Hyperon production in the threshold region was studied in the reaction pp→K+Λp using the time-of-flight spectrometer COSY-TOF. Exclusive data, covering the full phase-space, were taken at the three different beam momenta of pbeam=2.95, 3.20 and 3.30 GeV/c, corresponding to excess energies of ε=204, 285 and 316 MeV, respectively. Total cross-sections were deduced for the three beam momenta to be 23.9±0.8±2.0 μb, 28.4±1.3±2.2 μb and 35.0±1.3±3.0 μb. Differential observables including Dalitz plots were obtained. The analysis of the Dalitz plots reveals a strong influence of the N(1650)-resonance at pbeam=2.95 GeV/c, whereas for the higher momenta an increasing relative contribution of the N(1710)- and/or of the N(1720)-resonance was observed. In addition, the pΛ-final-state interaction turned out to have a significant influence on the Dalitz plot distribution.

Influence of N*-resonances on hyperon production in the channel pp->K+ Lambda p at 2.95, 3.20 and 3.30 GeV/c beam momentum

MARCELLO, Simonetta;
2010-01-01

Abstract

Hyperon production in the threshold region was studied in the reaction pp→K+Λp using the time-of-flight spectrometer COSY-TOF. Exclusive data, covering the full phase-space, were taken at the three different beam momenta of pbeam=2.95, 3.20 and 3.30 GeV/c, corresponding to excess energies of ε=204, 285 and 316 MeV, respectively. Total cross-sections were deduced for the three beam momenta to be 23.9±0.8±2.0 μb, 28.4±1.3±2.2 μb and 35.0±1.3±3.0 μb. Differential observables including Dalitz plots were obtained. The analysis of the Dalitz plots reveals a strong influence of the N(1650)-resonance at pbeam=2.95 GeV/c, whereas for the higher momenta an increasing relative contribution of the N(1710)- and/or of the N(1720)-resonance was observed. In addition, the pΛ-final-state interaction turned out to have a significant influence on the Dalitz plot distribution.
2010
688
142
149
http://arxiv.org/abs/arXiv:1003.0603
Associated strangeness production; hyperon production; total cross-section; baryon resonances; Dalitz plot
S. AbdEl-Samad; M. Abdel-Bary; K. Brinkmann; H. Clement; J. Dietrich; E. Dorochkevitch; S. Dshemuchadse; K. Ehrhardt; A. Erhardt; W. Eyrich; C. Fanara; D. Filges; A. Filippi; H. Freiesleben; M. Fritsch; W. Gast; J. Georgi; A. Gillitzer; J. Gottwald; J. Hauffe; D. Hesselbarth; H. Jaeger; B. Jakob; R. Jaekel; L. Karsch; K. Kilian; H. Koch; M. Krapp; J. Kress; E. Kuhlmann; A. Lehmann; S. Marcello; S. Marwinski; S. Mauro; A. Metzger; W. Meyer; P. Michel; K. Moeller; H. Moertel; H. P. Morsch; L. Naumann; N. Paul; L. Pinna; C. Pizzolotto; C. Plettner; S. Reimann; M. Richter; J. Ritman; E. Roderburg; A. Schamlott; P. Schoenmeier; M. Schulte-Wissermann; W. Schroeder; T. Sefzick; M. Steinke; F. Stinzing; G. Sun; A. Teufel; W. Ullrich; J. Waechter; G. J. Wagner; M. Wagner; R. Wenzel; A. Wilms; P. Wintz; S. Wirth; P. Wüstner and P. Zupranski
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/75726
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