Skip to main content
Log in

A proof of the mandelstam representation in perturbation theory

  • Published:
Il Nuovo Cimento (1955-1965)

Summary

The Mandelstam representation is proved in each finite order in perturbation theory for processes for which forward scattering dispersion relations have been proved. A continuation in the external masses is then made so that the proof is extended to all processes for which there is no anomalous threshold in lowest order.

Riassunto

Si dimostra la validità della rappresentazione di Mandelstam in ogni ordine finito nella teoria di perturbazione per processi pei quali sono state dimostrate relazioni di dispersione per lo scattering in avanti. Si fa poi una estensione alle masse esterne cosicchè la dimostrazione diviene valida per tutti i processi in cui non si hanno soglie anomale nell’ordine più basso.

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

References

  1. S. Mandelstam:Phys. Rev.,112, 1344 (1958).

    Article  MathSciNet  ADS  Google Scholar 

  2. R. Karplus, C. M. Sommerfield andE. H. Wichmann:Phys. Rev.,111, 1187 (1958).

    Article  MathSciNet  ADS  MATH  Google Scholar 

  3. R. Oehme:Nuovo Cimento,13, 778 (1959).

    Article  MATH  Google Scholar 

  4. G. Källén andA. S. Wightman:Dan. Vid. Selsk. Mat.-fys. Skr.,1, no. 6 (1958).

  5. J. C. Polkinghorne andG. R. Screaton:Nuovo Cimento,15, 289 and 925 (1960).

    Article  MathSciNet  Google Scholar 

  6. L. D. Landau:Nuclear Physics,13, 181 (1959).

    Article  MathSciNet  ADS  Google Scholar 

  7. J. Tarski:Journ. Math. Phys.,1, 154 (1960).

    Article  MathSciNet  ADS  MATH  Google Scholar 

  8. K. Symanzik:Prog. Theor. Phys.,20, 690 (1957). Note that the parameters α used bySymanzik are essentially the inverse of our Feynman parameters.

    Article  MathSciNet  ADS  Google Scholar 

  9. This point was raised and resolved in discussions with Dr.R. J. Eden. It also affects his proof (9).

  10. R. J. Eden: preprint (Cambridge).

  11. See, for example,H. Lehmann:Suppl. Nuovo Cimento,14, 153 (1959).

    Article  Google Scholar 

  12. R. J. Eden:Phys. Rev.,119, 1763 (1960).

    Article  MathSciNet  ADS  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Additional information

An outline of this work was given as an invited paper at the Tenth International Conference on High Energy Physics, Rochester, 1960.

Rights and permissions

Reprints and permissions

About this article

Cite this article

Landshoff, P.V., Polkinghorne, J.C. & Taylor, J.C. A proof of the mandelstam representation in perturbation theory. Nuovo Cim 19, 939–952 (1961). https://doi.org/10.1007/BF02731236

Download citation

  • Received:

  • Published:

  • Issue Date:

  • DOI: https://doi.org/10.1007/BF02731236

Navigation