2014
DOI: 10.1103/physrevc.90.034604
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Surface-integral formalism of deuteron stripping

Abstract: The purpose of this paper is to develop an alternative theory of deuteron stripping to resonance states based on the surface integral formalism of Kadyrov et al. [Ann. Phys. 324, 1516] and continuum-discretized coupled channels (CDCC). First we demonstrate how the surface integral formalism works in the three-body model and then we consider a more realistic problem in which a composite structure of target nuclei is taken via optical potentials. We explore different choices of channel wave functions and transit… Show more

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Cited by 14 publications
(9 citation statements)
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“…In Refs. [2,3], a generalized R-matrix approach was developed within the surface integral formalism [4]. The approach uses distorted waves in both initial and final states (see Eq.…”
Section: Introductionmentioning
confidence: 99%
“…In Refs. [2,3], a generalized R-matrix approach was developed within the surface integral formalism [4]. The approach uses distorted waves in both initial and final states (see Eq.…”
Section: Introductionmentioning
confidence: 99%
“…Faddeev calculations for (d,p) on heavy nuclei are not possible due to the difficulty of handling the Coulomb interaction. It has thus become clear to the TORUS collaboration that indeed a new formalism [14], more efficient at handling the three-body equations, which provides stable solutions for a wide variety of cases, including a wide range of relevant beam energies (5-50 MeV/u), light and heavy systems, well bound and loosely bound nuclei, is absolutely necessary in the field.…”
Section: Discussionmentioning
confidence: 99%
“…With the techniques of [3], reactions on heavy systems are not accessible. A new technique to handle Coulomb is being proposed within the scope of the TORUS collaboration [14].…”
Section: Looking At Breakup In More Detailmentioning
confidence: 99%
“…The two-body transition operator t ν for each interacting pair with inter-potential v ν is determined from the Lippmann-Schwinger equation t ν = v ν + v ν G 0 t ν . Additional approximations are often necessary and the correct treatment of the Coulomb interaction poses a major difficulty to solve the AGS set of equations [27]. One can treat the Coulomb interaction with help of screened Coulomb potentials, but this method works only for light nuclei since wild oscillations in the asymptotic region jeopardizes the accuracy of the solutions [28].…”
Section: (Dp) and Charge-exchange Reactionsmentioning
confidence: 99%

Indirect methods in nuclear astrophysics

Bertulani,
Mukhamedzhanov,
Kadyrov
et al. 2015
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