abstract duality: opposite category,
concrete duality: dual object, dualizable object, fully dualizable object, dualizing object
Examples
between higher geometry/higher algebra
Langlands duality, geometric Langlands duality, quantum geometric Langlands duality
In QFT and String theory
Loomis-Sikorski duality is a Stone-type duality between measurable spaces and particular (σ-complete) Boolean algebras, and it is one of the main approaches to point-free measure theory?.
It is closely related to point-free topology, as well as to measurable Gelfand duality? and to the duality between measure spaces (not measurable) and measurable locales.
Recall that a measurable space is a set equipped with a σ-algebra of subsets of . These subsets have the interpretation of “distinctions” that one can make, analogously to the open sets of a topology. Moreover, in the presence of a measure, these are precisely the subsets which have a “size” (the value of the measure), and in probability theory, they are the events to which one assigns a probability.
In point-free measure theory?, just as in point-free topology, one is interested in shifting the focus from the points of to the ordered structure of , and to study to which extent they determine one another.
Given a measurable space , the σ-algebra is by definition closed under complements and countable unions. In other words it is a σ-complete Boolean algebra (also known as Boolean σ-algebra).
Given a measurable map , the inverse image map preserves countable unions and complements, we therefore have a functor from measurable spaces to σ-complete Boolean algebras (where the morphisms are required to preserve countable unions and complements).
Let be a σ-complete Boolean algebra. We can define a point of to be any of the following equivalent structures:
Given a morphism and a point of , the composition is a point of . Denoting by the space of points of (or spectrum), we then have a function .
In order to turn this assignment into a functor , we need to equip the spaces with σ-algebras. We do it as follows (see also at zero-one measure - the monad): for every , define
The sets form a σ-algebra, and the maps are measurable. This gives the desired functor
Just as in the topological case, the functors and form a (contravariant) idempotent adjunction:
The adjunction induces an idempotent monad on (the monad of zero-one measures), and an idempotent monad on as well (or equivalently, an idempotent comonad on ).
As usual with idempotent adjunctions, we have that the center is equivalently given by
Because of this, sometimes one calls the monad on the sobrification monad.
(Work in progress. For now see the references.)
Roman Sikorski, Boolean Algebras, Springer, 1969.
Sean Moss and Paolo Perrone, Probability monads with submonads of deterministic states, LICS, 2022. (arXiv)
Ruiyuan Chen, A universal characterization of standard Borel spaces. The Journal of Symbolic Logic, 88(2), 2023. (arXiv)
Tobias Fritz and Antonio Lorenzin, Categories of abstract and noncommutative measurable spaces, 2025. (arXiv)
Last revised on June 12, 2025 at 08:57:23. See the history of this page for a list of all contributions to it.