Scattering of<sup>6</sup>He at energies around the Coulomb barrier

Sánchez-Benítez, Á. M.; Escrig, D.; Álvarez, M. A. G.; Andrés, M. V.; Angulo, C.; Borge, María José García; Cabrera, J.; Cherubini, S.; Espino, J. M.; Фігуера, П.; Freer, M.; García‐Ramos, J. E.; Gómez‐Camacho, J.; Gulino, M.; Kakuee, O.; Martel, I.; Metelco, C; Moro, A. M.; Rahighi, J.; Rusek, K.; Smirnov, D.; Tengblad, O.; Duppen, P. Van; Ziman, V.

doi:10.1088/0954-3899/31/10/109

Cited by 41 publications

(38 citation statements)

References 16 publications

(34 reference statements)

Supporting

Mentioning

Contrasting

Order By: Relevance

“…For example, it has already been shown that the elastic scattering of 6 He in a Coulomb potential dominated regime, with its low breakup threshold and large neutron-proton asymmetry, differs significantly from that of 6 Li [1][2][3][4][5][6]. The ultimate use of the observed potential differences is to be able to relate them to the underlying shell, cluster and halo structures of the interacting nuclei.…”

Section: Introductionmentioning

confidence: 99%

Elastic and inelastic scattering of 7Li + 18O versus 7Li+16O

et al. 2007

View full text Add to dashboard Cite

Section: Introductionmentioning

confidence: 99%

Elastic and inelastic scattering of 7Li + 18O versus 7Li+16O

et al. 2007

View full text Add to dashboard Cite

“…[1,5] due to careful recheck of the energy calibration of the beam monitor detectors. Charged reaction products were detected by means of the detector array DINEX [6]. For the present experiment we used 8 silicon detectors arranged in 4 ΔE (42-48 μm) -E (1000 μm) telescopes.…”

Section: Methodsmentioning

confidence: 99%

“…7 Be was chosen since it has a very small particle emission threshold (S α = 1.586 MeV) and since the majority of direct processes gives rise to either 3 He or 4 He stable ions (with similar energy domains) in the reaction output channels. This feature simplifies the experimental setup and avoids typical problems related to the low-efficiency detection of neutrons (as in 6,8 He-, 9,11 Li-and 9,11 Be-reaction studies), the emission of radioactive or loosely-bound nuclei (as in the case of reactions involving 6,7 Li or 8 B) or the detection of projectile fragments with completely different mass ranges, and in turn energy domains, (as for 17 F breaking up into 16 O+p). …”

Section: Introductionmentioning

confidence: 99%

Transfervs. Breakup in the interaction of the⁷Be Radioactive Ion Beam with a⁵⁸Ni target at Coulomb barrier energies

Mazzocco

Torresi

Acosta

et al. 2014

EPJ Web of Conferences

View full text Add to dashboard Cite

Abstract. We measured for the first time 7 Be elastically scattered nuclei as well as 3,4 He reaction products from a 58 Ni target at 22.3 MeV beam energy. The data were analyzed within the optical model formalism to extract the total reaction cross section. Extensive kinematical, Distorted Wave Born Approximation (DWBA) and Continuum Discretized Coupled Channel (CDCC) calculations were performed to investigate the 3,4 He originating mechanisms and the interplay between different reaction channels.

show abstract

“…Detection set-up: the detector array DINEX 7 Be scattered ions and other charged reaction products, originated from the interaction with a 1.0-mg/cm 2 58 Ni target, were detected by means of the array DINEX [15]. Four ∆E − E telescopes were located around the target in a cylindrical configuration.…”

Section: Be Secondary Beam Productionmentioning

confidence: 99%