Summary
We propose a model in which the elastic backward peak for high-energy pion-nucleon scattering is explained as the shadow of the production processes. The small height of the backward peak as compared to that of the forward one is due to the forward-backward asymmetries in the angular distributions of the secondaries in πp collisions. The application of the model to π+p scattering at 8 GeV/c gives the right order of magnitude for the height of the backward peak and a width approximately equal to that of the forward one.
Riassunto
Si propone un modello in cui il picco elastico all'indietro nella diffusione pione-nucleone ad alta energia è dovuto all'ombra dei processi di produzione. Il piccolo valore della sezione d'urto all'indietro in confronto con la sezione d'urto in avanti è dovuto alle asimmetrie avanti-indietro delle distribuzioni angolari dei secondari prodotti negli urti pione-nucleone. L'applicazione del modello all'urto π+p a 8 GeV/c fornisce il corretto ordine di grandezza per l'altezza del picco all'indietro ed una larghezza all'incirca uguale a quella del picco in avanti.
Similar content being viewed by others
References
C. Coffin, N. Dikman, L. Ettlinger, D. Meyer, A. Saulys, K. Terwilliger andD. Williams:Phys. Rev. Lett.,15, 838 (1965).
W. R. Frisken, A. L. Read, H. Ruderman, A. D. Krisch, J. Orear, R. Rubinstein, D. S. Scarl andD. H. White:Phys. Rev. Lett.,15, 313 (1965).
W. F. Baker, P. J. Carlson, V. Chabaud, A. Lundby, E. Michaelis, J. Banaige, J. Berger, C. Bonnel, J. Duflo, L. Goldzahl andF. Plouin:Oxford Conference on Elementary Particles and private communication.
S. W. Kormanyos, A. D. Krisch, J. R. O'Fallon, K. Ruddick andL. G. Ratner:Phys. Rev. Lett.,16, 709 (1966).
H. Brody, R. Lanza, R. Marshall, J. Niederer, W. Selove, M. Shochet andR. Van Berg:Phys. Rev. Lett.,16, 829 (1966).
D. I. Blokhintsev:Nuovo Cimento,23, 1061 (1962).
M. L. Perl, L. W. Jones andC. C. Ting:Phys. Rev.,132, 1252 (1963).
V. Singh andB. M. Udgaonkar:Phys. Rev.,123, 1487 (1961).
V. Cook, B. Cork, W. Holly andM. L. Perl:Phys. Rev.,130, 762 (1963).
R. M. Heinz andM. H. Ross:Phys. Rev. Lett.,14, 1091 (1965).
V. N. Gribov:Sov. Phys. JETP,16, 1080 (1963);T. Kinoshita:Fermion Regge Poles and the Asymptotic Behaviour of Backward Meson-Nucleon Scattering, CERN report 62-33 (1962);G. F. Chew andJ. D. Stack:Phys. Rev. (to be published);J. D. Stack:Phys. Rev. Lett.,16, 286 (1966).
N. Byers andC. N. Yang:Phys. Rev.,142, 976 (1966).
L. Van Hove:Nuovo Cimento,28, 798 (1963).
L. Van Hove:Rev. Mod. Phys.,36, 655 (1964);Theoretical Problems in Strong Interactions at High Energies, lectures given at CERN (1964).
L. Bertocchi, S. Fubini andM. Tonin:Nuovo Cimento,25, 626 (1962).
See, for instance,D. N. Perkins:Progr. in Elem. Part. Cosmic Ray Phys.,5, 328 (1960);Ch. Peyrou:Aix-en-Provence International Conference (1961), p. 99;I.C.E.F. Collaboration:Suppl. Nuovo Cimento,26, 1039 (1962).
A. Białas:Nuovo Cimento,33, 972 (1964).
H. Fukuda andC. Iso:Nuovo Cimento,43A 43 (1966).
Aachen-Berlin-CERN Collaboration: see for example,Phys. Lett.,12, 356 (1965); and19, 608 (1965) and private communication.
See, for instance,J. Orear, R. Rubinstein, D. B. Scarl, D. H. White, A. D. Krisch, W. R. Frisken, A. L. Read andH. Ruderman:Phys. Rev. Lett.,15, 305 (1965).
G. Cocconi, V. T. Cocconi, A. D. Krisch, J. Orear, R. Rubinstein, D. B. Scarl, B. T. Ulrich, W. F. Baker, E. W. Jenkins andA. L. Read:Phys. Rev.,138, B 165 (1965).
M. Bardadin, L. Michejda, S. Otwinowski andR. Sosnowski:Six-Prong Interactions of 10 GeV/cNegative Pions in Hydrogen, Warsaw report (1964). Figure 1 is due to Dr.L. Michejda.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Bertocchi, L., Capella, A. Shadow model for the high-energy pion-proton elastic backward peak. Nuovo Cimento A (1965-1970) 44, 1194–1209 (1966). https://doi.org/10.1007/BF02719359
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02719359