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Categorical properties of the complex numbers Jamie Vicary Imperial College London jamie.vicary05@imperial.ac.uk Category Theory 2008 Universit e du Littoral C ote dOpale Calais, France 23 June 2008 Category of Hilbert spaces


  1. Categorical properties of the complex numbers Jamie Vicary Imperial College London jamie.vicary05@imperial.ac.uk Category Theory 2008 Universit´ e du Littoral Cˆ ote d’Opale Calais, France 23 June 2008

  2. Category of Hilbert spaces Finite-dimensional quantum mechanics takes place in Hilb , with ◮ finite-dimensional complex Hilbert spaces as objects ◮ continuous linear maps as morphisms Symmetric monoidal structure, tensor unit is C Can access C as the scalars , Hom( I, I ) The field C is vitally important for quantum theory What are its categorical properties? Aim. Find a set of properties for a monoidal category which imply that the scalars are ‘similar’ to C . Strategy. Steal the properties of Hilb !

  3. Category of Hilbert spaces Finite-dimensional quantum mechanics takes place in Hilb , with ◮ finite-dimensional complex Hilbert spaces as objects ◮ continuous linear maps as morphisms Symmetric monoidal structure, tensor unit is C Can access C as the scalars , Hom( I, I ) The field C is vitally important for quantum theory What are its categorical properties? Aim. Find a set of properties for a monoidal category which imply that the scalars are ‘similar’ to C . Strategy. Steal the properties of Hilb !

  4. Category of Hilbert spaces Finite-dimensional quantum mechanics takes place in Hilb , with ◮ finite-dimensional complex Hilbert spaces as objects ◮ continuous linear maps as morphisms Symmetric monoidal structure, tensor unit is C Can access C as the scalars , Hom( I, I ) The field C is vitally important for quantum theory What are its categorical properties? Aim. Find a set of properties for a monoidal category which imply that the scalars are ‘similar’ to C . Strategy. Steal the properties of Hilb !

  5. Category of Hilbert spaces Finite-dimensional quantum mechanics takes place in Hilb , with ◮ finite-dimensional complex Hilbert spaces as objects ◮ continuous linear maps as morphisms Symmetric monoidal structure, tensor unit is C Can access C as the scalars , Hom( I, I ) The field C is vitally important for quantum theory What are its categorical properties? Aim. Find a set of properties for a monoidal category which imply that the scalars are ‘similar’ to C . Strategy. Steal the properties of Hilb !

  6. Category of Hilbert spaces Finite-dimensional quantum mechanics takes place in Hilb , with ◮ finite-dimensional complex Hilbert spaces as objects ◮ continuous linear maps as morphisms Symmetric monoidal structure, tensor unit is C Can access C as the scalars , Hom( I, I ) The field C is vitally important for quantum theory What are its categorical properties? Aim. Find a set of properties for a monoidal category which imply that the scalars are ‘similar’ to C . Strategy. Steal the properties of Hilb !

  7. The † -functor Definition. A † -category is a category C equipped with a † -functor , a functor † : C C which is ◮ contravariant ◮ involutive ◮ identity on objects Example: taking the adjoint of a map between Hilbert spaces f † : B f : A B A Gives a † -functor † : Hilb Hilb . A morphism f : A B is an isometry if it satisfies f † ◦ f = id A unitary if it satisfies f † ◦ f = id A and f ◦ f † = id B A is self-adjoint if f † = f A morphism f : A

  8. The † -functor Definition. A † -category is a category C equipped with a † -functor , a functor † : C C which is ◮ contravariant ◮ involutive ◮ identity on objects Example: taking the adjoint of a map between Hilbert spaces f † : B f : A B A Gives a † -functor † : Hilb Hilb . A morphism f : A B is an isometry if it satisfies f † ◦ f = id A unitary if it satisfies f † ◦ f = id A and f ◦ f † = id B A is self-adjoint if f † = f A morphism f : A

  9. The † -functor Definition. A † -category is a category C equipped with a † -functor , a functor † : C C which is ◮ contravariant ◮ involutive ◮ identity on objects Example: taking the adjoint of a map between Hilbert spaces f † : B f : A B A Gives a † -functor † : Hilb Hilb . A morphism f : A B is an isometry if it satisfies f † ◦ f = id A unitary if it satisfies f † ◦ f = id A and f ◦ f † = id B A is self-adjoint if f † = f A morphism f : A

  10. The † -functor Definition. A † -category is a category C equipped with a † -functor , a functor † : C C which is ◮ contravariant ◮ involutive ◮ identity on objects Example: taking the adjoint of a map between Hilbert spaces f † : B f : A B A Gives a † -functor † : Hilb Hilb . A morphism f : A B is an isometry if it satisfies f † ◦ f = id A unitary if it satisfies f † ◦ f = id A and f ◦ f † = id B A is self-adjoint if f † = f A morphism f : A

  11. The † -functor Definition. A † -category is a category C equipped with a † -functor , a functor † : C C which is ◮ contravariant ◮ involutive ◮ identity on objects Example: taking the adjoint of a map between Hilbert spaces f † : B f : A B A Gives a † -functor † : Hilb Hilb . A morphism f : A B is an isometry if it satisfies f † ◦ f = id A unitary if it satisfies f † ◦ f = id A and f ◦ f † = id B A is self-adjoint if f † = f A morphism f : A

  12. † -Biproducts Biproducts are defined by injections and projections. Idea: require these to be related by the † -functor.

  13. † -Biproducts Biproducts are defined by injections and projections. Idea: require these to be related by the † -functor. Definition. A † -biproduct is a biproduct for which the injections and projections are related by the † -functor. A B i A ; i A † = id A i B ; i A † = 0 B,A i A i B i A ; i B † = 0 A,B i B ; i B † = id B A ⊕ B i A † ; i A + i B † ; i B = id A ⊕ B i A † i B † A B Unique up to unique unitary isomorphism.

  14. † -Equalisers Equalisers are always monic. Idea: require these to be isometries. This is possible in Hilb . Definition (Selinger). In a † -category, a † -equaliser is an A such that e ; e † = id E . equaliser e : E Unique up to unique unitary isomorphism. In a category with a zero object, a † -functor is nondegenerate if f ; f † = 0 ⇒ f = 0 .

  15. † -Equalisers Equalisers are always monic. Idea: require these to be isometries. This is possible in Hilb . Definition (Selinger). In a † -category, a † -equaliser is an A such that e ; e † = id E . equaliser e : E Unique up to unique unitary isomorphism. In a category with a zero object, a † -functor is nondegenerate if f ; f † = 0 ⇒ f = 0 .

  16. † -Equalisers Equalisers are always monic. Idea: require these to be isometries. This is possible in Hilb . Definition (Selinger). In a † -category, a † -equaliser is an A such that e ; e † = id E . equaliser e : E Unique up to unique unitary isomorphism. In a category with a zero object, a † -functor is nondegenerate if f ; f † = 0 ⇒ f = 0 .

  17. † -Equalisers Equalisers are always monic. Idea: require these to be isometries. This is possible in Hilb . Definition (Selinger). In a † -category, a † -equaliser is an A such that e ; e † = id E . equaliser e : E Unique up to unique unitary isomorphism. In a category with a zero object, a † -functor is nondegenerate if f ; f † = 0 ⇒ f = 0 . ˜ f f A Lemma. In a † -category with a zero object and finite † -equalisers, f † k the † -functor is nondegenerate. K ⊂ B A 0 B,A f = ˜ f ; k = ˜ f ; k ; k † ; k = f ; k † ; k = 0 A,K ; k = 0 A,B .

  18. Cancellable addition What do we get if we combine † -biproducts and † -equalisers? Lemma. In a † -category with finite † -biproducts and † -equalisers, hom-set addition is cancellable : for all f, g, h in the same hom-set, f + h = g + h ⇒ f = g.

  19. Cancellable addition What do we get if we combine † -biproducts and † -equalisers? Lemma. In a † -category with finite † -biproducts and † -equalisers, hom-set addition is cancellable : for all f, g, h in the same hom-set, f + h = g + h ⇒ f = g.

  20. Cancellable addition What do we get if we combine † -biproducts and † -equalisers? Lemma. In a † -category with finite † -biproducts and † -equalisers, hom-set addition is cancellable : for all f, g, h in the same hom-set, f + h = g + h ⇒ f = g. � 0 � ˜ p = p 1 A � e 1 � e = ( f h ) e 2 E ⊂ A ⊕ A B ( g h ) � 1 � A q ˜ q = 1 Examples: Hilb has † -biproducts and † -equalisers ⇒ has cancellable addition Rel has † -biproducts, lacks cancellable addition ⇒ lacks † -equalisers

  21. Cancellable addition What do we get if we combine † -biproducts and † -equalisers? Lemma. In a † -category with finite † -biproducts and † -equalisers, hom-set addition is cancellable : for all f, g, h in the same hom-set, f + h = g + h ⇒ f = g. � 0 � ˜ p = p 1 A � e 1 � e = ( f h ) e 2 E ⊂ A ⊕ A B ( g h ) � 1 � A q ˜ q = 1 Examples: Hilb has † -biproducts and † -equalisers ⇒ has cancellable addition Rel has † -biproducts, lacks cancellable addition ⇒ lacks † -equalisers

  22. What about the complex numbers? Definition. A monoidal † -category is a monoidal category which is also a † -category, such that all of the structural isomorphisms are unitary. In a nontrivial monoidal † -category with finite † -biproducts and † -equalisers, the scalars will be ◮ commutative ◮ additively cancellable We’re on the right track!

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