Skip to main content
Log in

Particule composée et comportement asymptotique

  • Published:
Il Nuovo Cimento (1955-1965)

Summary

The renormalized propagator of the V-particle in the Lee model satisfies a spectral representation which, in the case of a composite particle, differs from the classical representation of Lehmann. In addition to the usual spectral integral, a constant term appears which modifies the asymptotic behaviour. It is shown that this term is related to the equal-time commutator which occurs in the dispersion relations, and a test of elementarity based on the presence of this commutator is discussed. However, in the case of an elementary particle, the test is weakened by the existence of a resonance at the bare mass of the V-particle.

Riassunto

Il propagatore rinormalizzato della particella V nel modello di Lee soddisfa una rappresentazione spettrale che, nel caso di una particella composta, differisce dalla rappresentazione classica di Lehmann. In aggiunta al solito integrale spettrale, appare un termine costante che modifica il comportamento asintotico. Si dimostra che questo termine è collegato al commutatore dei tempi uguali che si presenta nelle relazioni di dispersione, e si discute un metodo di prova dell’elementarità basato sulla presenza di questo commutatore. Tuttavia, nel caso di una particella elementare, il metodo è indebolito dall’esistenza di una risonanza situata alla massa nuda della particella V.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

Similar content being viewed by others

Literatur

  1. J. C. Houard etB. Jouvet:Nuovo Cimento,18, 466 (1960).

    Article  MathSciNet  MATH  Google Scholar 

  2. M. T. Vaughn, R. Aaron andR. D. Amado:Phys. Rev.,124, 1258 (1961).

    Article  ADS  MATH  Google Scholar 

  3. T. D. Lee:Phys. Rev.,95, 1329 (1954);G. Källén andW. Pauli:Dan. Mat. Fys. Medd.,30, n. 7 (1955).

    Article  ADS  MATH  Google Scholar 

  4. H. Lehmann:Nuovo Cimento,11, 342 (1954).

    Article  MathSciNet  MATH  Google Scholar 

  5. On retrouve ici dans un cas particulier la notion générale de champ quasi-local introduite parR. Haag:Phys. Rev.,112, 669 (1958).

    Article  MathSciNet  ADS  MATH  Google Scholar 

  6. Condition II de (1).

    Article  MathSciNet  MATH  Google Scholar 

  7. L’exemple contenu dans la réf. (1) correspond à un cas oùδν et l’intégrale deϱl sont tous deux divergents [δν l ϕ peut néanmoins rester fini d’après (5) et (15)]. Mais δν peut converger sans qu’il en soit de même pour εd l (a).

    Article  MathSciNet  MATH  Google Scholar 

  8. J. Hamilton andW. S. Woolcock:Rev. Mod. Phys.,35, 737 (1963).

    Article  ADS  Google Scholar 

  9. K. W. Ford:Nuovo Cimento,24, 467 (1962).

    Article  Google Scholar 

  10. Il en est de même pour le test du déphasage proposé dans la réf. (2).

    Article  ADS  MATH  Google Scholar 

  11. P. Borgeaud et al.:Phys. Lett.,10, 134 (1964);B. Amblard et al.:Phys. Lett.,10, 138 (1964).

    Article  ADS  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Additional information

Ce travail a bénéficié de l’aide du Commissariat à l’Energie Atomique.

Je suis heureux de remercierM. B. Jouvet pour ses nombreux conseils et critiques.

Rights and permissions

Reprints and permissions

About this article

Cite this article

Houard, J.C. Particule composée et comportement asymptotique. Nuovo Cim 35, 194–207 (1965). https://doi.org/10.1007/BF02734833

Download citation

  • Received:

  • Published:

  • Issue Date:

  • DOI: https://doi.org/10.1007/BF02734833

Navigation