Elastic proton-deuteron backward scattering at energies from 0.6 to 2.7 GeV
P Berthet; R Frascaria; M P Combes; Ch F Perdrisat; B Tatischeff; J Banaigs; J Berger; A Codino; J Duflo; L Goldzahl; F Plouin; F Fabbri; G Picozza; L Satta; M Boivin; P Berthet; Inst. de Phys. Nucleaire, Orsay, France; R Frascaria; Inst. de Phys. Nucleaire, Orsay, France; M P Combes; Inst. de Phys. Nucleaire, Orsay, France; Ch F Perdrisat; Inst. de Phys. Nucleaire, Orsay, France; B Tatischeff; Inst. de Phys. Nucleaire, Orsay, France; J Banaigs; Inst. de Phys. Nucleaire, Orsay, France; J Berger; Inst. de Phys. Nucleaire, Orsay, France; A Codino; Inst. de Phys. Nucleaire, Orsay, France; J Duflo; Inst. de Phys. Nucleaire, Orsay, France; L Goldzahl; Inst. de Phys. Nucleaire, Orsay, France; F Plouin; Inst. de Phys. Nucleaire, Orsay, France; F Fabbri; Inst. de Phys. Nucleaire, Orsay, France; G Picozza; Inst. de Phys. Nucleaire, Orsay, France; L Satta; Inst. de Phys. Nucleaire, Orsay, France; M Boivin; Inst. de Phys. Nucleaire, Orsay, France
Журнал:
Journal of Physics G: Nuclear Physics
Дата:
1982-08-01
Аннотация:
Elastic pd backward scattering in the kinetic energy range 0.6<T<sub>p</sub><2.7 GeV has been measured and is discussed in terms of the one-nucleon-exchange (ONE) and the one-pion-exchange (OPE) mechanisms. The experimental plateau appearing in the 180 degrees excitation function for T<sub>p</sub>>2 GeV could be explained as excitation of the Delta (1950) in the intermediate state.
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