Note on spin-orbit interactions in nuclei and hypernuclei
arXiv:0802.1190 · doi:10.1016/j.nuclphysa.2008.02.299
Abstract
A detailed comparison is made between the spin-orbit interactions in hypernuclei and ordinary nuclei. We argue that there are three major contributions to the spin-orbit interaction: 1) a short-range component involving scalar and vector mean fields; 2) a ''wrong-sign'' spin-orbit term generated by the pion exchange tensor force in second order; and 3) a three-body term induced by two-pion exchange with excitation of virtual -isobars (a la Fujita-Miyazawa). For nucleons in nuclei the long-range pieces related to the pion-exchange dynamics tend to cancel, leaving room dominantly for spin-orbit mechanisms of short-range origin (parametrized e.g. in terms of relativistic scalar and vector mean fields terms). In contrast, the absence of an analogous -exchange three-body contribution for hyperons in hypernuclei leads to an almost complete cancellation between the short-range (relativistic mean-field) component and the ''wrong-sign'' spin-orbit interaction generated by second order -exchange with an intermediate hyperon. These different balancing mechanisms between short- and long-range components are able to explain simultaneously the very strong spin-orbit interaction in ordinary nuclei and the remarkably weak spin-orbit splitting in hypernuclei.
10 pages, 7 figures, to be published in Nuclear Physics A, Special Issue on "Strangeness Nuclear Physics (ed. A. Gal)
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- Hypernuclear single particle spectra based on in-medium chiral SU(3) dynamics
- Structure of 55Ti from relativistic one-neutron knockout
- Nuclear energy density functional from chiral pion-nucleon dynamics revisited
- Addressing spectroscopic quality of covariant density functional theory
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- Overview of Strangeness Nuclear Physics
- Contribution of the rho meson and quark sub-structure to the nuclear spin-orbit potential
- Nuclear Matter and Finite Nuclei in the Effective Chiral Model
- From spin to pseudospin symmetry: The origin of magic numbers in nuclear structure
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