Analyzing power of the reaction 12C(d, p) leading to bound and unbound states in 13C

Lang, J.; Liechti, J.; Müller, R.; Schmelzbach, P.A.; Smyrski, J.; Godlewski, M.; Jarczyk, L.; Strałkowski, A.; Witała, H.

doi:10.1016/0375-9474(88)90361-2

Cited by 8 publications

(3 citation statements)

References 18 publications

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“…> 90 • . This discrepancy is comparable with the one in the 12 C(d, p) 13 C reaction [26], displayed in Fig. 4.…”

Section: Resultssupporting

confidence: 88%

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Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Deltuva

2015

Phys. Rev. C

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Exact Faddeev-type three-body equations are applied to the study of the proton transfer reactions (d, n) in the system consisting of a nuclear core and two nucleons. The integral equations for the three-body transition operators are solved in the momentum-space framework including the Coulomb interaction via the screening and renormalization method. For a weakly bound final nucleus the calculation of the (d, n) reaction is more demanding in terms of the screening radius as compared to the (d, p) reaction. Well converged differential cross section results are obtained for 7 Be(d, n) 8 B, 12 C(d, n) 13 N, and 16 O(d, n) 17 F reactions. A comparison with the corresponding (d, p) reactions is made. The calculations fail to reproduce the shape of the angular distribution for reactions on 12 C but provide quite successful description for reactions on 16 O, especially for the transfer to the 17 F excited state 1/2 + when using a nonlocal optical potential.

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“…> 90 • . This discrepancy is comparable with the one in the 12 C(d, p) 13 C reaction [26], displayed in Fig. 4.…”

Section: Resultssupporting

confidence: 88%

“…For all of them the angular shape fails in accounting 3, and the experimental data are from Ref. [26].…”

Section: Resultsmentioning

confidence: 99%

Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Deltuva

2015

Phys. Rev. C

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“…Nucleon transfer from the deuteron to a target nucleus leads to the formation of a recoiling residual nucleus in either the ground state or a low-lying excited state; a nucleon of the conjugate species is emitted. This interaction mechanism leads to a series of discrete sharp peaks in the energy spectrum of the emitted nucleon [6]. The positions of these peaks closely follow the excitation-energy spectrum of the residual nucleus.…”

Section: Introductionmentioning

confidence: 84%

Towards an effective model for (d,p) and (d,n) nucleon-transfer reactions to bound states for FLUKA

Salvat–Pujol

Ferrari²

2020

EPJ Web Conf.

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A general overview is presented of an effective model for the inclusion of (d,p) and (d,n) nucleon transfer direct reactions to bound states of the residual nucleus in the general-purpose radiation-transport code FLUKA. The model relies on the distorted-wave Born approximation, employing state-of-the-art subroutines for the numerical solution of the radial Schrödinger equation for the deuteron- and nucleon-nucleus wave-functions, as well as contemporary optical potential models for the latter two. A final variation of a handful of deuteron optical potential parameters provides the model with additional flexibility and enhances the agreement with experimental nucleon angular distributions in a considerable range of target nuclei and deuteron energies.

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Energy Levels of Light Nuclei A=13

Kelley,

Sheu,

Purcell

2024

Nuclear Data Sheets

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Analyzing power of the reaction 12C(d, p) leading to bound and unbound states in 13C

Cited by 8 publications

References 18 publications

Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Faddeev-type calculation of(d,n)transfer reactions in three-body nuclear systems

Towards an effective model for (d,p) and (d,n) nucleon-transfer reactions to bound states for FLUKA

Energy Levels of Light Nuclei A=13

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