References
F. J. Gilman, J. Pumplin, A. Schwimmer andL. Stodolsky:Phys. Lett.,31 B, 387 (1970).
H. H. Bingham, W. B. Fretter, K. C. Moffeit, W. J. Podolsky, M. S. Rabin, A. H. Rosenfeld, R. Windmolders, J. Ballam, G. B. Chadwick, R. Gearhart, Z. G. T. Guiragossián, M. Menke, J. J. Murray, P. Seyboth, A. Shapira, C. K. Sinclair, I. O. Skillicorn, G. Wolf andR. H. Milburn:Phys. Rev. Lett.,24, 955 (1970).
S. Mandelstam, J. E. Paton, R. F. Peierls andA. Q. Sarker:Ann. of Phys.,18, 198 (1962).
For the reader’s convenience we repeat here the definitions ofφ i:φ 1 −φ 1(3/2, 1/2),φ 2 =φ 2(1/2, 1/2),φ 3 =φ 3(− 1/2, 1/2),ϕ 4 =φ 1(− 3/2, 1/2). We have chosen the metrics −g 00 =: 1 − +g 11 −g 22 −g 33 instead of the metrics which has been used in ref. (3). There are several misprints in the formulae (A.9) of ref. (5).
If one takes into account the restrictions forB i that come from Froissart bounds for forward scattering amplitudes, one may find for larges that |B 1| ⩽c 1 s −1, |B 2| ⩽c 2 s 0 in the forward direction (neglecting the logs dependence of the Froissart bounds (7).
H. F. Jones andM. D. Scadron:Nuovo Cimento,48 A, 545 (1967).
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On leave of absence from the Institute for Nuclear Research, Warsaw.
This work was done during the author’s stay on a UNESCO Fellowship at the International Centre for Theoretical Physics, Trieste.
An erratum to this article is available at http://dx.doi.org/10.1007/BF02755272.
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Seweryński, M. On theγ 5-gauge invariance and helicity conservation in high-energy meson-baryon scattering. Lettere Nuovo Cimento (1969-1970) 4, 819–824 (1970). https://doi.org/10.1007/BF02755159
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DOI: https://doi.org/10.1007/BF02755159