Modelling nucleon-nucleon scattering above 1 GeV
arXiv:nucl-th/0311002 · doi:10.1140/epja/i2004-10014-0
Abstract
Motivated by the recent measurement of proton-proton spin-correlation parameters up to 2.5 GeV laboratory energy, we investigate models for nucleon-nucleon (NN) scattering above 1 GeV. Signatures for a gradual failure of the traditional meson model with increasing energy can be clearly identified. Since spin effects are large up to tens of GeV, perturbative QCD cannot be invoked to fix the problems. We discuss various theoretical scenarios and come to the conclusion that we do not have a clear phenomenological understanding of the spin-dependence of the NN interaction above 1 GeV.
36 pages, 8 figures
References in corpus (9)
- Accurate Charge-Dependent Nucleon-Nucleon Potential at Fourth Order of Chiral Perturbation Theory
- Effective Field Theory for Few-Nucleon Systems
- Effective Field Theory of Nuclear Forces
- Accurate Nucleon-Nucleon Potential Based upon Chiral Perturbation Theory
- Chiral 2pi exchange at order four and peripheral NN scattering
- Nucleon-nucleon elastic scattering to 3 GeV
- Chiral -exchange NN-potentials: results for representation invariant classes of diagrams
- Study of the p p -> p p pi+ pi- Reaction in the Low-Energy Tail of the Roper Resonance
- Measurement of Spin Correlation Parameters A, A, and A_ at 2.1 GeV in Proton-Proton Elastic Scattering
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