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Phys. Rev. C 59, 21–40 (1999)

Soft-core hyperon-nucleon potentials

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Th. A. Rijken
Institute for Theoretical Physics, University of Nijmegen, Nijmegen, The Netherlands

V. G. J. Stoks
Physics Division, Argonne National Laboratory, Argonne, Illinois 60439
Centre for the Subatomic Structure of Matter, University of Adelaide, SA 5005, Australia

Y. Yamamoto
Physics Section, Tsuru University, Tsuru, Yamanashi 402-0054, Japan

Received 13 July 1998; published in the issue dated January 1999

A new Nijmegen soft-core OBE potential model is presented for the low-energy YN interactions. Besides the results for the fit to the scattering data, which largely defines the model, we also present some applications to hypernuclear systems using the G-matrix method. The potentials are generated by the exchange of nonets of pseudoscalar, vector, and scalar mesons. As is standard in the Nijmegen soft-core models, we also include the J=0 contributions from the tensor f2,f2,a2, and pomeron Regge trajectories, and use Gaussian form factors to guarantee that the potentials have a soft behavior near the origin. An important innovation with respect to the original soft-core potential is the assignment of the cutoff masses for the baryon-baryon-meson (BBM) vertices in accordance with broken SU(3)F, which serves to connect the NN and the YN channels. As a novel feature, we allow for medium strong breaking of the coupling constants, using the 3P0 model with a Gell-Mann–Okubo hypercharge breaking for the BBM coupling. Charge-symmetry breaking in the Λp and Λn channels is included as well. We present six hyperon-nucleon potentials which describe the available YN cross section data equally well, but which exhibit some differences on a more detailed level. The differences are constructed such that the models encompass a range of scattering lengths in the ΣN and ΛN channels. In all cases, we obtained χ2/Ndata0.55 for 35 YN data. In particular, we were able to fit the precise experimental datum rR=0.468±0.010 for the inelastic capture ratio at rest. For the scalar-meson mixing angle we obtained values θS=37°–40°, which points to almost ideal mixing angles for the scalar qq̅ states. The G-matrix results indicate that the remarkably different spin-spin terms of the six potentials appear specifically in the energy spectra of Λ hypernuclei.

© 1999 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevC.59.21
DOI:
10.1103/PhysRevC.59.21
PACS:
13.75.Ev, 12.39.Pn, 21.30.-x, 21.80.+a