References
J. Ballam, G. B. Chadwick, R. Gearhart, Z. G. T. Guiragossián, M. Menke, J. J. Murray, P. Seyboth, A. Shapira, C. K. Singclair, I. O. Skillicorn, G. Wolf, R. H. Milburn, H. H. Bingham, W. B. Fretter, K. C. Moffeit, W. J. Podolsky, M. S. Rabin, A. H. Rosenfeld andR. Windmolders:Phys. Rev. Lett.,24, 960 (1970).
G. Höhler andR. Strauss:Zeits. Phys.,232, 205 (1970).
F. J. Gilman, J. Pumplin, A. Schwimmer andL. Stodolsky:Phys. Lett.,31 B, 387 (1970).
H. F. Jones andM. D. Scadron:Nucl. Phys.,4 B, 267 (1968).
H. F. Jones andM. D. Scadron:Phys. Rev.,171, 1809 (1968).
F. D. Gault andM. D. Scadron:Nucl. Phys.,15 B, 442 (1970).
G. Cohen-Tannoudji, Ph. Salin andA. Morel:Nuovo Cimento,55 A, 412 (1968).
S. Mandelstam andL. Wang:Phys. Rev.,160, 1490 (1967).
J. H. Schwarz:Phys. Rev.,159, 1271 (1967).
V. D. Mur:Sov. Phys. JETP,17, 1458 (1963).
H. F. Jones, M. D. Scadron andF. D. Gault:Nuovo Cimento,66 A, 424 (1970).
F. Arbab andR. C. Browner:Phys. Rev.,181, 2124 (1969).
The expected angular distribution is given in ref. (3).
C. B. Chiu andS. Matsuda:Phys. Lett.,31 B, 455 (1970).
Though also consistent withs-channel helicity considerations, we do not favour the scheme of ref. (17), in which the ρ and ω, members of the sameSU 3 multiplet, belong to opposite analyticity classes.
J. Finkelstein:Phys. Rev. Lett.,22, 362 (1969).
Author information
Authors and Affiliations
Additional information
An erratum to this article is available at http://dx.doi.org/10.1007/BF02753776.
Rights and permissions
About this article
Cite this article
Jones, H.F. s-Channel helicity conservation, fixed poles and dip mechanisms. Lettere Nuovo Cimento (1969-1970) 4, 545–548 (1970). https://doi.org/10.1007/BF02755310
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02755310