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References
W. Siegel, Nucl. Phys. B156, 135 (1979); R. Jackiw and S. Templeton, Phys. Rev. D23, 2291 (1981); J. Schonfeld, Nucl. Phys. B185, 157 (1981); S. Deser, R. Jackiw and S. Templeton, Phys. Rev. Lett. 48, 975 (1982) and Ann. Phys. (NY) 140, 372 (1982); H. Nielsen and H. Woo (unpublished).
Other reviews are R. Jackiw in “Asymptotic Realms of Physics” (A. Guth, K. Huang, and R. Jaffe, editors), MIT Press, Cambridge, MA, 1983 and Arctic Summer School Proceedings (1982); S. Deser, DeWitt Festschrift, to appear.
R. Jackiw and C. Rebbi, Phys. Rev. Lett. 37, 172 (1976); R. Jackiw, Rev. Mod. Phys. 52, 661 (1980).
S. Chern, “Complex Manifolds without Potential Theory”, 2 ed. Springer Verlag, Berlin, 1979.
See Deser, Jackiw and Templeton, Ref. 1; Deser, Ref. 2.
The canonical description is due to J. Goldstone and E. Witten unpublished; for details see Jackiw, Ref. 2(second cited work).
An analogous quantization condition has been obtained by E. Witten in a 4-dimensional SU(2) gauge theory, Princeton University preprint (unpublished). One begins with the observation that Π4(SU(2)) = Π4(S3) = cyclic group of two integers, to conclude that the 4-dimensional gauge functions U(t,\(\vec x\)) fall into two homotopically distinct classes. Next one finds that when N species of left-handed Weyl fermions in the fundamental [doublet] representation are coupled to the SU(2) gauge field, their functional [fermionic] determinant is not invariant against homotopically non-trivial gauge transformations. Rather it changes by the factor (−1)N; hence N must be even.
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© 1983 Springer-Verlag
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Jackiw, R. (1983). Massive gauge theories in three dimensions (= at high temperature). In: Kikkawa, K., Nakanishi, N., Nariai, H. (eds) Gauge Theory and Gravitation. Lecture Notes in Physics, vol 176. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-11994-9_7
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DOI: https://doi.org/10.1007/3-540-11994-9_7
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