Extension of the Isobaric Nucleon Model for Pion Production in Pion-Nucleon, Nucleon-Nucleon, and Antinucleon-Nucleon Interactions

1961 ◽  
Vol 123 (1) ◽  
pp. 333-376 ◽  
Author(s):  
R. M. Sternheimer ◽  
S. J. Lindenbaum

1969 ◽  
Vol 64 (4) ◽  
pp. 881-899 ◽  
Author(s):  
G. Bozóki ◽  
E. Gombosi ◽  
M. Posch ◽  
L. Vanicsek


Cross-sections for pion production in nucleon-nucleon collisions are calculated on the assumption that the production takes place into a few angular momentum states only, and that the matrix element for each particular transition is constant except for factors due to the final-state pion-nucleon and nucleon-nucleon interactions. The outgoing pion is assumed to be in a resonant (3/2, 3/2) state with one of the nucleons. The angular momentum states introduced are compared with those of Rosenfeld (1954) and Gell-Mann & Watson (1954). It is found that a three-parameter theory can give a good account of most of the experiments on pion production, both total and differential, up to 660 MeV, except near threshold when non-resonance production is important and further parameters are necessary. Energy distribution and angular correlation experiments bring out the importance of the pion-nucleon resonance. The cross-section for neutral pion production is predicted fairly accurately in terms of that for positive pion production from threshold to 660 MeV; at 660 MeV, the calculated positive:neutral ratio is 3⋅9. The difference between this value and that of Peaslee (1954) is partly due to the mass difference between the positive and neutral pion and partly to the inclusion of interference effects between the outgoing nucleons.



1960 ◽  
Vol 5 (1) ◽  
pp. 24-26 ◽  
Author(s):  
S. J. Lindenbaum ◽  
R. M. Sternheimer


2021 ◽  
Vol 71 (1) ◽  
pp. 377-402
Author(s):  
L. Fabbietti ◽  
V. Mantovani Sarti ◽  
O. Vázquez Doce

The strong interaction among hadrons has been measured in the past by scattering experiments. Although this technique has been extremely successful in providing information about the nucleon–nucleon and pion–nucleon interactions, when unstable hadrons are considered the experiments become more challenging. In the last few years, the analysis of correlations in the momentum space for pairs of stable and unstable hadrons measured in pp and p+Pb collisions by the ALICE Collaboration at the LHC has provided a new method to investigate the strong interaction among hadrons. In this article, we review the numerous results recently achieved for hyperon–nucleon, hyperon–hyperon, and kaon–nucleon pairs, which show that this new method opens the possibility of measuring the residual strong interaction of any hadron pair.



1973 ◽  
Vol 44 (1) ◽  
pp. 1-4 ◽  
Author(s):  
R. Vinh Mau ◽  
J.M. Richard ◽  
B. Loiseau ◽  
M. Lacombe ◽  
W.N. Cottingham


2006 ◽  
Vol 74 (1) ◽  
Author(s):  
N. Paar ◽  
P. Papakonstantinou ◽  
H. Hergert ◽  
R. Roth


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