Scattering of α particles on 11B nuclei at energies 40 and 50 MeV

Burtebaev, N.; Baktybayev, M. K.; Duisebaev, B. A.; Peterson, R.J.; Sakuta, S.B.

doi:10.1134/1.2011493

Cited by 15 publications

(14 citation statements)

References 21 publications

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“…The analysis of alpha elastically scattered by 11 B at energies 29-65MeV [60][61][62][63] has been performed phenomenologically using (CRC) and semimicroscopically (CM). The effect of inelastic and 7 Li transfer has been studied as shown in Fig.…”

Section: Alpha Elastically Scattered On 11 Bmentioning

confidence: 99%

Applying Crystal model on different nuclear systems; deuteron, alpha and 6Li as projectiles

Amar

2022

Arab Journal of Nuclear Sciences and Applications

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Section: Alpha Elastically Scattered On 11 Bmentioning

confidence: 99%

Applying Crystal model on different nuclear systems; deuteron, alpha and 6Li as projectiles

Amar

2022

Arab Journal of Nuclear Sciences and Applications

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“…The analysis of the experimental data for alpha elastically scattered by 11 B at 29-54 MeV [39][40][41][42] has been achieved in CRC and CM frameworks. CRC analysis of the experimental data was performed using WS forms for the real and imaginary parts of the potential.…”

Section: Alpha Elastically Scattered By 11 Bmentioning

confidence: 99%

“…The energy dependences of the real volume and imaginary volume integrals are presented in Fig7. The experimental data were taken from [39][40][41][42].…”

Section: Alpha Elastically Scattered By 11 Bmentioning

confidence: 99%

Analysis of Alpha Elastically Scattered by Light Nuclei Using Crystalline Model Approach

Amar

2021

Arab Journal of Nuclear Sciences and Applications

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Elastic scattering of alpha particles by light nuclei is achieved using coupled reaction channel (CRC) and crystaline model approach (CM) to compare and reanalyze the availability of applying novel ideas in the nuclear reaction field. Coupled reaction channel (CRC) and crystal model (CM) have been used on alpha elastically scattered by 6,7 Li, 9 Be, and 11 B, where alpha-target interaction has been modified. The real part of the potential has been selected as crystal model (CM) with a Gaussian form. The imaginary part of the potential was taken in Woods-Saxon form, where the spin-orbit effect has been excluded from this analysis. Fitting of experimental data obtained using CRC and CM agreed well for alpha elastically scattered by 6,7 Li and 9 Be, whereas results obtained for 11 B using CM were poor. More modifications should be made on CM to reproduce the differential cross-section for alpha elastically scattered by 11 B .

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“…The analysis of elastic and inelastic α+ 11 B scattering, with excitations of 11 В nucleus was studied in few works through the last four decades [12][13][14][15]. Denisov et al [12] investigated the scattering of 24 MeV α particles by 10,11 B.…”

Section: Introductionmentioning

confidence: 99%

Analysis of α+¹¹B elastic and inelastic scattering using microscopic and semi-microscopic representations

Mokhtar¹,

Ebrahim²,

Ahmed³

et al. 2020

Phys. Scr.

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In the present study angular distributions of the differential cross section for elastic and inelastic scattering of alpha (α)-particles of 11В nuclei at different bombarding energies have been analyzed in the framework of the optical model (OM) potential. Two OM folding approaches were adopted in order to construct the real part of the α-nucleus potential. First, we generated the semi-microscopic single folding (SF) potential by folding an effective α-nucleon (α-N) interaction over the nuclear matter density of the target (11B) nucleus. In addition, the double folding (DF) approach was employed in order to deduce a microscopic representation of the optical potential by folding an effective density-dependent (DDM3Y) nucleon–nucleon interaction over the matter densities of the colliding nuclei. Successful theoretical predictions of six sets of experimental elastic scattering data have been obtained over the whole measured angular range. However, it was found that introducing real renormalization coefficients (∼0.9–1.6) is essential in order to obtain best fits with data. On the other side, sixteen sets of the inelastic scattering data at several excited states of 11B nucleus were analyzed using the constructed SF and DF deformed potentials. In general, reasonable description of the data is obtained. However underestimated predictions of data were obtained at backward measured angles. The deduced reaction (absorption) cross sections and nuclear deformation lengths were also investigated.

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Scattering of α particles on 11B nuclei at energies 40 and 50 MeV

Cited by 15 publications

References 21 publications

Applying Crystal model on different nuclear systems; deuteron, alpha and 6Li as projectiles

Applying Crystal model on different nuclear systems; deuteron, alpha and 6Li as projectiles

Analysis of Alpha Elastically Scattered by Light Nuclei Using Crystalline Model Approach

Analysis of α+¹¹B elastic and inelastic scattering using microscopic and semi-microscopic representations

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Scattering of α particles on 11B nuclei at energies 40 and 50 MeV

Cited by 15 publications

References 21 publications

Applying Crystal model on different nuclear systems; deuteron, alpha and 6Li as projectiles

Applying Crystal model on different nuclear systems; deuteron, alpha and 6Li as projectiles

Analysis of Alpha Elastically Scattered by Light Nuclei Using Crystalline Model Approach

Analysis of α+11B elastic and inelastic scattering using microscopic and semi-microscopic representations

Contact Info

Product

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Analysis of α+¹¹B elastic and inelastic scattering using microscopic and semi-microscopic representations