By Chris Heunen
This dissertation stories the common sense in the back of quantum physics, utilizing classification idea because the significant software and conceptual advisor. to take action, ideas of quantum mechanics are modeled categorically. those specific quantum types are justified by means of an embedding into the class of Hilbert areas, the conventional formalism of quantum physics. particularly, complicated numbers emerge with no need been prescribed explicitly. reading good judgment in such different types leads to orthomodular estate lattices, and in addition presents a usual surroundings to contemplate quantifiers. ultimately, topos concept, incorporating specific good judgment in a polished method, we could one research a quantum approach as though it have been classical, particularly resulting in a singular mathematical thought of quantum-
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Additional resources for Categorical Quantum Models and Logics (Pallas Proefschriften)
X∈f −1 (y) R is a monad in Set. Its unit η : X → R(X) is given by the Kronecker function η(x)(x ) = 1 0 if x = x , otherwise. Its multiplication µ : R(R(X)) → R(X) is matrix multiplication Φ(ϕ) · ϕ(x). µ(Φ)(x) = b ϕ∈R(X) In fact, ( ) is a functor from Rg to the category of monads on Set. The category of (Eilenberg-Moore) algebras of R is ModR . 4]. e. e. coequalisers of a morphism and the zero morphism. Moreover, as the construction of finite biproducts in ModR for a ring R does not need subtraction of scalars, it descends to ModR for a rig R.
Likewise, a product X1 × X2 comes with projections that we denote by π, π1 π2 G X2 . e. there is a unique morphism X → 1 for every object X. e. the tuple id , id : X → X × X, by ∆. The following theorem characterises algebraically when a monoidal product is a coproduct, without any reference to universal properties, in a way reminiscent of  (see also ). 2 Theorem A symmetric monoidal structure (⊕, 0) on a category C provides finite coproducts if and only if the forgetful functor cMon(C) → C is an isomorphism of categories.
All n-dimensional manifolds form the objects of a category whose morphisms are so-called cobordisms. These are n + 1-dimensional manifolds, whose boundary is the disjoint union of its domain and codomain manifolds. This category is a dagger category; the dagger of a cobordism is its reversal . 8 Example This example describes ‘the mother of all dagger categories’. A functor ∗ : Cop → C is called involutive when ∗ ◦ ∗ = Id. ) Define a category InvAdj as follows. Its objects are pairs (C, ∗) of a category with an involution.
Categorical Quantum Models and Logics (Pallas Proefschriften) by Chris Heunen