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Gauge Theory


Gauge theory studies principal bundle connections, called gauge fields, on a principal bundle. These connections correspond to fields, in physics, such as an electromagnetic field, and the Lie group of the principal bundle corresponds to the symmetries of the physical system. The base manifold to the principal bundle is usually a four-dimensional manifold which corresponds to space-time. In the case of an electromagnetic field, the symmetry group is the unitary group U(1)={e^(itheta)}. The other two groups that arise in physical theories are the special unitary groups SU(2) and SU(3). Also, a group representation V of the symmetry group, called internal space, gives rise to an associated vector bundle.

The principal bundle connections of interest include critical points of an energy functional. For example, Yang-Mills connections are critical points of the Yang-Mills functional and need not minimize it. These connections are useful in low-dimensional topology. In fact, in Donaldson theory, the collection of Yang-Mills connections gives topological invariants of the base manifold M.


See also

Group Representation, Lie Group, Manifold, Principal Bundle, Seiberg-Witten Equations, Vector Bundle, Yang-Mills Theory

Portions of this entry contributed by Todd Rowland

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References

Friedman, R. and Morgan, J. W. (Eds.). Gauge Theory and the Topology of Four-Manifolds. Providence, RI: Amer. Math. Soc., 1998.Naber, G. Topology, Geometry, and Gauge Fields. New York: Springer-Verlag, 2000.

Referenced on Wolfram|Alpha

Gauge Theory

Cite this as:

Weisstein, Eric W., with contributions by Todd Rowland. "Gauge Theory." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/GaugeTheory.html

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