This title appears in the Scientific Report :
2007
Please use the identifier:
http://dx.doi.org/10.1007/978-3-540-72039-3_4 in citations.
Please use the identifier: http://hdl.handle.net/2128/10529 in citations.
The Hyperon-nucleon interaction: Conventional versus effective field theory approach
The Hyperon-nucleon interaction: Conventional versus effective field theory approach
Hyperon-nucleon interactions are presented that are derived either in the conventional meson-exchange picture or within leading order chiral effective field theory. The chiral potential consists of one-pseudoscalar-meson exchanges and non-derivative four-baryon contact terms. With regard to meson-ex...
Saved in:
Personal Name(s): | Haidenbauer, J. |
---|---|
Meissner, U.G. / Nogga, A. / Polinder, H. | |
Contributing Institute: |
Theorie der starken Wechselwirkung; IKP-3 |
Published in: |
Lecture Notes in Physics. - 724 (2007). - Berlin, Springer. - 978-3-540-72038-6. - S. 113 - 140 |
Imprint: |
2007
|
DOI: |
10.1007/978-3-540-72039-3_4 |
Document Type: |
Contribution to a book Contribution to a conference proceedings |
Research Program: |
Physik der Hadronen und Kerne |
Subject (ZB): | |
Link: |
Get full text OpenAccess OpenAccess |
Publikationsportal JuSER |
Please use the identifier: http://hdl.handle.net/2128/10529 in citations.
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520 | |a Hyperon-nucleon interactions are presented that are derived either in the conventional meson-exchange picture or within leading order chiral effective field theory. The chiral potential consists of one-pseudoscalar-meson exchanges and non-derivative four-baryon contact terms. With regard to meson-exchange hyperon-nucleon models we focus on the new potential of the Juelich group, whose most salient feature is that the contributions in the scalar--isoscalar (\sigma) and vector--isovector (\rho) exchange channels are constrained by a microscopic model of correlated \pi\pi and KKbar exchange. | ||
650 | 7 | |a nucleon hyperon: scattering amplitude |2 INSPIRE | |
650 | 7 | |a coupled channel |2 INSPIRE | |
650 | 7 | |a nucleon Lambda: interaction |2 INSPIRE | |
650 | 7 | |a nucleon Sigma: interaction |2 INSPIRE | |
650 | 7 | |a Lippmann-Schwinger equation |2 INSPIRE | |
650 | 7 | |a effective Lagrangian: chiral |2 INSPIRE | |
650 | 7 | |a effective potential |2 INSPIRE | |
650 | 7 | |a baryon: four-fermion interaction |2 INSPIRE | |
650 | 7 | |a meson: exchange |2 INSPIRE | |
650 | 7 | |a pseudoscalar meson |2 INSPIRE | |
650 | 7 | |a scalar meson |2 INSPIRE | |
650 | 7 | |a vector meson |2 INSPIRE | |
650 | 7 | |a exchange: (2pseudoscalar meson) |2 INSPIRE | |
650 | 7 | |a nucleon hyperon: elastic scattering |2 INSPIRE | |
650 | 7 | |a channel cross section: momentum dependence |2 INSPIRE | |
650 | 7 | |a angular distribution: momentum dependence |2 INSPIRE | |
650 | 7 | |a scattering length |2 INSPIRE | |
650 | 7 | |a partial wave analysis |2 INSPIRE | |
650 | 7 | |a hydrogen: hypernucleus |2 INSPIRE | |
650 | 7 | |a helium: hypernucleus |2 INSPIRE | |
650 | 7 | |a energy levels |2 INSPIRE | |
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