symmetric monoidal (∞,1)-category of spectra
With braiding
With duals for objects
category with duals (list of them)
dualizable object (what they have)
ribbon category, a.k.a. tortile category
With duals for morphisms
monoidal dagger-category?
With traces
Closed structure
Special sorts of products
Semisimplicity
Morphisms
Internal monoids
Examples
Theorems
In higher category theory
monoid theory in algebra:
For and two commutative monoids, their tensor product is a new commutative monoid such that a monoid homomorphism is equivalently a bilinear map out of and .
Another way to think of it is that commutative monoid maps are in natural bijection with commutative monoid maps , where is the set of commutative monoid maps provided with the pointwise-defined commutative monoid structure.
Let CMon be the collection of commutative monoids, regarded as a multicategory whose multimorphisms are the multilinear maps .
The tensor product in this multicategory is the tensor product of commutative monoids.
Equivalently this means explicitly:
For two commutative monoids, their tensor product of commutative monoids is the commutative monoid which is the quotient of the free commutative monoid on the product of their underlying sets by the relations
for all and .
By definition of the free construction and the quotient there is a canonical function of the underlying sets
(where is the forgetful functor).
On elements this sends to the equivalence class that it represents under the above equivalence relations.
The following relates the tensor product to bilinear functions. It is a definition or a proposition depending on whether one takes the notion of bilinear function to be defined before or after that of tensor product of commutative monoids.
A function of underlying sets is a bilinear function precisely if it factors by the morphism of through a monoid homomorphism out of the tensor product:
Equipped with the tensor product of def. and the exchange map generated by , CMon becomes a symmetric monoidal category.
The unit object in is the additive monoid of natural numbers .
To see that is the unit object, consider for any commutative monoid the map
which sends for
Due to the quotient relation defining the tensor product, the element on the left is also equal to
This shows that is in fact an isomorphism.
Showing that is natural in is trivial, so is a braiding. is identity, so it gives CMon a symmetric monoidal structure.
Notice the symmetry or braiding provides a natural isomorphism .
The symmetric monoidal structure is naturally seen as adjoint to a closed structure, where the internal hom of commutative monoids, whose underlying set consists of commutative monoid maps , is defined in pointwise fashion:
That so defined is a homomorphism uses commutativity in the monoid :
Given , define by . The linearity of in the second argument follows from the fact that is a linear map. The linearity in the first argument follows from the fact that is itself linear, and the pointwise-defined structure of :
In the other direction, given , define by . The linearity of follows from an argument similar to the one in the paragraph above. The fact that the assignments and are mutually inverse is obvious.
Since and its isomorph are thus left adjoint functors, and since left adjoints preserve coproducts, we also have the following result.
The tensor product of commutative monoids distributes over the biproduct of commutative monoids
Let be a monoid in . The fact that the multiplication
is bilinear means by the above that for all we have
This is precisely the distributivity law and absorption law of the rig.
The assignment satisfies base change for presentable (∞,1)-categories, i.e.
In particular, is a mode; this implies that for a presentably symmetric monoidal(∞,1)-category, possesses a unique symmetric monoidal structure subject to the condition that the free functor
is symmetric monoidal. This is due to Gepner-Groth-Nikolaus
Last revised on May 20, 2025 at 13:56:50. See the history of this page for a list of all contributions to it.