# nLab BF-theory

Contents

### Context

#### $\infty$-Chern-Simons theory

∞-Chern-Weil theory

∞-Chern-Simons theory

∞-Wess-Zumino-Witten theory

## Examples

#### Quantum field theory

functorial quantum field theory

# Contents

## Idea

What is called BF-theory is a topological quantum field theory defined by an action functional $S_{BF}$ on a space of certain connections and differential forms over a 4-manifold $X$, such that locally on $X$ the space of field histories is given by

1. Lie algebra-valued 1-forms$\;A$ with values in some Lie algebra $\mathfrak{g}_1$ and with field strength/curvature 2-form $F_A$;

2. differential 2-forms$\;B$ with values in some Lie algebra $\mathfrak{g}_2$,

3. together with

1. a homomorphism $\partial \colon \mathfrak{g}_2 \to \mathfrak{g}_1$

2. an invariant polynomial $\langle -,- \rangle$

by

$S_{BF} \;\colon\; (A,B) \;\mapsto\; \int_X \langle F_A \wedge \partial B\rangle \,.$

There is not much of a proposal in the literature for how to make sense of this expression globally. It has been observed that it looks like the action functional is one on ∞-Lie algebra-valued forms with values in a strict Lie 2-algebra $\mathfrak{g} = (\mathfrak{g}_2 \stackrel{\partial}{\to} \mathfrak{g}_1)$.

This would suggest that the BF-action functional is to be regarded as a functional on the space (2-groupoid) of $G$-principal 2-bundles with connection on a 2-bundle, where $G = (G_2 \to G_1)$ is a Lie 2-group integrating $\mathfrak{g}$.

If one couples to the above action functional that for topological Yang-Mills theory and a cosmological constant with coefficients as in

$\int_X( \langle F_A \wedge B\rangle - \frac{1}{2} \langle F_A \wedge F_A\rangle - \frac{1}{2}\langle \partial B \wedge \partial B\rangle)$

then this is the generalized Chern-Simons theory action functional induced from the canonical Chern-Simons element on the strict Lie 2-algebra $\mathfrak{g}$. See Chern-Simons element for details.

## Applications

Much of the interest in BF-theory results from the fact that on a 4-dimensional manifold, to some extent the Einstein-Hilbert action for gravity may be encoded in BF-theory form. See gravity as a BF-theory.

## References

BF theory was maybe first considered in

• Gary Horowitz, Exactly soluable diffeomorphism invariant theories Commun. Math. Phys. 125, 417-437 (1989)

The observation that the BF-theory action functional looks like it should be read as a functional on a space of ∞-Lie algebra valued forms with values in a strict Lie 2-algebra possibly appears in print first in section 3.9 of

The observation that coupled to topological Yang-Mills theory it can be read as the ∞-Chern-Simons theory action functional on connections on 2-bundles is in

and a more comprehensive discussion is in section 4.3 of

• Aristide Baratin, Florian Girelli, Daniele Oriti, Diffeomorphisms in group field theories, Physical Review D, vol. 83, Issue 10, id. 104051, doi, arxiv/1101.0590

There is a more general BFCG action introduced by Girelli, Pfeiffer and Popescu which has been shown to be a special case of the categorified BF-theory in

• João Martins, Aleksandar Miković, Lie crossed modules and gauge-invariant actions for 2-BF theories, Adv. Theor. Math. Phys. 15:4 (2011), 913-1199 euclid

BF gravity

• Mariano Celada, Diego González, Merced Montesinos, BF gravity, arxiv/1610.02020

For the use of a version of BF-theory in arithmetic to deal with the non-orientability of arithmetic schemes see

Last revised on May 4, 2020 at 04:59:03. See the history of this page for a list of all contributions to it.