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Yang-Mills gauge field theory

Gauge theories, Yang-Mills field, 204-205 Gauge transformation ... [Pg.78]

Neumann boundary conditions, electronic states, adiabatic-to-diabatic transformation, two-state system, 304-309 Newton-Raphson equation, conical intersection location locations, 565 orthogonal coordinates, 567 Non-Abelian theory, molecular systems, Yang-Mills fields nuclear Lagrangean, 250 pure vs. tensorial gauge fields, 250-253 Non-adiabatic coupling ... [Pg.88]

A simple example in classical electrodynamics of what is now known as gauge invariance was introduced by Heaviside [3,4], who reduced the original electrodynamical equations of Maxwell to their present form. Therefore, these equations are more properly known as the Maxwell-Heaviside equations and, in the terminology of contemporary gauge field theory, are identifiable as U(l) Yang-Mills equations [15]. The subj ect of this chapter is 0(3) Yang-Mills gauge theory applied to electrodynamics and electroweak theory. [Pg.86]


See other pages where Yang-Mills gauge field theory is mentioned: [Pg.637]    [Pg.768]    [Pg.270]    [Pg.42]    [Pg.80]    [Pg.82]    [Pg.103]    [Pg.125]    [Pg.176]    [Pg.192]    [Pg.460]    [Pg.155]    [Pg.561]    [Pg.346]   
See also in sourсe #XX -- [ Pg.204 ]

See also in sourсe #XX -- [ Pg.204 ]




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