Fix an algebraically closed field kk. A fusion category over kk is an essentially small with a , such that:

  1. each vector space Hom⁡(X,Y)\operatorname{Hom}(X,Y) is finite-dimensional;
  2. there are finitely many isomorphism classes of ;
  3. the tensor product is kk-bilinear on morphisms;
  4. the tensor unit 1\mathbb1 is simple.

Here semisimplicity means every object is a finite direct sum of simples. Essentially small means that the isomorphism classes of objects form a set. Many treatments additionally assume char⁡k=0\operatorname{char}k=0; that assumption will be stated whenever needed here.

Unpacking the bundle
IngredientWhat it lets you do
Form kernels, cokernels, and exact sequences.
Add and scale parallel arrows.
Decompose objects into finite sums of simple pieces.
Tensor objects and arrows, with coherent associativity and unit maps.
Evaluate and coevaluate left and right duals.
Finiteness and simple unitUse a finite list of simple building blocks and an indecomposable tensor identity.

Neither nor symmetry is required. Forgetting the simple-unit condition gives a . Equivalently, a fusion category is a semisimple .

Fusion of simple objects

Choose simple representatives S0=1,S1,…,SrS_0=\mathbb1,S_1,\ldots,S_r. Their tensor products decompose as

Si⊗Sj≅⨁ℓ=0rSℓ⊕Nijℓ,Nijℓ=dim⁡kHom⁡(Sℓ,Si⊗Sj).S_i\otimes S_j\cong\bigoplus_{\ell=0}^{r}S_\ell^{\oplus N_{ij}^{\ell}}, \qquad N_{ij}^{\ell}=\dim_k\operatorname{Hom}(S_\ell,S_i\otimes S_j).

The nonnegative integers NijℓN_{ij}^{\ell} are the fusion multiplicities. These integers do not specify the associator; the monoidal coherence data remain part of the category.

Examples

Finite-dimensional kk-vector spaces form a fusion category with one simple class. For a finite group GG and char⁡k=0\operatorname{char}k=0, finite-dimensional representations of GG give another example.

Finite-dimensional GG-graded vector spaces, with (V⊗W)g=⨁ab=gVa⊗Wb(V\otimes W)_g=\bigoplus_{ab=g}V_a\otimes W_b, give an example for any finite group GG. Simples are one-dimensional spaces concentrated in a single degree. If GG is nonabelian, this category cannot be braided: the simple tensor products in degrees ghgh and hghg would otherwise have to be isomorphic.

The unit and the ground field

Under the hypotheses above, simplicity of 1\mathbb1 is equivalent to End⁡(1)≅k\operatorname{End}(\mathbb1)\cong k. In a semisimple category, a decomposition into two nonzero summands gives a nontrivial idempotent endomorphism, so an endomorphism algebra equal to kk forces simplicity. Conversely, simplicity, finite-dimensional Hom spaces, and algebraic closure force its endomorphisms to be scalars. The finite-dimensionality and ground-field assumptions should not be dropped from that converse.

References

P. Etingof, S. Gelaki, D. Nikshych, and V. Ostrik, Tensor Categories (2015), §4.1 and §4.9; author-hosted text.