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References - Bogoliubov Laboratory of Theoretical Physics - JINR

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3.3 Effect <strong>of</strong> valence neutrons on spin-orbit potential<br />

Here, we discuss the effect <strong>of</strong> valence neutrons on the spin-orbit potential from the systematics<br />

in helium isotopes. For this purpose, an α + xn cluster folding calculation [5]<br />

could be a useful method, since the contribution <strong>of</strong> an α core and valence neutrons can be<br />

separately evaluated. It has been expected from the calculation that the contribution <strong>of</strong><br />

valence neutrons to the spin-orbit potential is one-order <strong>of</strong> magnitude smaller than that<br />

<strong>of</strong> an α core. Consequently, the spin-orbit potentials <strong>of</strong> 6,8 He are expected to be related<br />

to the spatial distribution <strong>of</strong> the α core in a nucleus, i.e., the LS radius should increase<br />

with the diffuseness <strong>of</strong> the α core distribution, whereas the LS amplitude should decrease.<br />

The LS radius and LS amplitude <strong>of</strong> helium<br />

isotopes are plotted in Fig. 5 as a<br />

function <strong>of</strong> the proton orbital radius, which<br />

represents the diffuseness <strong>of</strong> the α core distribution.<br />

Although there are large experimental<br />

uncertainties, almost linear relations<br />

can be seen. From this we can derive<br />

a picture that the valence neutrons affect<br />

the spin-orbit potential rather strongly<br />

through the p − α interaction than via the<br />

direct p − n interaction. The recoil motion<br />

Figure 5: LS radius and LS amplitude <strong>of</strong> helium<br />

isotopes as functions <strong>of</strong> proton radius.<br />

<strong>of</strong> the α core induced by valence neutrons can be important in the explanation <strong>of</strong> the<br />

large difference between spin-orbit potentials in 4 He and neutron-rich helium isotopes.<br />

4 Summary<br />

The vector analyzing power <strong>of</strong> the proton elastic scattering from 6 He and 8 He have been<br />

measured at 71 MeV/A. We found that the spin-orbit potentials in 6 He and 8 He are<br />

significantly shallower than those in stable nuclei. This shallowness can be naturally<br />

explained by the large diffuseness <strong>of</strong> the neutron-rich helium isotopes. The dominance <strong>of</strong><br />

p − α core interaction in the p− 6,8 He spin-orbit potentials is also indicated.<br />

<strong>References</strong><br />

[1] T. Wakui et al., Nucl. Instr. and Meth. 550 (2005) 521.<br />

[2] T. Uesaka et al., Nucl. Instr. and Meth. 526 (2004) 186.<br />

[3] A. Korsheninnikov et al., Nuclear <strong>Physics</strong> A 617 (1997) 45.<br />

[4] R. Henneck et al., Nuclear <strong>Physics</strong> A 571 (1994) 541.<br />

[5] Y. Iseri et al., Genshikaku Kenkyu 49 No.4 (2005) 53.<br />

[6] H. Sakaguchi et al., Physical Review C 26 (1982) 944.<br />

[7] B.A. Watson et al., Physical Review 182 (1969) 977.<br />

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