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BF model : ウィキペディア英語版
BF model
The BF model is a topological field, which when quantized, becomes a topological quantum field theory. BF stands for background field. B and F, as can be seen below, are also the variables appearing in the Lagrangian of the theory, which is helpful as a mnemonic device.

We have a 4-dimensional differentiable manifold M, a gauge group G, which has as "dynamical" fields a two-form B taking values in the adjoint representation of G, and a connection form A for G.
The action is given by
:S=\int_M K(\mathbf )
where K is an invariant nondegenerate bilinear form over \mathfrak (if G is semisimple, the Killing form will do) and F is the curvature form
:\mathbf\equiv d\mathbf+\mathbf\wedge \mathbf
This action is diffeomorphically invariant and gauge invariant. Its Euler–Lagrange equations are
:\mathbf=0 (no curvature)
and
:d_\mathbfB=0 (the covariant exterior derivative of B is zero).
In fact, it is always possible to gauge away any local degrees of freedom, which is why it is called a topological field theory.
However, if M is topologically nontrivial, A and B can have nontrivial solutions globally.
== See also ==

* Spin foam
* Background field method

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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