Advertisement

Il Nuovo Cimento A (1965-1970)

, Volume 21, Issue 3, pp 503–517 | Cite as

An application to a sequential decay scheme for multiparticle phenomena

  • A. Ballestrero
Article

Summary

The formalism previously developed for multiparticle production phenomena is applied to a specific choice of energy distribution probability which is guessed from inclusive one-particle data. The asymptotic picture that emerges is in rather nice qualitative agreement with the experimental trend.

Применение схемы последовательного распада к многочастичным явлениям

Реэюме

Ранее раэвитый формалиэм для явлений многочастичного рождения применяется к специальному выбору вероятности распределения знергии, которая предполагается иэ инклюэивных одночастичных данных. Асимптотическая картина согласуется с зкспериментальными данными.

Riassunto

Il formalismo sviluppato precedentemente per descrivere fenomeni di produzione multipla è applicato ad una scelta specifica di distribuzione di probabilità nella variabile energia che è suggerita dai dati inclusivi ad una particella. La descrizione che ne emerge nel limite asintotico è in buon accordo qualitativo con l’andamento sperimentale.

Preview

Unable to display preview. Download preview PDF.

Unable to display preview. Download preview PDF.

Literatur

  1. (1).
    A. Ballestrero andE. Predazzi:Nuovo Cimento,21 A, 485 (1974).CrossRefADSGoogle Scholar
  2. (2).
    H. Bøggild, E. Dahl-Jensen, K. H. Hansen, J. Johnstad, E. Lohse, M. Suk, L. Veje, V. J. Karimäki, K. V. Laurikainen, E. Riipinen, T. Jacobsen, S. O. Sørensen, J. Allan, G. Blomquist, O. Danielsen, G. Ekspong, L. Granstrøm, S. O. Holmgren, S. Nilsson, B. E. Ronne, U. Svedin andN. K. Yamdagni:Nucl. Phys.,27 B, 285 (1971).CrossRefADSGoogle Scholar
  3. (3).
    A. Erdélyi, W. Magnus, F. Oberhettinger andF. Tricomi:Bateman Manuscript Project; Tables of Integral Transforms, Vol.1 (New York, N. Y., 1953), p. 232, eq. (18).Google Scholar
  4. (4).
    W. Furry:Phys. Rev.,52, 569 (1937).MATHCrossRefADSGoogle Scholar
  5. (5).
    A. Giovannini andE. Predazzi:Nuovo Cimento,52 A, 255 (1967);A. Ballestrero, A. Giovannini, R. Nulmann andE. Predazzi:Nuovo Cimento,5 A, 197 (1971).CrossRefADSGoogle Scholar
  6. (6).
    A. Giovannini:Nuovo Cimento,2 A, 209 (1971);10 A, 713 (1972).MATHCrossRefADSGoogle Scholar
  7. (7).
    A. Wroblewski:Strong interactions, inLectures Notes Ecole Internationale de la Physique des Particules Elementaires, Basko Polje Makarska (1972).Google Scholar
  8. (9).
    E. Kamke:Differentialgleichungen. Lösungsmethoden und Lösungen, Sect. A 22.1 (Leipzig, 1961), p. 105.Google Scholar
  9. (10).
    S. Yamada andM. Koshiba:Phys. Rev.,157, 1279 (1967).CrossRefADSGoogle Scholar
  10. (11,12).
    For a report of these data see, for example,M. Jacob:High-energy collision production processes at high energy. Theory and experiment, Th. 1570-CERN (1972).Google Scholar
  11. (13).
    Z. Koba, H. B. Nielsen andP. Olesen:Nucl. Phys.,40 B, 317 (1972).CrossRefADSGoogle Scholar
  12. (14).
    P. Slattery:Evidence for systematic behaviour of charged prong multiplicity distributions in high-energy proton-proton collisions, Rochester preprint, COO-3065-26, Sept. 1972.Google Scholar
  13. (15).
    E. L. Berger, D. Horn andG. H. Thomas:Correlations between neutral and charged pions in multiparticle production, Argonne preprint ANL/HEP 7240, Sept. 1972.Google Scholar
  14. (16).
    G. G. Beznogikh, A. Bujak, V. A. Nikitin, M. G. Shafranova, V. A. Sviridov, Truong Bien, L. V. Vikhlyantseva, V. I. Zayachki andL. S. Zolin:Phys. Lett.,43 B, 85 (1973).CrossRefADSGoogle Scholar

Copyright information

© Società Italiana di Fisica 1974

Authors and Affiliations

  • A. Ballestrero
    • 1
  1. 1.Istituto Nazionale di Fisica NucleareSezione di TorinoItaly

Personalised recommendations