Scattering of Protons by Deuterons

Sherr, R.; Blair, J. M.; Kratz, H.R.; Bailey, Carl L.; Taschek, R. F.

doi:10.1103/physrev.72.662

Cited by 64 publications

(15 citation statements)

References 9 publications

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“…The central part of the entrance potentials for α-p and d-p has been derived as previously [27] from empirical p-α and p-d potentials by means of a single-folding method. The empirical potentials were obtained from p + d and p + α elastic-scattering studies at E = 2.52-5 MeV/u measured previously [40][41][42][43][44][45][46]. These p + d and p + α elastic-scattering data were fitted by simple Woods-Saxon form factors for both real volume and imaginary volume parts for the p + α system and a real volume and a surface imaginary term for the p + d system.…”

mentioning

confidence: 99%

Reexamination ofLi6+pelastic scattering in inverse kinematics

Soukeras¹,

Pakou²,

Cappuzzello³

et al. 2015

Phys. Rev. C

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mentioning

confidence: 99%

Reexamination ofLi6+pelastic scattering in inverse kinematics

Soukeras¹,

Pakou²,

Cappuzzello³

et al. 2015

Phys. Rev. C

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“…The data are taken from Refs. [29,30,31,32,33,34], as indicated in detail in the figure captions. By inspection of the figures, we can observe that: (i) theory and experiment are in disagreement for the A y and iT 11 Exp.…”

Section: Resultsmentioning

confidence: 99%

N−delastic scattering using the hyperspherical harmonics approach with realistic local and nonlocal interactions

et al. 2009

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The application of the hyperspherical harmonic approach to the case of the N − d scattering problem below deuteron breakup threshold is described. The nuclear Hamiltonian includes twoand three-nucleon interactions, in particular the Argonne v 18 , the N3LO-Idaho, and the V low−k two-nucleon, and the Urbana IX and N2LO three-nucleon interactions. Some of these models are local, some are non-local. Also electromagnetic effects are included. Accurate calculations for many scattering observables at various center-of-mass energies are performed and the results are compared with the available experimental data. Furthermore, a χ 2 analysis of some of the Hamiltonian models has been performed to compare their capability to describe the scattering process.

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“…If Eq. (47) is rewritten as follows: (49) then, it is seen that upon "switching off" nuclear inter actions between particle 1 and two others (i.e., at V 12 = V 31 = 0) the solution to the following equation (50) will be given by the function Ψ = χ (23) . This is also seen from initial equations (39) and (40), because here we have:…”

Section: Reformulation Of Equations Of Motionmentioning

confidence: 99%

Faddeev equations and the method of hyperspherical harmonics in the problem of three-nucleon continuum

Kovalchuk

Kozlovskii

2012

Phys. Part. Nuclei

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A method for solving the Faddeev equations in configuration space is developed for a three nucleon system in the continuum by using the decomposition over a hyperspherical basis. The wave functions of Nd system, phase shifts, and cross sections of Nd scattering at subthreshold energies are calculated. Also, within the framework of this method, one dimensional integral equations are formulated for the problem of infinite motion of all three strongly interacting particles, and the Faddeev equations for a system of three had rons with Coulomb interaction in the continuum are modified. Similar methods of investigation of three par ticle systems are reviewed.

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Scattering of Protons by Deuterons

Cited by 64 publications

References 9 publications

Reexamination ofLi6+pelastic scattering in inverse kinematics

Reexamination ofLi6+pelastic scattering in inverse kinematics

N−delastic scattering using the hyperspherical harmonics approach with realistic local and nonlocal interactions

Faddeev equations and the method of hyperspherical harmonics in the problem of three-nucleon continuum

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