}Y scattering at low energies

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    Elastic scattering cross sections of the 89^{89}Y(α\alpha,α\alpha)89^{89}Y reaction have been measured at energies Ec.m._{c.m.} = 15.51 and 18.63 MeV. The high precision data for the semi-magic N=50N = 50 nucleus 89^{89}Y are used to derive a local potential and to evaluate the predictions of global and regional α\alpha-nucleus potentials. The variation of the elastic alpha scattering cross sections along the N=50N = 50 isotonic chain is investigated by a study of the ratios of angular distributions for 89^{89}Y(α\alpha,α\alpha)89^{89}Y and 92^{92}Mo(α\alpha,α\alpha)92^{92}Mo at Ec.m._{c.m.} \approx 15.51 and 18.63 MeV. This ratio is a very sensitive probe at energies close to the Coulomb barrier, where scattering data alone is usually not enough to characterize the different potentials. Furthermore, α\alpha-cluster states in 93^{93}Nb = 89^{89}Y \otimes α\alpha are investigated

    The 106Cd(α, α)106Cd elastic scattering in a wide energy range for γ process studies

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    Date of Acceptance: 15/04/2015Alpha elastic scattering angular distributions of the 106Cd(α, α)106Cd reaction were measured at three energies around the Coulomb barrier to provide a sensitive test for the α + nucleus optical potential parameter sets. Furthermore, the new high precision angular distributions, together with the data available from the literature were used to study the energy dependence of the locally optimized α + nucleus optical potential in a wide energy region ranging from ELab=27.0MeV down to 16.1 MeV.The potentials under study are a basic prerequisite for the prediction of α-induced reaction cross sections and thus, for the calculation of stellar reaction rates used for the astrophysical γ process. Therefore, statistical model predictions using as input the optical potentials discussed in the present work are compared to the available 106Cd + alpha cross section data.Peer reviewe

    187^{187}Re(\gamm,n) cross section close to and above the neutron threshold

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    The neutron capture cross section of the unstable nucleus 186^{186}Re is studied by investigating the inverse photodisintegration reaction 187^{187}Re(γ\gamma,n). The special interest of the {\it s}-process branching point 186^{186}Re is related to the question of possible {\it s}-process contributions to the abundance of the {\it r}-process chronometer nucleus ^{187}Re.Weusethephotoactivationtechniquetomeasurephotodisintegrationrates.Ourexperimentalresultsareingoodagreementwithtwodifferentstatisticalmodelcalculations.AlthoughthecrosssectionspredictedbybothmodelsfortheinversereactionRe. We use the photoactivation technique to measure photodisintegration rates. Our experimental results are in good agreement with two different statistical model calculations. Although the cross sections predicted by both models for the inverse reaction ^{186}Re(n,Re(n,\gamma)istoolowtoremovetheoverproductionof) is too low to remove the overproduction of ^{186}$Os; the two predicted neutron-capture cross sections differ by a factor of 2.4; this calls for future theoretical study.Comment: Phys. Rev. C, in pres

    Z=50 shell gap near 100^{100}Sn from intermediate-energy Coulomb excitations in even-mass 106112^{106--112}Sn isotopes

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    Rare isotope beams of neutron-deficient 106,108,110^{106,108,110}Sn nuclei from the fragmentation of 124^{124}Xe were employed in an intermediate-energy Coulomb excitation experiment yielding B(E2,01+21+)B(E2, 0^+_1 \to 2^+_1) transition strengths. The results indicate that these B(E2,01+21+)B(E2,0^+_1 \to 2^+_1) values are much larger than predicted by current state-of-the-art shell model calculations. This discrepancy can be explained if protons from within the Z = 50 shell are contributing to the structure of low-energy excited states in this region. Such contributions imply a breaking of the doubly-magic 100^{100}Sn core in the light Sn isotopes.Comment: 4 pages, 4 figure

    TOF-Brho Mass Measurements of Very Exotic Nuclides for Astrophysical Calculations at the NSCL

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    Atomic masses play a crucial role in many nuclear astrophysics calculations. The lack of experimental values for relevant exotic nuclides triggered a rapid development of new mass measurement devices around the world. The Time-of-Flight (TOF) mass measurements offer a complementary technique to the most precise one, Penning trap measurements, the latter being limited by the rate and half-lives of the ions of interest. The NSCL facility provides a well-suited infrastructure for TOF mass measurements of very exotic nuclei. At this facility, we have recently implemented a TOF-Brho technique and performed mass measurements of neutron-rich nuclides in the Fe region, important for r-process calculations and for calculations of processes occurring in the crust of accreting neutron stars.Comment: 8 pages, 4 figures, submitted to Journal of Physics G, proceedings of Nuclear Physics in Astrophysics II

    Determining the 7Li(n,gamma) cross section via Coulomb dissociation of 8Li

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    The applicability of Coulomb dissociation reactions to determine the cross section for the inverse neutron capture reaction was explored using the reaction 8Li(gamma,n)7Li. A 69.5 MeV/nucleon 8Li beam was incident on a Pb target, and the outgoing neutron and 7Li nucleus were measured in coincidence. The deduced (n,gamma) excitation function is consistent with data for the direct capture reaction 7Li(n,gamma)8Li and with low-energy effective field theory calculations.Comment: Accepted for publication in Phys. Rev.
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