Chern–Simons form

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Short description: Secondary characteristic classes of 3-manifolds

In mathematics, the Chern–Simons forms are certain secondary characteristic classes.[1] The theory is named for Shiing-Shen Chern and James Harris Simons, co-authors of a 1974 paper entitled "Characteristic Forms and Geometric Invariants," from which the theory arose.[2]

Definition

Given a manifold and a Lie algebra valued 1-form 𝐀 over it, we can define a family of p-forms:[3]

In one dimension, the Chern–Simons 1-form is given by

Tr[𝐀].

In three dimensions, the Chern–Simons 3-form is given by

Tr[𝐅𝐀13𝐀𝐀𝐀]=Tr[d𝐀𝐀+23𝐀𝐀𝐀].

In five dimensions, the Chern–Simons 5-form is given by

Tr[𝐅𝐅𝐀12𝐅𝐀𝐀𝐀+110𝐀𝐀𝐀𝐀𝐀]=Tr[d𝐀d𝐀𝐀+32d𝐀𝐀𝐀𝐀+35𝐀𝐀𝐀𝐀𝐀]

where the curvature F is defined as

𝐅=d𝐀+𝐀𝐀.

The general Chern–Simons form ω2k1 is defined in such a way that

dω2k1=Tr(Fk),

where the wedge product is used to define Fk. The right-hand side of this equation is proportional to the k-th Chern character of the connection 𝐀.

In general, the Chern–Simons p-form is defined for any odd p.[4]

Application to physics

In 1978, Albert Schwarz formulated Chern–Simons theory, early topological quantum field theory, using Chern-Simons forms.[5]

In the gauge theory, the integral of Chern-Simons form is a global geometric invariant, and is typically gauge invariant modulo addition of an integer.

See also

References

Further reading