algebraic quantum field theory (perturbative, on curved spacetimes, homotopical)
quantum mechanical system, quantum probability
interacting field quantization
A C*-category can be thought of as a horizontal categorification of a C*-algebra. Equivalently, a C*-algebra is thought of as a pointed one-object C*-category (the delooping of ). Accordingly, a more systematic name for C*-categories would be C*-algebroids.
A (unital) C*-category is a *-category enriched in the category Ban of Banach spaces such that:
Every arrow satisfies the C*-identity .
Composition satisfies for all composable pairs of arrows and . (That is, we give the projective tensor product.)
For every arrow there exists an arrow such that .
Condition (3) above is equivalent to requiring that every arrow of the form is positive in the sense of C*-algebras. Unlike C*-algebras, this does not follow automatically, as can be seen by considering the category with two objects with all morphism sets a copy of and with involution defined on by if and otherwise.
A C*-category can be defined analogously to unital C*-categories, using enriched nonunital categories instead of (unital) enriched categories.
The -representation category of a weak Hopf -algebra (see there for details) is naturally a rigid monoidal -category.
The category of Hilbert spaces and bounded linear maps is a C*-category.
C*-algebras can be represented as algebras of bounded linear operators on some choice of Hilbert space, using the G.N.S. construction. C*-categories have an analogue of the G.N.S. construction that allows them to represented on the category of Hilbert spaces and bounded linear maps.
For any (small) C*-category there exists a faithful *-functor .
With emphasis on the special case of -categories:
Last revised on January 13, 2024 at 13:09:51. See the history of this page for a list of all contributions to it.