In mathematical physics, six-dimensional holomorphic Chern–Simons theory or sometimes holomorphic Chern–Simons theory is a gauge theory on a three-dimensional complex manifold. It is a complex analogue of Chern–Simons theory, named after Shiing-Shen Chern and James Simons who first studied Chern–Simons forms which appear in the action of Chern–Simons theory. The theory is referred to as six-dimensional as the underlying manifold of the theory is three-dimensional as a complex manifold, hence six-dimensional as a real manifold. The theory has been used to study integrable systems through four-dimensional Chern–Simons theory, which can be viewed as a symmetry reduction of the six-dimensional theory. For this purpose, the underlying three-dimensional complex manifold is taken to be the three-dimensional complex projective space P 3 {\displaystyle \mathbb {P} ^{3}} , viewed as twistor space.
Formulation The background manifold W {\displaystyle {\mathcal {W}}} on which the theory is defined is a complex manifold which has three complex dimensions and therefore six real dimensions. The theory is a gauge theory with gauge group a complex, simple Lie group G . {\displaystyle G.} The field content is a partial connection A ¯ {\displaystyle {\bar {\mathcal {A}}}} . The action is
S H C S [ A ¯ ] = 1 2 π i ∫ W Ω ∧ H C S ( A ¯ ) {\displaystyle S_{\mathrm {HCS} }[{\bar {\mathcal {A}}}]={\frac {1}{2\pi i}}\int _{\mathcal {W}}\Omega \wedge \mathrm {HCS} ({\bar {\mathcal {A}}})}
where
H C S ( A ¯ ) = t r ( A ¯ ∧ ∂ ¯ A ¯ + 2 3 A ¯ ∧ A ¯ ∧ A ¯ ) {\displaystyle \mathrm {HCS} ({\bar {\mathcal {A}}})=\mathrm {tr} \left({\bar {\mathcal {A}}}\wedge {\bar {\partial }}{\bar {\mathcal {A}}}+{\frac {2}{3}}{\bar {\mathcal {A}}}\wedge {\bar {\mathcal {A}}}\wedge {\bar {\mathcal {A}}}\right)}
where Ω {\displaystyle \Omega } is a holomorphic (3,0)-form and with t r {\displaystyle \mathrm {tr} } denoting a trace functional which as a bilinear form is proportional to the Killing form.
On twistor space P3 Here W {\displaystyle {\mathcal {W}}} is fixed to be P 3 {\displaystyle \mathbb {P} ^{3}} . For application to integrable theory, the three form Ω {\displaystyle \Omega } must be chosen to be meromorphic.
See also Chern–Simons theory Four-dimensional Chern-Simons theory Infinite-dimensional Chern–Simons theory
External links Holomorphic Chern–Simons theory nLab
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