References
Cf.,e.g.,M. Gell-Mann andF. E. Low:Phys. Rev.,95, 1300 (1954).
I. F. Ginzburg, A. V. Efremov andV. G. Serbo:Yad. Fiz.,9, 451 (1969);I. F. Ginzburg andV. G. Serbo:Yad. Fiz.,9, 868 (1969).
A. V. Efremov, I. F. Ginzburg andV. G. Serbo: JINR E2-4572 (1969);V. M. Budnev, I. F. Ginzburg andV. G. Serbo:Sov. Journ. Theor. Math. Phys.,6, 55 (1971);A. V. Efremov andI. F. Ginzburg:Phys. Lett.,36 B, 371 (1971). Here the calculations were made at\(\varepsilon _{\dot \iota } = 0\) andg s =0. However, their extension to the case\(\varepsilon _{\dot \iota } \ne 0\) andg s ≠0 is easy.
In the nonrelativistic casej→j+1/2.
In fact the amplitude with a negative signature appcars to be somewhat complicated. We neglect these complications here.
E. P. Heifez andL. I. Perlovsky: TP-70, Inst. Mathem. (Novosibirsk, 1973);Sov. Journ. Theor. Math. Phys., in print.
A. V. Efremov andR. Peschanski: JINR E2-6350 (1972).
A. M. Polyakov:Žurn Ėksp. Teor. Fiz.,59, 542 (1970);60, 1572 (1971);61, 2193 (1971).
V. M. Budnev, A. V. Efremov andI. F. Ginzburg: JINR E2-6283 (1972). See also,e.g.,M. Lusignoli andY. Srivastava:Lett. Nuovo Cimento,4, 550 (1972).
I. F. Ginzburg andL. I. Perlovsky:Lett. Nuovo Cimento,6, 695 (1973). Cf. in this connection alsoM. Jacob andS. Nussinov:Nuovo Cimento,14 A, 335 (1973).
I. F. Ginzburg: TP-18. Inst. Mathem. (Novosibirsk, 1965);Lett. Nuovo Cimento,6, 603 (1973).
An extended version of this paper (see also TP-74 Inst. Mathem. (Novosibirsk, 1972)) and the paper ofA. V. Efremov: E2-6612 JINR (1972) will be printed inProc. Int. Conf. on Mathem. Problems of Quantum Field Theory (Moscow, 1972).
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Ginzburg, I.F. Scale invariance, elementary particles and high-energy scattering in quantum field theory. Lett. Nuovo Cimento 7, 155–159 (1973). https://doi.org/10.1007/BF02746348
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DOI: https://doi.org/10.1007/BF02746348