Abstract:Angular distributions of the 'Be ions from ( Be,'Be) reactions on the target nuclei "Si and ' Ca have been measured at an energy of 20 MeV (lab). The products of the spectroscopic factors of Be and several states of the residual nuclei ' Si and "Ca were extracted from a distortedwave-Born-approximation analysis.Using the spectroscopic factors of "Si and "Ca levels, known from (d, p) reactions, a spectroscopic factor of 0.42 + 0.04 for 'Be was found.
NUCLEAR REACTIONSSi( Be, 8Be) and 40Ca{~Be,8Be), E|~b --20 Me… Show more
“…However, it has one important difference in that the spectroscopic factor for the 9 Be → 8 Be + n overlap is considerably smaller (0.42 [241]) than those for similar processes involving weakly-bound radioactive nuclei. These properties make 9 Be an excellent benchmark for comparison with the light weakly-bound radioactive nuclei.…”
Section: Reactions Induced By 9 Be Beamsmentioning
confidence: 91%
“…The spectroscopic factor and binding potential for the 9 Be = n + 8 Be overlap were from Ref. [241]. Transfer to the lowest 0 + resonance of 8 Be only was included, with couplings to states in 209 Pb as per Table 1 (transfers to the 11/2 + and 15/2 − states were again omitted).…”
Section: Reactions Induced By 9 Be Beamsmentioning
“…However, it has one important difference in that the spectroscopic factor for the 9 Be → 8 Be + n overlap is considerably smaller (0.42 [241]) than those for similar processes involving weakly-bound radioactive nuclei. These properties make 9 Be an excellent benchmark for comparison with the light weakly-bound radioactive nuclei.…”
Section: Reactions Induced By 9 Be Beamsmentioning
confidence: 91%
“…The spectroscopic factor and binding potential for the 9 Be = n + 8 Be overlap were from Ref. [241]. Transfer to the lowest 0 + resonance of 8 Be only was included, with couplings to states in 209 Pb as per Table 1 (transfers to the 11/2 + and 15/2 − states were again omitted).…”
Section: Reactions Induced By 9 Be Beamsmentioning
“…The latter set of form factors were taken to be those obtained from the adiabatic model analysis of the 20 MeV 208 Pb(d,p) 209 Pb data. Lang et al [27] obtained a 9 Be/ 8 Be spectroscopic factor of C 2 S = 0.42 for the 1p 1/2 neutron bound in a Woods-Saxon potential well with parameters R = 1.15 × 8 1/3 fm, a = 0.57 fm with the depth adjusted to give the correct binding energy and a spin-orbit component with the same geometry parameters and a fixed depth of 5.5 MeV. The form-factors of Kovar et al [22] bound the neutron in a Woods-Saxon potential well with parameters R = 1.23 × 208 1/3 fm, a = 0.65 fm with the depth adjusted to give the correct binding energy and a spin-orbit component with the same geometry parameters and a fixed depth of 6.0 MeV.…”
Section: The Calculationsmentioning
confidence: 97%
“…We therefore performed a second set of calculations including the single neutron stripping, with the form factors for the 9 Be/ 8 Be and 209 Pb/ 208 Pb overlaps being taken from Lang et al [27] and Kovar et al [22], respectively. The latter set of form factors were taken to be those obtained from the adiabatic model analysis of the 20 MeV 208 Pb(d,p) 209 Pb data.…”
A series of coupled reaction channels calculations for the 9 Be+ 209 Pb system at near-barrier energies is presented. Single neutron stripping couplings leading to several states in 209 Pb together with coupling to the direct breakup of 9 Be using a 5 He+α cluster model are included. We find that the transfer couplings give rise to a dynamic polarization potential with the same characteristics in the nuclear surface region as that produced by breakup.
“…The Woods-Saxon potential parameters (radius and diffuseness) along with a spin-orbit component for the binding of neutron in 9 Be is taken from Ref. [23]. The 1/2 + and 5/2 + resonance states are generated by using the radius and diffuseness parameters same as that of the ground state while the potential depth is varied.…”
He model, the former being more prominent at lower energies and for the heavier target systems. The behaviour of extracted dynamic polarisation potentials (DPP) generated due to breakup and one neutron transfer couplings have been investigated.
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