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| {{dablink|For applications to 4-manifolds see ]}} | {{dablink|For applications to 4-manifolds see ]}} | ||
| In ], '''Seiberg-Witten gauge theory''' is a set of calculations that determine the low-energy |
In ], '''Seiberg-Witten gauge theory''' is a set of calculations that determine the low-energy physics—namely the ] and the masses of electrically and ] supersymmetric particles as a function of the moduli space. | ||
| This is possible and nontrivial in ] with ''N'' = 2 ] by combining the fact that various parameters of the ] are ]s (a consequence of supersymmetry) and the known behavior of the theory in the classical limit. | This is possible and nontrivial in ] with ''N'' = 2 ] by combining the fact that various parameters of the ] are ]s (a consequence of supersymmetry) and the known behavior of the theory in the classical limit. | ||
| The moduli space in the full quantum theory has a slightly different structure from that in the classical theory. | The moduli space in the full quantum theory has a slightly different structure from that in the classical theory. | ||
| ==See also== | |||
| *] | |||
| ==External links== | ==External links== | ||
| * | * | ||
| ⚫ | {{phys-stub}} | ||
| ] | ] | ||
| ] | ] | ||
| ⚫ | {{phys-stub}} | ||
| ] | ] | ||
Revision as of 00:57, 28 March 2010
For applications to 4-manifolds see Seiberg–Witten invariantIn theoretical physics, Seiberg-Witten gauge theory is a set of calculations that determine the low-energy physics—namely the moduli space and the masses of electrically and magnetically charged supersymmetric particles as a function of the moduli space.
This is possible and nontrivial in gauge theory with N = 2 extended supersymmetry by combining the fact that various parameters of the Lagrangian are holomorphic functions (a consequence of supersymmetry) and the known behavior of the theory in the classical limit.
The moduli space in the full quantum theory has a slightly different structure from that in the classical theory.
See also
External links
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