2012
DOI: 10.1103/physrevc.86.044607
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Elastic scattering in the6,7Li+80Se systems

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Cited by 32 publications
(35 citation statements)
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“…Left panel: The strengths of the real (b) and imaginary (a) parts of the optical potential at the distance of maximal absorption, R M , in collisions of6 Li projectiles with the 80 Se target[107]; Right panel: the same as in the left panel but for a 144 Sm target[112]. Source: For detail, see the original papers[107,112].…”
mentioning
confidence: 97%
“…Left panel: The strengths of the real (b) and imaginary (a) parts of the optical potential at the distance of maximal absorption, R M , in collisions of6 Li projectiles with the 80 Se target[107]; Right panel: the same as in the left panel but for a 144 Sm target[112]. Source: For detail, see the original papers[107,112].…”
mentioning
confidence: 97%
“…The strength of real part also decreases. This has already been argued in several articles [15][16][17][18][19][20][21][22][23][24][25][26]. However, authors Rodrigo et al in recent article [27] have argued the Threshold Anomaly (TA) for weakly bound projectile system like 6 Li + 209 Bi and 6 He + 208 Pb, contrary to the observations in other references.…”
Section: Introductionmentioning
confidence: 90%
“…For example, for the tightly bound system 16 O + 208 Pb, the threshold energy can be determined easily as about 0.93V B [3]. For the stable weakly bound nucleus 6 Li, on the other hand, the decreasing trend of the imaginary potential was observed only in a few medium-mass target systems, such as 6 Li + 80 Se [20] and 6 Li + 144 Sm [21], with a threshold energy of about 0.76V B and 0.81V B , respectively. However, for a heavy target system as investigated in the present work, no similar result has been reported so far, because the imaginary potential still presents an increasing trend at the lowest energies, such as 0.86V B for 6 Li + 208 Pb [46] and 0.94V B for 9 Be + 209 Bi [47].…”
Section: Energy Dependence Of the Omp Of 6 He + 209 Bimentioning
confidence: 99%
“…However, because of the large data uncertainties as well as the lack of enough data points [11,16], it is nearly impossible to investigate the optical potentials of halo systems in the subbarrier region directly with low-intensity radioactive ion beams. Even for stable weakly bound systems, we are still far from a clear understanding of the properties of OMPs, e.g., the behavior of the potential in the deep subbarrier region leaves much to be desired [5,20,21], and the application of the dispersion relation is still debatable [4,17,18,22].…”
Section: Introductionmentioning
confidence: 99%