Dynamic polarization in the Coulomb breakup of loosely bound 17F

Liang, J. F.; Beene, J. R.; Caraley, A. L.; Esbensen, H.; Galindo-Uribarri, A.; Gross, C. J.; Mueller, P. E.; Schmitt, K. T.; Shapira, D.; Stracener, D. W.; Varner, R. L.

doi:10.1016/j.physletb.2009.09.055

Cited by 29 publications

(66 citation statements)

References 27 publications

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“…42 (top panel) along with the predictions of the MCDCC model [226], described in the previous section. Calculations with the São Paulo potential [33], using default parameters, provided a good description of the data [220]. Figure 42 also includes older data for the same system, not only at 170 MeV (top panel) but also at 98 MeV (middle panel) and 90.4 MeV (bottom panel).…”

Section: 13mentioning

confidence: 93%

“…[220]. A 17 F beam of ∼ 8 × 10 6 pps was produced by the 16 O(d, n) reaction at the HRIBF facility (Oak Ridge, TN, USA), bombarding a 1.0 mg/cm 2 58 Ni target.…”

Section: 12mentioning

confidence: 99%

“…Other reactions measured in ref. [220] will also be discussed later: quasielastic scattering of 17 [221]. The maximum excitation energy and the number of discrete bins in the continuum were dictated by convergence of the calculated observables.…”

Section: 12mentioning

confidence: 99%

“…A 1.84 mg/cm 2 lead target was also used in the experiment of ref. [220] which was described at the beginning of sect. 17.1.2, so a quasielastic-scattering angular distribution for 17 F + 208 Pb at 170 MeV also was obtained.…”

Section: 13mentioning

confidence: 99%

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Elastic scattering, fusion, and breakup of light exotic nuclei

2016

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Abstract. The present status of fusion reactions involving light (A < 20) radioactive projectiles at energies around the Coulomb barrier (E < 10 MeV per nucleon) is reviewed, emphasizing measurements made within the last decade. Data on elastic scattering (providing total reaction cross section information) and breakup channels for the involved systems, demonstrating the relationship between these and the fusion channel, are also reviewed. Similarities and differences in the behavior of fusion and total reaction cross section data concerning halo nuclei, weakly-bound but less exotic projectiles, and strongly-bound systems are discussed. One difference in the behavior of fusion excitation functions near the Coulomb barrier seems to emerge between neutron-halo and proton-halo systems. The role of charge has been investigated by comparing the fusion excitation functions, properly scaled, for different neutron-and proton-rich systems. Possible physical explanations for the observed differences are also reviewed.

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Section: 13mentioning

confidence: 93%

“…[220]. A 17 F beam of ∼ 8 × 10 6 pps was produced by the 16 O(d, n) reaction at the HRIBF facility (Oak Ridge, TN, USA), bombarding a 1.0 mg/cm 2 58 Ni target.…”

Section: 12mentioning

confidence: 99%

Section: 12mentioning

confidence: 99%

Section: 13mentioning

confidence: 99%

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Elastic scattering, fusion, and breakup of light exotic nuclei

2016

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“…Such nuclei are unstable by beta emission or electron capture, with relatively long lifetimes (milliseconds up to seconds), sufficient to produce a secondary beam. Light exotic nuclei usually present a pronounced cluster structure, with very low separation energies in comparison to their stable partners and can be found either in the neutron rich [9][10][11][12][13][14][15][16][17][18] or in the proton rich sides [19][20][21][22][23][24] of the nuclear chart. One of these nuclei is 8 B which is formed by a 7 Be core plus one proton bound by only 0.137 MeV to the core.…”

Section: Introductionmentioning

confidence: 99%

B8+Al27 scattering at low energies

et al. 2017

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We present 8 B+ 27 Al elastic scattering angular distributions for the proton-halo nucleus 8 B at two energies above the Coulomb barrier, namely E lab = 15.3 MeV and 21.7 MeV. The experiments have been performed in the Radioactive Ion Beams in Brasil facility (RIBRAS) in São Paulo, and in the TwinSol facility at the University of Notre Dame, USA. The angular distributions were measured in the angular range of 15-80 degrees. Optical model and Continuum Discretized Coupled Channels calculations have been performed and the total reaction cross sections have been derived. A comparison of the 8 B+ 27 Al total reaction cross sections with similar systems including exotic, weakly and tightly bound projectiles impinging on the same target is presented.

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