Abstract
An important, and highly non-trivial, problem is proving the renormalizability and unitarity of quantized non-Abelian gauge theories. Lee and Zinn-Justin have given the first proof of the renormalizability of non-Abelian gauge theories in the spontaneously broken phase. An essential ingredient in the proof has been the observation, by Slavnov and Taylor, of a non-linear, non-local symmetry of the quantized theory, a direct consequence of Faddeev and Popov’s quantization procedure. After the introduction of non-physical fermions to represent the Faddeev-Popov determinant, this symmetry has led to the Becchi-Rouet-Stora-Tyutin fermionic symmetry of the quantized action and, finally, to the resulting Zinn-Justin equation, which makes it possible to solve the renormalization and unitarity problems in their full generality. For an elementary introduction to the discussion of quantum non-Abelian gauge field theories in the spirit of the article, see, for example, L. D. Faddeev, “Faddeev-Popov ghosts,” Scholarpedia 4 (4), 7389 (2009); A. A. Slavnov, “Slavnov-Taylor identities,” Scholarpedia 3 (10), 7119 (2008); C. M. Becchi and C. Imbimbo, “Becchi-Rouet-Stora-Tyutin symmetry,” Scholarpedia 3 (10), 7135 (2008); J. Zinn-Justin, “Zinn-Justin equation,” Scholarpedia 4 (1), 7120 (2009).
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In honour of the 80th birthday of my very esteemed colleague and friend A. A. Slavnov
Published in Russian in Trudy Matematicheskogo Instituta imeni V.A. Steklova, 2020, Vol. 309, pp. 338–345.
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Zinn-Justin, J. From Slavnov—Taylor Identities to the Renormalization of Gauge Theories. Proc. Steklov Inst. Math. 309, 317–324 (2020). https://doi.org/10.1134/S0081543820030232
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DOI: https://doi.org/10.1134/S0081543820030232