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- W207201209 abstract "One of the most familiar non-covariant gauges is the Coulomb gauge defined by ∂kAk (x) = 0, k = 1,2,3, with applications mainly in quantum electrodynamics (Ak is the photon field). In non-Abelian models, the dominant non-covariant gauge is the general axial gauge which includes the pure axial gauge, the light-cone gauge and the temporal gauge; the latter are characterized by $$ {n^mu }A_mu ^a(x) = 0,mu = 0,1,2,3, {n^2} = n_o^2 - {vec n^2}, $$ where nµ = (no,n) is a fixed vector and A µ a a massless Yang-Mills field, a = 1,2,...,N2-1 for SU(N). The corresponding gauge-fixing part of the Lagrangian density reads $$ {L_{fix}} = - {1 over {2alpha }}{(n{A^a})^2},alpha to 0,alpha $$ gauge parameter." @default.
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- W207201209 date "1989-01-01" @default.
- W207201209 modified "2023-09-27" @default.
- W207201209 title "Practical Look at Non-Covariant Gauges" @default.
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- W207201209 doi "https://doi.org/10.1007/978-3-642-74136-4_77" @default.
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