Microscopic model analyses of proton scattering from 12C, 20Ne, 24Mg, 28Si and 40Ca

Kim, Y.J.; Amos, K.; Karataglidis, S.; Richter, W. A.

doi:10.1016/j.nuclphysa.2008.04.006

Cited by 9 publications

(4 citation statements)

References 38 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…137. Here, to describe the ground-state structure of the nuclei under consideration, the shell-model and the Skyrme-Hartree-Fock approximation were used.…”

Section: -38mentioning

confidence: 99%

See 1 more Smart Citation

Intermediate energy multiple scattering of particles by light α-cluster nuclei

Berezhnoy

Mikhailyuk

Pilipenko

2015

Int. J. Mod. Phys. E

View full text Add to dashboard Cite

The survey of cluster models used for the description of the properties of nuclei was carried out. The interaction of intermediate protons with various odd and even nuclei is reviewed. The influence of the clusterization effects on the behavior of the elastic and inelastic scattering observables are demonstrated by using multiple diffraction scattering theory (MDST) and the α-cluster model with dispersion. The comparison of the calculations, based on two-and four-nucleon correlation models, have been performed. The elastic scattering of light nuclei from α-cluster nuclei is analyzed. The results given in this review suggest that the MDST variants based on cluster models seem to be rather attractive as compared with those based on the single-nucleon approximation. Such approaches, considering nucleon and light-nuclei scattering on α-clusters, are among the best examples of using Glauber's MDST, since they automatically include the internal nucleon-nucleon correlations both in the incident and target nuclei. Besides, α-clusters have zero spin and, in this case, the scattering amplitude does not involve explicit consideration of spin-spin effects. Moreover, these models often permit an accurate analytical calculation of the MDST series.

show abstract

“…137. Here, to describe the ground-state structure of the nuclei under consideration, the shell-model and the Skyrme-Hartree-Fock approximation were used.…”

Section: -38mentioning

confidence: 99%

“…In particular, in Ref. 137, the elastic p-12 C and p- 24 Mg scattering at 200 MeV and 250 MeV was considered. The p-12 C and p- 24 Mg differential cross-sections calculated in this approach are in agreement with the existing experimental data.…”

Section: -38mentioning

confidence: 99%

Intermediate energy multiple scattering of particles by light α-cluster nuclei

Berezhnoy

Mikhailyuk

Pilipenko

2015

Int. J. Mod. Phys. E

View full text Add to dashboard Cite

show abstract

“…The numerical techniques necessary to solve the Schrödinger equation with these finite electromagnetic potentials are explained in chapter 3, equation (3.28) of [24]. The solutions of U l from equation (18) are introduced in the S matrix equation (10.58) of [24], which is,…”

Section: The Schrödinger Equation With Finite Electromagnetic Potentialsmentioning

confidence: 99%

“…Recently results have been obtained at low energies for the reaction + p p [11][12][13][14][15], 3 He, 20 Ne, 40 Ar, 14 N [16], p+ 12 C [17,18], and for p+ 3 He [12,[18][19][20]. We compare ours results for the reaction − e + ( 3 He, 20 Ne, 40 Ar, 14 N ), n+ ( 12 C, 208 Pb), and p+ 12 C to show that these potentials obtained from extra-dimensions are compared with known experimental data and to set bound on the scale of the scenarios.…”

Section: Introductionmentioning

confidence: 99%

Elastic cross sections in an RSIIpscenario

Arceo¹,

Pedraza²,

González-Espinosa³

et al. 2014

J. Phys. G: Nucl. Part. Phys.

View full text Add to dashboard Cite

The elastic differential cross section is calculated at low energies (below 100 MeV) for the elements 3He, 20Ne, 40Ar, 14N, 12C, and for the 208Pb using a finite electromagnetic potential, which is obtained by considering a Randall–Sundrum II scenario modified by the inclusion of p compact extra-dimensions. The length scale is adjusted in the potential to compare with known experimental data and to set bounds for the parameter of the model. The effective four-dimensional (4D) electromagnetic potential is produced by a point charge, as seen from the three-brane that contains it, in uniform motion in an RSIIp scenario.

show abstract