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1.
Phys Rev Lett ; 111(8): 082701, 2013 Aug 23.
Article in English | MEDLINE | ID: mdl-24010432

ABSTRACT

We propose an extension of the continuum discretized coupled channels (CDCC) method, where the projectile is described by a microscopic cluster model. This microscopic generalization (MCDCC) relies only on nucleon-target interactions, and therefore presents an important predictive power. Core excitations can be included without any further parameter. As an example, we investigate the 7Li+208Pb elastic scattering at Elab=27 and 35 MeV. The 7Li nucleus is known to present an α+t cluster structure, and is well described by the resonating group method. An excellent agreement is obtained for the 7Li+208Pb elastic cross sections, provided that breakup channels are properly included. We also present an application to inelastic scattering and discuss future applications of the MCDCC.

2.
Phys Rev Lett ; 107(13): 132502, 2011 Sep 23.
Article in English | MEDLINE | ID: mdl-22026847

ABSTRACT

The (2)H(d,p)(3)H, (2)H(d,n)(3)He, and (2)H(d,γ)(4)He reactions are studied at low energies in a multichannel ab initio model that takes into account the distortions of the nuclei. The internal wave functions of these nuclei are given by the stochastic variational method with the AV8' realistic interaction and a phenomenological three-body force included to reproduce the two-body thresholds. The obtained astrophysical S factors are all in very good agreement with the experiment. The most important channels for both transfer and radiative capture are identified by comparing to calculations with an effective central force. They are all found to dominate thanks to the tensor force.

3.
Phys Rev Lett ; 96(16): 162501, 2006 Apr 28.
Article in English | MEDLINE | ID: mdl-16712219

ABSTRACT

The low-energy reaction 14C(n,gamma)15C provides a rare opportunity to test indirect methods for the determination of neutron capture cross sections by radioactive isotopes versus direct measurements. It is also important for various astrophysical scenarios. Currently, puzzling disagreements exist between the 14C(n,gamma)15C cross sections measured directly, determined indirectly, and calculated theoretically. To solve this puzzle, we offer a strong test based on a novel idea that the amplitudes for the virtual 15C-->14C + n and the real 15F -->14O + p decays are related. Our study of this relation, performed in a microscopic model, shows that existing direct and some indirect measurements strongly contradict charge symmetry in the 15C and 15F mirror pair. This brings into question the experimental determinations of the astrophysically important (n,gamma) cross sections for short-lived radioactive targets.

4.
Phys Rev Lett ; 87(4): 042501, 2001 Jul 23.
Article in English | MEDLINE | ID: mdl-11461610

ABSTRACT

Radiative capture of protons is investigated as a probe of clustering in nuclei far from stability. The first such measurement on a halo nucleus is reported here for the reaction 6He(p,gamma) at 40 MeV. Capture into 7Li is observed as the strongest channel. In addition, events have been recorded that may be described by quasifree capture on a halo neutron, the alpha core, and 5He. The possibility of describing such events by capture into the continuum of 7Li is also discussed.

5.
Phys Rev Lett ; 85(7): 1404-7, 2000 Aug 14.
Article in English | MEDLINE | ID: mdl-10970515

ABSTRACT

Photons originating from coherent bremsstrahlung have been measured over a large dynamic range for the reaction of 200 MeV alpha particles with protons. At low photon energies the bremsstrahlung spectrum exhibits the classical behavior with an approximate 1/E(gamma) shape. At higher photon energies there is a pronounced contribution from capture into the unbound ground state and first excited state of 5Li. These results allow one, for the first time, to test theoretical models for a consistent description of bremsstrahlung and radiative capture in a complex system. Calculations predict both features qualitatively but fail to account for their relative importance.

7.
Phys Rev C Nucl Phys ; 52(2): 704-710, 1995 Aug.
Article in English | MEDLINE | ID: mdl-9970560
11.
12.
Phys Rev C Nucl Phys ; 48(6): 2746-2752, 1993 Dec.
Article in English | MEDLINE | ID: mdl-9969151
13.
Phys Rev C Nucl Phys ; 47(1): 210-215, 1993 Jan.
Article in English | MEDLINE | ID: mdl-9968427
15.
Phys Rev A ; 42(7): 3835-3843, 1990 Oct 01.
Article in English | MEDLINE | ID: mdl-9904481
16.
Phys Rev C Nucl Phys ; 39(4): 1557-1562, 1989 Apr.
Article in English | MEDLINE | ID: mdl-9955363
17.
Phys Rev C Nucl Phys ; 38(5): 2397-2407, 1988 Nov.
Article in English | MEDLINE | ID: mdl-9955066
18.
Phys Rev C Nucl Phys ; 38(5): 2463-2464, 1988 Nov.
Article in English | MEDLINE | ID: mdl-9955082
19.
Phys Rev C Nucl Phys ; 36(6): 2206-2211, 1987 Dec.
Article in English | MEDLINE | ID: mdl-9954344
20.
Phys Rev C Nucl Phys ; 36(4): 1249-1255, 1987 Oct.
Article in English | MEDLINE | ID: mdl-9954212
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