Symmetric monoidal category

{{Short description|Monoidal category where A ⊗ B is naturally equivalent to B ⊗ A}}In category theory, a branch of mathematics, a symmetric monoidal category is a monoidal category (i.e. a category in which a "tensor product" $\otimes$ is defined) such that the tensor product is symmetric (i.e. $A\otimes B$ is, in a certain strict sense, naturally isomorphic to $B\otimes A$ for all objects $A$ and $B$ of the category). One of the prototypical examples of a symmetric monoidal category is the category of vector spaces over some fixed field k, using the ordinary tensor product of vector spaces.

Definition

A symmetric monoidal category is a monoidal category (C, ⊗, I) such that, for every pair A, B of objects in C, there is an isomorphism $s_{AB}: A \otimes B \to B \otimes A$ called the swap map{{Cite arXiv |last1=Fong |first1=Brendan |last2=Spivak |first2=David I. |date=2018-10-12 |title=Seven Sketches in Compositionality: An Invitation to Applied Category Theory |class=math.CT |eprint=1803.05316 }} that is natural in both A and B and such that the following diagrams commute:

The unit coherence:
:File:symmetric monoidal unit coherence.png
The associativity coherence:
:File:symmetric monoidal associativity coherence.png
The inverse law:
:File:symmetric monoidal inverse law.png

In the diagrams above, a, l, and r are the associativity isomorphism, the left unit isomorphism, and the right unit isomorphism respectively.

Examples

Some examples and non-examples of symmetric monoidal categories:

The category of sets. The tensor product is the set theoretic cartesian product, and any singleton can be fixed as the unit object.
The category of groups. Like before, the tensor product is just the cartesian product of groups, and the trivial group is the unit object.
More generally, any category with finite products, that is, a cartesian monoidal category, is symmetric monoidal. The tensor product is the direct product of objects, and any terminal object (empty product) is the unit object.
The category of bimodules over a ring R is monoidal (using the ordinary tensor product of modules), but not necessarily symmetric. If R is commutative, the category of left R-modules is symmetric monoidal. The latter example class includes the category of all vector spaces over a given field.
Given a field k and a group (or a Lie algebra over k), the category of all k-linear representations of the group (or of the Lie algebra) is a symmetric monoidal category. Here the standard tensor product of representations is used.
The categories (Ste, $\circledast$ ) and (Ste, $\odot$ ) of stereotype spaces over ${\mathbb C}$ are symmetric monoidal, and moreover, (Ste, $\circledast$ ) is a closed symmetric monoidal category with the internal hom-functor $\oslash$ .

Properties

The classifying space (geometric realization of the nerve) of a symmetric monoidal category is an $E_\infty$ space, so its group completion is an infinite loop space.{{cite journal |author-link=Robert Wayne Thomason |first=R.W. |last=Thomason |url=http://www.tac.mta.ca/tac/volumes/1995/n5/v1n5.pdf |title=Symmetric Monoidal Categories Model all Connective Spectra |journal=Theory and Applications of Categories |volume=1 |issue=5 |date=1995 |pages=78–118 |citeseerx=10.1.1.501.2534 }}

Specializations

A dagger symmetric monoidal category is a symmetric monoidal category with a compatible dagger structure.

A cosmos is a complete cocomplete closed symmetric monoidal category.

Generalizations

In a symmetric monoidal category, the natural isomorphisms $s_{AB}: A \otimes B \to B \otimes A$ are their own inverses in the sense that $s_{BA}\circ s_{AB}=1_{A\otimes B}$ . If we abandon this requirement (but still require that $A\otimes B$ be naturally isomorphic to $B\otimes A$ ), we obtain the more general notion of a braided monoidal category.

References

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Category:Monoidal categories