Categories and Quantum Informatics
|
|
- Ralph Hart
- 5 years ago
- Views:
Transcription
1 Categories and Quantum Informatics Week 6: Frobenius structures Chris Heunen 1 / 41
2 Overview Frobenius structure: interacting co/monoid, self-duality Normal forms: coherence theorem Frobenius law: coherence between dagger and closure Classification: in FHilb and Rel Phases: unitary operators 2 / 41
3 Idea Orthonormal basis { } for H in FHilb gives comonoid :. Its adjoint is comparison: and e j 0 if i j. 3 / 41
4 Idea Orthonormal basis { } for H in FHilb gives comonoid :. Its adjoint is comparison: and e j 0 if i j. These cooperate: e j e j if i j 0 if i j e j 3 / 41
5 Idea Orthonormal basis { } for H in FHilb gives comonoid :. Its adjoint is comparison: and e j 0 if i j. These cooperate: e j e j if i j 0 if i j e j This monoid/comonoid interaction is called the Frobenius law. 3 / 41
6 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: 4 / 41
7 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: If, called dagger Frobenius structure. 4 / 41
8 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: If, called dagger Frobenius structure. Examples of dagger Frobenius structures: In FHilb: a Hilbert space equipped with an orthogonal basis 4 / 41
9 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: If, called dagger Frobenius structure. Examples of dagger Frobenius structures: In FHilb: a Hilbert space equipped with an orthogonal basis In FHilb: let G be finite group, spanning Hilbert space A. Define group algebra : g h gh, and : z z 1 G. 4 / 41
10 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: If, called dagger Frobenius structure. Examples of dagger Frobenius structures: In FHilb: a Hilbert space equipped with an orthogonal basis In FHilb: let G be finite group, spanning Hilbert space A. Define group algebra : g h gh, and : z z 1 G. Adjoint: : h G gh 1 h, and : 1 G g and 1 G g 0. 4 / 41
11 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: If, called dagger Frobenius structure. Examples of dagger Frobenius structures: In FHilb: a Hilbert space equipped with an orthogonal basis In FHilb: let G be finite group, spanning Hilbert space A. Define group algebra : g h gh, and : z z 1 G. Adjoint: : h G gh 1 h, and : 1 G g and 1 G g 0. Frobenius law: LHS(g h) k G gk 1 kh RHS(g h). 4 / 41
12 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: If, called dagger Frobenius structure. Examples of dagger Frobenius structures: In FHilb: a Hilbert space equipped with an orthogonal basis In FHilb: let G be finite group, spanning Hilbert space A. Define group algebra : g h gh, and : z z 1 G. Adjoint: : h G gh 1 h, and : 1 G g and 1 G g 0. Frobenius law: LHS(g h) k G gk 1 kh RHS(g h). In Rel: let G be groupoid. Monoid in Rel: : (g, h) g h, and : id X. 4 / 41
13 Frobenius structures In a monoidal category, a Frobenius structurs a comonoid (A,, ) and monoid (A,, ) satisfying the Frobenius law: If, called dagger Frobenius structure. Examples of dagger Frobenius structures: In FHilb: a Hilbert space equipped with an orthogonal basis In FHilb: let G be finite group, spanning Hilbert space A. Define group algebra : g h gh, and : z z 1 G. Adjoint: : h G gh 1 h, and : 1 G g and 1 G g 0. Frobenius law: LHS(g h) k G gk 1 kh RHS(g h). In Rel: let G be groupoid. Monoid in Rel: : (g, h) g h, and : id X. Frobenius law: (g, h) (a, b h) for g a b, t(h) s(b). 4 / 41
14 Pair of pants In a dagger monoidal category, if A A, the pair of pants monoid A A carries a dagger Frobenius structure. 5 / 41
15 Pair of pants In a dagger monoidal category, if A A, the pair of pants monoid A A carries a dagger Frobenius structure. Proof. 5 / 41
16 Extended Frobenius law Any Frobenius structure satisfies: 6 / 41
17 Extended Frobenius law Any Frobenius structure satisfies: Proof. 6 / 41
18 Speciality If copies orthogonal basis { }, can find (squared) norm of : and 7 / 41
19 Speciality If copies orthogonal basis { }, can find (squared) norm of : and So can characterize orthonormality via Frobenius structure. 7 / 41
20 Speciality If copies orthogonal basis { }, can find (squared) norm of : and So can characterize orthonormality via Frobenius structure. A Frobenius structurs special if: 7 / 41
21 Speciality If copies orthogonal basis { }, can find (squared) norm of : and So can characterize orthonormality via Frobenius structure. A Frobenius structurs special if: Examples: 7 / 41
22 Speciality If copies orthogonal basis { }, can find (squared) norm of : and So can characterize orthonormality via Frobenius structure. A Frobenius structurs special if: Examples: Group algebra in FHilb is only special for trivial group 7 / 41
23 Speciality If copies orthogonal basis { }, can find (squared) norm of : and So can characterize orthonormality via Frobenius structure. A Frobenius structurs special if: Examples: Group algebra in FHilb is only special for trivial group Orthogonal basis in FHilb is special just when basis is orthonormal 7 / 41
24 Speciality If copies orthogonal basis { }, can find (squared) norm of : and So can characterize orthonormality via Frobenius structure. A Frobenius structurs special if: Examples: Group algebra in FHilb is only special for trivial group Orthogonal basis in FHilb is special just when basis is orthonormal Groupoid Frobenius structurn Rel is always special 7 / 41
25 Classical structures In a braided monoidal dagger category, a classical structurs a special commutative dagger Frobenius structure. 8 / 41
26 Classical structures In a braided monoidal dagger category, a classical structurs a special commutative dagger Frobenius structure. Examples: In FHilb: an orthonormal basis In Rel: abelian group 8 / 41
27 Classical structures In a braided monoidal dagger category, a classical structurs a special commutative dagger Frobenius structure. Examples: In FHilb: an orthonormal basis In Rel: abelian group Definition of classical structure redundant: (Co)commutativity implies half of (co)unitality Speciality and Frobenius law imply (co)associativity Dual object and Frobenius law imply (co)unitality 8 / 41
28 Classical structures In a braided monoidal dagger category, a classical structurs a special commutative dagger Frobenius structure. Examples: In FHilb: an orthonormal basis In Rel: abelian group Definition of classical structure redundant: (Co)commutativity implies half of (co)unitality Speciality and Frobenius law imply (co)associativity Dual object and Frobenius law imply (co)unitality To check that (A,, ) is classical structure, only need: 8 / 41
29 Symmetry Pair of pants hardly ever commutative. However: A Frobenius structurs symmetric when: 9 / 41
30 Symmetry Pair of pants hardly ever commutative. However: A Frobenius structurs symmetric when: In a compact category, this is equivalent to the following: 9 / 41
31 Symmetry Pair of pants hardly ever commutative. However: A Frobenius structurs symmetric when: In a compact category, this is equivalent to the following: Examples: Pair of pants: in FHilb this says Tr(ab) Tr(ba) Group algebras: inverses in groups are two-sided inverses Groupoid Frobenius structure: inverses are two-sided 9 / 41
32 Self-duality If (A,,,, ) Frobenius structurn monoidal category, then A A is self-dual with: A A A A A A A A 10 / 41
33 Self-duality If (A,,,, ) Frobenius structurn monoidal category, then A A is self-dual with: A A A A A A A A Proof. 10 / 41
34 Nondegenerate forms Monoid (A,, ) forms Frobenius structure with comonoid (A,, ) iff allows nondegenerate form: map : A I with part of self-duality A A. 11 / 41
35 Nondegenerate forms Monoid (A,, ) forms Frobenius structure with comonoid (A,, ) iff allows nondegenerate form: map : A I with part of self-duality A A. Proof. One direction is the previous theorem. 11 / 41
36 Nondegenerate forms Monoid (A,, ) forms Frobenius structure with comonoid (A,, ) iff allows nondegenerate form: map : A I with part of self-duality A A. Proof. One direction is the previous theorem. Conversely, suppose I η A A satisfies: η η 11 / 41
37 Nondegenerate forms Monoid (A,, ) forms Frobenius structure with comonoid (A,, ) iff allows nondegenerate form: map : A I with part of self-duality A A. Proof. One direction is the previous theorem. Conversely, suppose I η A A satisfies: η η Define comultiplication as: η 11 / 41
38 Nondegenerate forms Proof (continued.) Could have defined the comultiplication with η left or right: η η η η η η 12 / 41
39 Nondegenerate forms Proof (continued.) Could have defined the comultiplication with η left or right: η η η η η η Counitality: η η η 12 / 41
40 Nondegenerate forms Proof (continued.) Coassociativity: η η η η η η 13 / 41
41 Nondegenerate forms Proof (continued.) Coassociativity: η η η η η η Frobenius law: η η 13 / 41
42 Homomorphisms A homomorphism of Frobenius structures is morphism which is both monoid and comonoid homomorphism. 14 / 41
43 Homomorphisms A homomorphism of Frobenius structures is morphism which is both monoid and comonoid homomorphism. They arsomorphisms. Proof. Given homomorphism A f B, construct inverse as: f 1 f 14 / 41
44 Homomorphisms A homomorphism of Frobenius structures is morphism which is both monoid and comonoid homomorphism. They arsomorphisms. Proof. Given homomorphism A f B, construct inverse as: f 1 f Indeed: f f f 14 / 41
45 Normal forms Two ways to think about graphical calculus: diagram represents morphism: merely shorthand to write down e.g. linear map; diagram is entity in its own right: can be manipulated by replacing equal parts. 15 / 41
46 Normal forms Two ways to think about graphical calculus: diagram represents morphism: merely shorthand to write down e.g. linear map; diagram is entity in its own right: can be manipulated by replacing equal parts. First viewpoint: ok if different diagrams represent same morphism. Second viewpoint: combinatorial/graph theoretic flavour. 15 / 41
47 Normal forms Two ways to think about graphical calculus: diagram represents morphism: merely shorthand to write down e.g. linear map; diagram is entity in its own right: can be manipulated by replacing equal parts. First viewpoint: ok if different diagrams represent same morphism. Second viewpoint: combinatorial/graph theoretic flavour. A normal form theorem connects the two: proving that all diagrams representing fixed morphism can be rewritten into canonical diagram (like coherence theorem) 15 / 41
48 Normal forms Two ways to think about graphical calculus: diagram represents morphism: merely shorthand to write down e.g. linear map; diagram is entity in its own right: can be manipulated by replacing equal parts. First viewpoint: ok if different diagrams represent same morphism. Second viewpoint: combinatorial/graph theoretic flavour. A normal form theorem connects the two: proving that all diagrams representing fixed morphism can be rewritten into canonical diagram (like coherence theorem) Unique way to copy ( ), discard ( ), fuse ( ), create ( ) data! 15 / 41
49 Spider theorem Let (A,,,, ) be a special Frobenius structure. Any connected morphism A m A n built out of finitely many pieces,,,, and id, using and, equals: n m 16 / 41
50 Spider theorem Let (A,,,, ) be a special Frobenius structure. Any connected morphism A m A n built out of finitely many pieces,,,, and id, using and, equals: n m Proof. Induction on the number of dots. 16 / 41
51 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. 17 / 41
52 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. Induction step. Assume all diagrams with at most n dots can be brought in normal form, and consider a diagram with n + 1 dots. 17 / 41
53 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. Induction step. Assume all diagrams with at most n dots can be brought in normal form, and consider a diagram with n + 1 dots. Use naturality to write diagram in form with topmost dot. 17 / 41
54 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. Induction step. Assume all diagrams with at most n dots can be brought in normal form, and consider a diagram with n + 1 dots. Use naturality to write diagram in form with topmost dot. Topmost dot is : use counitality to eliminatt. 17 / 41
55 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. Induction step. Assume all diagrams with at most n dots can be brought in normal form, and consider a diagram with n + 1 dots. Use naturality to write diagram in form with topmost dot. Topmost dot is : use counitality to eliminatt. Topmost dot is : use coassociativity to reach normal form. 17 / 41
56 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. Induction step. Assume all diagrams with at most n dots can be brought in normal form, and consider a diagram with n + 1 dots. Use naturality to write diagram in form with topmost dot. Topmost dot is : use counitality to eliminatt. Topmost dot is : use coassociativity to reach normal form. Topmost dot is : impossible by connectedness. 17 / 41
57 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. Induction step. Assume all diagrams with at most n dots can be brought in normal form, and consider a diagram with n + 1 dots. Use naturality to write diagram in form with topmost dot. Topmost dot is : use counitality to eliminatt. Topmost dot is : use coassociativity to reach normal form. Topmost dot is : impossible by connectedness. Topmost dot is : the most interesting case. 17 / 41
58 Spider theorem Proof. (continued.) Base case. Trivial, as the diagram must be one of,,,. Induction step. Assume all diagrams with at most n dots can be brought in normal form, and consider a diagram with n + 1 dots. Use naturality to write diagram in form with topmost dot. Topmost dot is : use counitality to eliminatt. Topmost dot is : use coassociativity to reach normal form. Topmost dot is : impossible by connectedness. Topmost dot is : the most interesting case. Is the diagram underneath the connected? If so, use coassociativity and speciality. 17 / 41
59 Spider theorem Proof. (continued.) Supposnstead the rest of the diagram is disconnected: 18 / 41
60 More spider theorems In a monoidal category, let (A,,,, ) be a Frobenius structure. Any connected morphism A m A n built out of finitely many pieces,,,, and id, using and, equals ( ). ( ) 19 / 41
61 More spider theorems In a monoidal category, let (A,,,, ) be a Frobenius structure. Any connected morphism A m A n built out of finitely many pieces,,,, and id, using and, equals ( ). ( ) In a symmetric monoidal category, let (A,,,, ) be a commutative Frobenius structure. Any connected morphism A m A n built out of finitely many pieces,,,, id,, using and, equals ( ). 19 / 41
62 No braided spider theorem In a braided non-symmetric monoidal category, thers no normal form for commutative Frobenius algebras. 20 / 41
63 No braided spider theorem In a braided non-symmetric monoidal category, thers no normal form for commutative Frobenius algebras. Proof. Regard the following diagram as a piece of string on which an overhand knot is tied: 20 / 41
64 No braided spider theorem In a braided non-symmetric monoidal category, thers no normal form for commutative Frobenius algebras. Proof. Regard the following diagram as a piece of string on which an overhand knot is tied: The Frobenius algebra axioms induce homotopy equivalences ( deformations ) of the corresponding graph. Such moves cannot untie the knot. 20 / 41
65 Involutive monoids If (A, m, u) is monoid, so is (A, m, u ). 21 / 41
66 Involutive monoids If (A, m, u) is monoid, so is (A, m, u ). An involution for a monoid (A,, ) is a monoid homomorphism A i A satisfying i i id A. A A i i A A 21 / 41
67 Involutive monoids If (A, m, u) is monoid, so is (A, m, u ). An involution for a monoid (A,, ) is a monoid homomorphism A i A satisfying i i id A. A A B B i i i B f f i A A A A A A morphism of involutive monoids is monoid homomorphism A f satisfying i B f f i A. B 21 / 41
68 Examplnvolutive monoids Matrix algebra. M n is an involutive monoid in FHilb. Opposite monoid M n: multiplication ab in M n is ba in M n. Canonical involution M n M n given by f f. 22 / 41
69 Examplnvolutive monoids Matrix algebra. M n is an involutive monoid in FHilb. Opposite monoid M n: multiplication ab in M n is ba in M n. Canonical involution M n M n given by f f. Pair of pants. A A involutivn a dagger pivotal category. Identity map as involution, because of conventions: ( ) 22 / 41
70 Examplnvolutive monoids Matrix algebra. M n is an involutive monoid in FHilb. Opposite monoid M n: multiplication ab in M n is ba in M n. Canonical involution M n M n given by f f. Pair of pants. A A involutivn a dagger pivotal category. Identity map as involution, because of conventions: ( ) Groupoids. G in Rel is involutive. Opposite monoid: induced by opposite groupoid G op Canonical involution G G given by g g / 41
71 Frobenius law from way of the dagger Monoid (A,, ) is dagger Frobenius if and only if i is involution: i 23 / 41
72 Frobenius law from way of the dagger Monoid (A,, ) is dagger Frobenius if and only if i is involution: i Proof. Assume dagger Frobenius. 23 / 41
73 Frobenius law from way of the dagger Monoid (A,, ) is dagger Frobenius if and only if i is involution: i Proof. Assume dagger Frobenius. i preserves multiplication: i i i 23 / 41
74 Frobenius law from way of the dagger Monoid (A,, ) is dagger Frobenius if and only if i is involution: i Proof. Assume dagger Frobenius. i preserves multiplication: i i i i preserves units: easy. 23 / 41
75 Frobenius law from way of the dagger Monoid (A,, ) is dagger Frobenius if and only if i is involution: i Proof. Assume dagger Frobenius. i preserves multiplication: i i i i preserves units: easy. i is involution: i i 23 / 41
76 Frobenius law from way of the dagger Proof. (continued.) Conversely, suppos i id. Then: and by applying, 24 / 41
77 Frobenius law from way of the dagger Proof. (continued.) Conversely, suppos i id. Then: and by applying, So we have a Frobenius structure, defined by a nondegenerate form. Is it a dagger Frobenius structure? 24 / 41
78 Frobenius law from way of the dagger Proof. (continued.) Conversely, suppos i id. Then: and by applying, So we have a Frobenius structure, defined by a nondegenerate form. Is it a dagger Frobenius structure? The condition that i preserves multiplication gives: ( ) So the form definition gives rise to the correct comultiplication. 24 / 41
79 Classification in FHilb Theorem: special dagger Frobenius structures in FHilb are of the form M n1 M nk. 25 / 41
80 Classification in FHilb Theorem: special dagger Frobenius structures in FHilb are of the form M n1 M nk. Proof: Cayley: dagger Frobenius structure on H embeds into H H H H isomorphic to M dim(h) so H involutive subalgebra of M dim(h) : C*-algebra Artin-Wedderburn: must be of form M n1 M nk 25 / 41
81 Classification in FHilb Theorem: special dagger Frobenius structures in FHilb are of the form M n1 M nk. Proof: Cayley: dagger Frobenius structure on H embeds into H H H H isomorphic to M dim(h) so H involutive subalgebra of M dim(h) : C*-algebra Artin-Wedderburn: must be of form M n1 M nk Corollary: classical structurn FHilb copy orthonormal bases Proof: must be of form C C. 25 / 41
82 Orthogonal bases Frobenius structure that copies basis is dagger Frobenius if and only if basis is orthogonal. 26 / 41
83 Orthogonal bases Frobenius structure that copies basis is dagger Frobenius if and only if basis is orthogonal. Proof. For nonzero copyable states: x x y x y x y x y y x x x x x x x x x x 26 / 41
84 Orthogonal bases Frobenius structure that copies basis is dagger Frobenius if and only if basis is orthogonal. Proof. For nonzero copyable states: x x y x y x y x y y x x x x x x x x x x If x y 0, then this is satisfied. 26 / 41
85 Orthogonal bases Frobenius structure that copies basis is dagger Frobenius if and only if basis is orthogonal. Proof. For nonzero copyable states: x x y x y x y x y y x x x x x x x x x x If x y 0, then this is satisfied. If x y 0, this implies x x x y. Similarly y x y y. 26 / 41
86 Orthogonal bases Frobenius structure that copies basis is dagger Frobenius if and only if basis is orthogonal. Proof. For nonzero copyable states: x x y x y x y x y y x x x x x x x x x x If x y 0, then this is satisfied. If x y 0, this implies x x x y. Similarly y x y y. Hence x y x y x x x y y x + y y 0, so x y. 26 / 41
87 Orthogonal bases and morphisms In FHilb, morphism between two commutative dagger Frobenius structures acts as function on copyable states if and only if it is comonoid homomorphism. 27 / 41
88 Orthogonal bases and morphisms In FHilb, morphism between two commutative dagger Frobenius structures acts as function on copyable states if and only if it is comonoid homomorphism. Proof. Suffices to see about basis of copyable states { }. f f f f f Hence f( ) copyable. 27 / 41
89 Classification in Rel Theorem: Special dagger Frobenius structures in Rel correspond exactly to groupoids. 28 / 41
90 Classification in Rel Theorem: Special dagger Frobenius structures in Rel correspond exactly to groupoids. Proof. Write A A M A for multiplication, U A for unit. 28 / 41
91 Classification in Rel Theorem: Special dagger Frobenius structures in Rel correspond exactly to groupoids. Proof. Write A A M A for multiplication, U A for unit. M is single-valued: by speciality a(m M )b iff a b: b b c d a a So: if (c, d)ma and (c, d)mb, must have a b. May simply write ab for unique c with (a, b)mc. Remember: ab not always defined! 28 / 41
92 Classification in Rel Proof. (continued) Associativity: (ab)c a(bc) ab bc a b c a b c So ab and (ab)c defined exactly when bc and a(bc) are defined, and then (ab)c a(bc). 29 / 41
93 Classification in Rel Proof. (continued) Unitality: for units x, y U b b b x y a a a So: a, b allow x U with xa b iff a b. And: a, b allow y U with ay b iff a b. If z U then xz x for some x U. But then x z! Units idempotent; multiplication of different ones undefined. If xa a x a, then a xa x(x a) (xx )a, so x x. So every element has unique left/right identity. 30 / 41
94 Classification in Rel Proof. (continued) Category: U set of objects, A set of morphisms. If fg defined and gh defined, want (fg)h f(gh) defined too: fg h fg h g f(gh) (fg)h f gh f gh If fg and gh defined then LHS defined, so RHS defined too. 31 / 41
95 Classification in Rel Proof. (continued) Inverses: for f A with left unit x and right unit y: x f x f g f f y f y 32 / 41
96 Phases Let (A,, ) be Frobenius structurn a monoidal dagger category. State I a A is called phase when: a a a a 33 / 41
97 Phases Let (A,, ) be Frobenius structurn a monoidal dagger category. State I a A is called phase when: a a a a Its (right) phase shift is the following morphism A A: a a 33 / 41
98 Example phases For classical structurn FHilb copying basis { }, vector a a 1 e 1 + a n e n is phasff each a i on unit circle: a i / 41
99 Example phases For classical structurn FHilb copying basis { }, vector a a 1 e 1 + a n e n is phasff each a i on unit circle: a i 2 1. The unit of a Frobenius structurs always a phase. 34 / 41
100 Example phases For classical structurn FHilb copying basis { }, vector a a 1 e 1 + a n e n is phasff each a i on unit circle: a i 2 1. The unit of a Frobenius structurs always a phase. In a compact dagger category, phases for pair of pants (A A,, ) correspond to unitary morphisms. Proof. 34 / 41
101 Example phases For classical structurn FHilb copying basis { }, vector a a 1 e 1 + a n e n is phasff each a i on unit circle: a i 2 1. The unit of a Frobenius structurs always a phase. In a compact dagger category, phases for pair of pants (A A,, ) correspond to unitary morphisms. Proof. The name of an morphism A f A is a phase when: f f f f But this means f f id A ; similarly f f id A. 34 / 41
102 Example phases Phases of Frobenius structure M n in FHilb form set U(n) of n-by-n unitary matrices. Hence phases of M k1 M kn range over U(k 1 ) U(k n ). 35 / 41
103 Example phases Phases of Frobenius structure M n in FHilb form set U(n) of n-by-n unitary matrices. Hence phases of M k1 M kn range over U(k 1 ) U(k n ). Classical structure C n copying basis {e 1,..., e n }. Phases are elements of U(1) U(1); phase shift C n C n is accompanying unitary matrix. 35 / 41
104 Example phases Phases of Frobenius structure M n in FHilb form set U(n) of n-by-n unitary matrices. Hence phases of M k1 M kn range over U(k 1 ) U(k n ). Classical structure C n copying basis {e 1,..., e n }. Phases are elements of U(1) U(1); phase shift C n C n is accompanying unitary matrix. The phases of a Frobenius structurn Rel induced by a group G are elements of that group G itself. 35 / 41
105 Example phases Phases of Frobenius structure M n in FHilb form set U(n) of n-by-n unitary matrices. Hence phases of M k1 M kn range over U(k 1 ) U(k n ). Classical structure C n copying basis {e 1,..., e n }. Phases are elements of U(1) U(1); phase shift C n C n is accompanying unitary matrix. The phases of a Frobenius structurn Rel induced by a group G are elements of that group G itself. Proof. For a subset a G, equation defining phases reads {g 1 h g, h a} {1 G } {hg 1 g, h a}. So if g G, then a {g} is a phase. But if a contains distinct elements g h of G, cannot be phase. Similarly, a not phase. Hence a phase precisely when singleton {g}. 35 / 41
106 Phase group In a monoidal dagger category, the phases for a dagger Frobenius structure form a group, with unit and: a + b a b 36 / 41
107 Phase group In a monoidal dagger category, the phases for a dagger Frobenius structure form a group, with unit and: a + b a b Proof. This is again a well-defined phase: a + b a b a b b a + b a b a b b The flipped equation follows similarly. Associativity is clear, hence phases form a monoid. 36 / 41
108 Phase group Proof. (continued) Left-inverse of phase a is: a a 37 / 41
109 Phase group Proof. (continued) Left-inverse of phase a is: a a Left-inverse of a is a: ( a) + a a a a a 37 / 41
110 Phase group Proof. (continued) Left-inverse of phase a is: a a Left-inverse of a is a: ( a) + a a a a a Similarly thers right-inverse. But in monoids, left and right inverses are equal: l l(xr) (lx)r r. 37 / 41
111 Example phase groups In FHilb, the phase group for the pair of pants Frobenius structurs the unitary group. 38 / 41
112 Example phase groups In FHilb, the phase group for the pair of pants Frobenius structurs the unitary group. Phase addition in the Frobenius structure M k1 M kn in FHilb is entrywise multiplication in U(k 1 ) U(k n ). In particular, phase addition in a classical structurn FHilb is multiplication of diagonal matrices. 38 / 41
113 Example phase groups In FHilb, the phase group for the pair of pants Frobenius structurs the unitary group. Phase addition in the Frobenius structure M k1 M kn in FHilb is entrywise multiplication in U(k 1 ) U(k n ). In particular, phase addition in a classical structurn FHilb is multiplication of diagonal matrices. In Rel, the phase group induced by a group G is the group itself. 38 / 41
114 Phased spider theorem Let (A,, ) be classical structurn braided monoidal dagger category. Any connected morphism A m A n built of finitely many,, id, σ and phases using,, and, equals n {}}{ a }{{} m where a ranges over all the phases used in the diagram. 39 / 41
115 Phased spider theorem Let (A,, ) be classical structurn braided monoidal dagger category. Any connected morphism A m A n built of finitely many,, id, σ and phases using,, and, equals n {}}{ a }{{} m where a ranges over all the phases used in the diagram. Proof. Use braidings to have all phases dangle at the bottom. Apply Spider Theorem. Use phase addition to reduce to single phase a on bottom right. Apply Spider Theorem again. 39 / 41
116 State transfer State transfer protocol: transfer state of Hilbert space H from one system to another, with success probability 1/ dim(h) 2. May be lax in drawing, e.g. projection H H H H: The procedure looks like this: 1 n 1 n measure the first qubit measure both qubits together prepare the second qubit 1 n 1 n Extra challenge: apply phase gate while transferring state 1 n φ φ condition on first qubit measurement projection prepare second qubit 40 / 41
117 Summary Frobenius structures: interacting co/monoid, self-duality Normal forms: spider theorems Frobenius law: justified by coherence Classification: matrix algebras, bases, groupoids Phases: unitary operators, state transfer Next week: interaction between two Frobenius structures 41 / 41
Categorical quantum mechanics
Categorical quantum mechanics Chris Heunen 1 / 76 Categorical Quantum Mechanics? Study of compositional nature of (physical) systems Primitive notion: forming compound systems 2 / 76 Categorical Quantum
More informationEndomorphism Semialgebras in Categorical Quantum Mechanics
Endomorphism Semialgebras in Categorical Quantum Mechanics Kevin Dunne University of Strathclyde November 2016 Symmetric Monoidal Categories Definition A strict symmetric monoidal category (A,, I ) consists
More informationCategories and Quantum Informatics: Hilbert spaces
Categories and Quantum Informatics: Hilbert spaces Chris Heunen Spring 2018 We introduce our main example category Hilb by recalling in some detail the mathematical formalism that underlies quantum theory:
More informationMix Unitary Categories
1/31 Mix Unitary Categories Robin Cockett, Cole Comfort, and Priyaa Srinivasan CT2018, Ponta Delgada, Azores Dagger compact closed categories Dagger compact closed categories ( -KCC) provide a categorical
More information2-DIMENSIONAL TOPOLOGICAL QUANTUM FIELD THEORIES AND FROBENIUS ALGEBRAS. Contents 1. The main theorem 1
2-DIMENSIONL TOPOLOGICL QUNTUM FIELD THEORIES ND FROBENIUS LGEBRS CROLINE TERRY bstract. Category theory provides a more abstract and thus more general setting for considering the structure of mathematical
More informationFourier transforms from strongly complementary observables
Fourier transforms from strongly complementary observables Stefano Gogioso William Zeng Quantum Group, Department of Computer Science University of Oxford, UK stefano.gogioso@cs.ox.ac.uk william.zeng@cs.ox.ac.uk
More informationInfinite-dimensional Categorical Quantum Mechanics
Infinite-dimensional Categorical Quantum Mechanics A talk for CLAP Scotland Stefano Gogioso and Fabrizio Genovese Quantum Group, University of Oxford 5 Apr 2017 University of Strathclyde, Glasgow S Gogioso,
More informationTHE QUANTUM DOUBLE AS A HOPF ALGEBRA
THE QUANTUM DOUBLE AS A HOPF ALGEBRA In this text we discuss the generalized quantum double construction. treatment of the results described without proofs in [2, Chpt. 3, 3]. We give several exercises
More informationMONADS ON DAGGER CATEGORIES
MONDS ON DGGER CTEGORIES CHRIS HEUNEN ND MRTTI KRVONEN bstract. The theory of monads on categories equipped with a dagger (a contravariant identity-on-objects involutive endofunctor) works best when everything
More informationMONADS ON DAGGER CATEGORIES
MONDS ON DGGER CTEGORIES CHRIS HEUNEN ND MRTTI KRVONEN bstract. The theory of monads on categories equipped with a dagger (a contravariant identity-on-objects involutive endofunctor) works best when all
More informationCategorical relativistic quantum theory. Chris Heunen Pau Enrique Moliner Sean Tull
Categorical relativistic quantum theory Chris Heunen Pau Enrique Moliner Sean Tull 1 / 15 Idea Hilbert modules: naive quantum field theory Idempotent subunits: base space in any category Support: where
More informationCategorical Models for Quantum Computing
Categorical odels for Quantum Computing Linde Wester Worcester College University of Oxford thesis submitted for the degree of Sc in athematics and the Foundations of Computer Science September 2013 cknowledgements
More informationREVERSIBLE MONADIC COMPUTING
REVERSILE MONDIC COMPUTING CHRIS HEUNEN ND MRTTI KRVONEN bstract. We extend categorical semantics of monadic programming to reversible computing, by considering monoidal closed dagger categories: the dagger
More informationReversible Monadic Computing
MFPS 2015 Reversible Monadic Computing Chris Heunen 1,2 Department of Computer Science University of Oxford United Kingdom Martti Karvonen 3 Department of Mathematics and Systems nalysis alto University
More informationCategories and functors
Lecture 1 Categories and functors Definition 1.1 A category A consists of a collection ob(a) (whose elements are called the objects of A) for each A, B ob(a), a collection A(A, B) (whose elements are called
More informationNotation. For any Lie group G, we set G 0 to be the connected component of the identity.
Notation. For any Lie group G, we set G 0 to be the connected component of the identity. Problem 1 Prove that GL(n, R) is homotopic to O(n, R). (Hint: Gram-Schmidt Orthogonalization.) Here is a sequence
More informationA Graph Theoretic Perspective on CPM(Rel)
A Graph Theoretic Perspective on CPM(Rel) Daniel Marsden Mixed states are of interest in quantum mechanics for modelling partial information. More recently categorical approaches to linguistics have also
More information1 Categories, Functors, and Natural Transformations. Discrete categories. A category is discrete when every arrow is an identity.
MacLane: Categories or Working Mathematician 1 Categories, Functors, and Natural Transormations 1.1 Axioms or Categories 1.2 Categories Discrete categories. A category is discrete when every arrow is an
More informationREPRESENTATIONS OF FINITE GROUPS OF LIE TYPE: EXERCISES. Notation. 1. GL n
REPRESENTATIONS OF FINITE GROUPS OF LIE TYPE: EXERCISES ZHIWEI YUN Fix a prime number p and a power q of p. k = F q ; k d = F q d. ν n means ν is a partition of n. Notation Conjugacy classes 1. GL n 1.1.
More informationQuantum groupoids and logical dualities
Quantum groupoids and logical dualities (work in progress) Paul-André Melliès CNS, Université Paris Denis Diderot Categories, ogic and Foundations of Physics ondon 14 May 2008 1 Proof-knots Aim: formulate
More informationAbstract structure of unitary oracles for quantum algorithms
Abstract structure o unitary oracles or quantum algorithms William Zeng 1 Jamie Vicary 2 1 Department o Computer Science University o Oxord 2 Centre or Quantum Technologies, University o Singapore and
More informationQuantum Groups and Link Invariants
Quantum Groups and Link Invariants Jenny August April 22, 2016 1 Introduction These notes are part of a seminar on topological field theories at the University of Edinburgh. In particular, this lecture
More information1 Recall. Algebraic Groups Seminar Andrei Frimu Talk 4: Cartier Duality
1 ecall Assume we have a locally small category C which admits finite products and has a final object, i.e. an object so that for every Z Ob(C), there exists a unique morphism Z. Note that two morphisms
More informationTopological aspects of restriction categories
Calgary 2006, Topological aspects of restriction categories, June 1, 2006 p. 1/22 Topological aspects of restriction categories Robin Cockett robin@cpsc.ucalgary.ca University of Calgary Calgary 2006,
More informationCATEGORY THEORY. Cats have been around for 70 years. Eilenberg + Mac Lane =. Cats are about building bridges between different parts of maths.
CATEGORY THEORY PROFESSOR PETER JOHNSTONE Cats have been around for 70 years. Eilenberg + Mac Lane =. Cats are about building bridges between different parts of maths. Definition 1.1. A category C consists
More informationThe Structure of Fusion Categories via Topological Quantum Field Theories
The Structure of Fusion Categories via Topological Quantum Field Theories Chris Schommer-Pries Department of Mathematics, MIT April 27 th, 2011 Joint with Christopher Douglas and Noah Snyder Chris Schommer-Pries
More informationKathryn Hess. Conference on Algebraic Topology, Group Theory and Representation Theory Isle of Skye 9 June 2009
Institute of Geometry, lgebra and Topology Ecole Polytechnique Fédérale de Lausanne Conference on lgebraic Topology, Group Theory and Representation Theory Isle of Skye 9 June 2009 Outline 1 2 3 4 of rings:
More informationUnbounded operators in the context of C -algebras
Unbounded operators in the context of C -algebras Department of Mathematical Methods in Physics Faculty of Physics, Warsaw University Bȩdlewo, 23.07.2009 Affiliation relation η Murray, von Neumann: W -algebra
More information1 Categorical Background
1 Categorical Background 1.1 Categories and Functors Definition 1.1.1 A category C is given by a class of objects, often denoted by ob C, and for any two objects A, B of C a proper set of morphisms C(A,
More information0.2 Vector spaces. J.A.Beachy 1
J.A.Beachy 1 0.2 Vector spaces I m going to begin this section at a rather basic level, giving the definitions of a field and of a vector space in much that same detail as you would have met them in a
More informationDiagrammatic Methods for the Specification and Verification of Quantum Algorithms
Diagrammatic Methods or the Speciication and Veriication o Quantum lgorithms William Zeng Quantum Group Department o Computer Science University o Oxord Quantum Programming and Circuits Workshop IQC, University
More informationvon Neumann algebras, II 1 factors, and their subfactors V.S. Sunder (IMSc, Chennai)
von Neumann algebras, II 1 factors, and their subfactors V.S. Sunder (IMSc, Chennai) Lecture 3 at IIT Mumbai, April 24th, 2007 Finite-dimensional C -algebras: Recall: Definition: A linear functional tr
More informationLecture 3: Hilbert spaces, tensor products
CS903: Quantum computation and Information theory (Special Topics In TCS) Lecture 3: Hilbert spaces, tensor products This lecture will formalize many of the notions introduced informally in the second
More informationWhat is a quantum symmetry?
What is a quantum symmetry? Ulrich Krähmer & Angela Tabiri U Glasgow TU Dresden CLAP 30/11/2016 Uli (U Glasgow) What is a quantum symmetry? CLAP 30/11/2016 1 / 20 Road map Classical maths: symmetries =
More informationElliott s program and descriptive set theory I
Elliott s program and descriptive set theory I Ilijas Farah LC 2012, Manchester, July 12 a, a, a, a, the, the, the, the. I shall need this exercise later, someone please solve it Exercise If A = limna
More informationAn introduction to calculus of functors
An introduction to calculus of functors Ismar Volić Wellesley College International University of Sarajevo May 28, 2012 Plan of talk Main point: One can use calculus of functors to answer questions about
More informationIntroduction to Kleene Algebras
Introduction to Kleene Algebras Riccardo Pucella Basic Notions Seminar December 1, 2005 Introduction to Kleene Algebras p.1 Idempotent Semirings An idempotent semiring is a structure S = (S, +,, 1, 0)
More informationCONSTRUCTING FROBENIUS ALGEBRAS
CONSTRUCTING FROBENIUS LGEBRS DYLN G.L. LLEGRETTI bstract. We discuss the relationship between algebras, coalgebras, and Frobenius algebras. We describe a method of constructing Frobenius algebras, given
More informationConstruction of Physical Models from Category Theory. Master Thesis in Theoretical Physics. Marko Marjanovic
Construction of Physical Models from Category Theory Master Thesis in Theoretical Physics Marko Marjanovic Department of Physics University of Gothenburg Gothenburg, Sweden 2017 Construction of Physical
More informationUniversal Algebra and Diagrammatic Reasoning
Universal Algebra and Diagrammatic Reasoning John Baez Geometry of Computation 2006 January 30 - Feburary 3 = figures by Aaron D. Lauda available online at http://math.ucr.edu/home/baez/universal/ 1 Universal
More informationCategory Theory. Categories. Definition.
Category Theory Category theory is a general mathematical theory of structures, systems of structures and relationships between systems of structures. It provides a unifying and economic mathematical modeling
More informationNOTES ON ATIYAH S TQFT S
NOTES ON ATIYAH S TQFT S J.P. MAY As an example of categorification, I presented Atiyah s axioms [1] for a topological quantum field theory (TQFT) to undergraduates in the University of Chicago s summer
More informationModèles des langages de programmation Domaines, catégories, jeux. Programme de cette seconde séance:
Modèles des langages de programmation Domaines, catégories, jeux Programme de cette seconde séance: Modèle ensembliste du lambda-calcul ; Catégories cartésiennes fermées 1 Synopsis 1 the simply-typed λ-calculus,
More informationNON-SYMMETRIC -AUTONOMOUS CATEGORIES
NON-SYMMETRIC -AUTONOMOUS CATEGORIES MICHAEL BARR 1. Introduction In [Barr, 1979] (hereafter known as SCAT) the theory of -autonomous categories is outlined. Basically such a category is a symmetric monoidal
More informationFUNCTORS AND ADJUNCTIONS. 1. Functors
FUNCTORS AND ADJUNCTIONS Abstract. Graphs, quivers, natural transformations, adjunctions, Galois connections, Galois theory. 1.1. Graph maps. 1. Functors 1.1.1. Quivers. Quivers generalize directed graphs,
More informationFormal Homotopy Quantum Field Theories and 2-groups.
Formal Homotopy Quantum Field Theories and 2-groups. ex-university of Wales, Bangor; ex-univertiy of Ottawa; ex-nui Galway, still PPS Paris, then...? All have helped! June 21, 2008 1 Crossed Modules, etc
More informationSerre A -functors. Oleksandr Manzyuk. joint work with Volodymyr Lyubashenko. math.ct/ Notation. 1. Preliminaries on A -categories
Serre A -functors Oleksandr Manzyuk joint work with Volodymyr Lyubashenko math.ct/0701165 0. Notation 1. Preliminaries on A -categories 2. Serre functors 3. Serre A -functors 0. Notation k denotes a (ground)
More informationOperads. Spencer Liang. March 10, 2015
Operads Spencer Liang March 10, 2015 1 Introduction The notion of an operad was created in order to have a well-defined mathematical object which encodes the idea of an abstract family of composable n-ary
More informationarxiv: v1 [math.oa] 20 Feb 2018
C*-ALGEBRAS FOR PARTIAL PRODUCT SYSTEMS OVER N RALF MEYER AND DEVARSHI MUKHERJEE arxiv:1802.07377v1 [math.oa] 20 Feb 2018 Abstract. We define partial product systems over N. They generalise product systems
More informationCoarse geometry and quantum groups
Coarse geometry and quantum groups University of Glasgow christian.voigt@glasgow.ac.uk http://www.maths.gla.ac.uk/~cvoigt/ Sheffield March 27, 2013 Noncommutative discrete spaces Noncommutative discrete
More informationModular Categories and Applications I
I Modular Categories and Applications I Texas A&M University U. South Alabama, November 2009 Outline I 1 Topological Quantum Computation 2 Fusion Categories Ribbon and Modular Categories Fusion Rules and
More informationThus we get. ρj. Nρj i = δ D(i),j.
1.51. The distinguished invertible object. Let C be a finite tensor category with classes of simple objects labeled by a set I. Since duals to projective objects are projective, we can define a map D :
More informationCategorical quantum channels
Attacking the quantum version of with category theory Ian T. Durham Department of Physics Saint Anselm College 19 March 2010 Acknowledgements Some of this work has been the result of some preliminary collaboration
More information30 Surfaces and nondegenerate symmetric bilinear forms
80 CHAPTER 3. COHOMOLOGY AND DUALITY This calculation is useful! Corollary 29.4. Let p, q > 0. Any map S p+q S p S q induces the zero map in H p+q ( ). Proof. Let f : S p+q S p S q be such a map. It induces
More informationA NOTE ON FREE QUANTUM GROUPS
A NOTE ON FREE QUANTUM GROUPS TEODOR BANICA Abstract. We study the free complexification operation for compact quantum groups, G G c. We prove that, with suitable definitions, this induces a one-to-one
More informationActions of Compact Quantum Groups I
Actions of Compact Quantum Groups I Definition Kenny De Commer (VUB, Brussels, Belgium) Course material Material that will be treated: Actions and coactions of compact quantum groups. Actions on C -algebras
More informationSome Nearly Quantum Theories (extended abstract)
Some Nearly Quantum Theories (extended abstract) Howard Barnum University of New Mexico Albuquerque, USA hnbarnum@aol.com Matthew A. Graydon Perimeter Institute for Theoretical Physics Waterloo, Canada
More informationBoolean Algebras, Boolean Rings and Stone s Representation Theorem
Boolean Algebras, Boolean Rings and Stone s Representation Theorem Hongtaek Jung December 27, 2017 Abstract This is a part of a supplementary note for a Logic and Set Theory course. The main goal is to
More informationMV-algebras and fuzzy topologies: Stone duality extended
MV-algebras and fuzzy topologies: Stone duality extended Dipartimento di Matematica Università di Salerno, Italy Algebra and Coalgebra meet Proof Theory Universität Bern April 27 29, 2011 Outline 1 MV-algebras
More informationPeter Hochs. Strings JC, 11 June, C -algebras and K-theory. Peter Hochs. Introduction. C -algebras. Group. C -algebras.
and of and Strings JC, 11 June, 2013 and of 1 2 3 4 5 of and of and Idea of 1 Study locally compact Hausdorff topological spaces through their algebras of continuous functions. The product on this algebra
More informationarxiv: v2 [math.kt] 12 Dec 2008
EQUIVARIANT REPRESENTABLE K-THEORY HEATH EMERSON AND RALF MEYER arxiv:0710.1410v2 [math.kt] 12 Dec 2008 Abstract. We interpret certain equivariant Kasparov groups as equivariant representable K-theory
More informationCHAPTER 0: A (VERY) BRIEF TOUR OF QUANTUM MECHANICS, COMPUTATION, AND CATEGORY THEORY.
CHPTER 0: (VERY) BRIEF TOUR OF QUNTUM MECHNICS, COMPUTTION, ND CTEGORY THEORY. This chapter is intended to be a brief treatment of the basic mechanics, framework, and concepts relevant to the study of
More informationSome Nearly Quantum Theories
Some Nearly Quantum Theories Howard Barnum, Matthew Graydon and Alex Wilce QPL XII, Oxford, July 2015 Outline I Euclidean Jordan algebras II Composites of EJAs III Categories of embedded EJAs I. Euclidean
More informationAlmost periodic functionals
Almost periodic functionals Matthew Daws Leeds Warsaw, July 2013 Matthew Daws (Leeds) Almost periodic functionals Warsaw, July 2013 1 / 22 Dual Banach algebras; personal history A Banach algebra A Banach
More informationBases as Coalgebras. Bart Jacobs
Bases as Coalgebras Bart Jacobs Institute for Computing and Information Sciences (icis), Radboud University Nijmegen, The Netherlands. Webaddress: www.cs.ru.nl/b.jacobs Abstract. The free algebra adjunction,
More informationGaussian automorphisms whose ergodic self-joinings are Gaussian
F U N D A M E N T A MATHEMATICAE 164 (2000) Gaussian automorphisms whose ergodic self-joinings are Gaussian by M. L e m a ńc z y k (Toruń), F. P a r r e a u (Paris) and J.-P. T h o u v e n o t (Paris)
More informationarxiv:math/ v1 [math.at] 5 Oct 1999
arxiv:math/990026v [math.at] 5 Oct 999 REPRESENTATIONS OF THE HOMOTOPY SURFACE CATEGORY OF A SIMPLY CONNECTED SPACE MARK BRIGHTWELL AND PAUL TURNER. Introduction At the heart of the axiomatic formulation
More informationA quantum double construction in Rel
Under consideration for publication in Math. Struct. in Comp. Science A quantum double construction in Rel M A S A H I T O H A S E G A W A Research Institute for Mathematical Sciences, Kyoto University,
More informationLECTURE 25-26: CARTAN S THEOREM OF MAXIMAL TORI. 1. Maximal Tori
LECTURE 25-26: CARTAN S THEOREM OF MAXIMAL TORI 1. Maximal Tori By a torus we mean a compact connected abelian Lie group, so a torus is a Lie group that is isomorphic to T n = R n /Z n. Definition 1.1.
More informationMonoidal Categories, Bialgebras, and Automata
Monoidal Categories, Bialgebras, and Automata James Worthington Mathematics Department Cornell University Binghamton University Geometry/Topology Seminar October 29, 2009 Background: Automata Finite automata
More informationIntroduction to Index Theory. Elmar Schrohe Institut für Analysis
Introduction to Index Theory Elmar Schrohe Institut für Analysis Basics Background In analysis and pde, you want to solve equations. In good cases: Linearize, end up with Au = f, where A L(E, F ) is a
More informationWhat s category theory, anyway? Dedicated to the memory of Dietmar Schumacher ( )
What s category theory, anyway? Dedicated to the memory of Dietmar Schumacher (1935-2014) Robert Paré November 7, 2014 Many subjects How many subjects are there in mathematics? Many subjects How many subjects
More informationSymmetries, Fields and Particles 2013 Solutions
Symmetries, Fields and Particles 013 Solutions Yichen Shi Easter 014 1. (a) Define the groups SU() and SO(3), and find their Lie algebras. Show that these Lie algebras, including their bracket structure,
More informationA Brief Introduction to Functional Analysis
A Brief Introduction to Functional Analysis Sungwook Lee Department of Mathematics University of Southern Mississippi sunglee@usm.edu July 5, 2007 Definition 1. An algebra A is a vector space over C with
More informationMTH 428/528. Introduction to Topology II. Elements of Algebraic Topology. Bernard Badzioch
MTH 428/528 Introduction to Topology II Elements of Algebraic Topology Bernard Badzioch 2016.12.12 Contents 1. Some Motivation.......................................................... 3 2. Categories
More informationA non-commutative notion of separate continuity
A non-commutative notion of separate continuity Matthew Daws Leeds November 2014 Matthew Daws (Leeds) Separate continuity November 2014 1 / 22 Locally compact spaces Let X be a locally compact (Hausdorff)
More informationMath Camp II. Basic Linear Algebra. Yiqing Xu. Aug 26, 2014 MIT
Math Camp II Basic Linear Algebra Yiqing Xu MIT Aug 26, 2014 1 Solving Systems of Linear Equations 2 Vectors and Vector Spaces 3 Matrices 4 Least Squares Systems of Linear Equations Definition A linear
More informationarxiv:math/ v2 [math.qa] 29 Jan 2001
DAMTP-98-117 arxiv:math/9904142v2 [math.qa] 29 Jan 2001 Cross Product Bialgebras Yuri Bespalov Part II Bernhard Drabant July 1998/March 1999 Abstract This is the central article of a series of three papers
More informationYale University Department of Mathematics Math 350 Introduction to Abstract Algebra Fall Midterm Exam Review Solutions
Yale University Department of Mathematics Math 350 Introduction to Abstract Algebra Fall 2015 Midterm Exam Review Solutions Practice exam questions: 1. Let V 1 R 2 be the subset of all vectors whose slope
More informationLecture 1: Crossed Products of C*-Algebras by Finite Groups. General motivation. A rough outline of all three lectures
Winter School on Operator Algebras Lecture 1: Crossed Products of C*-Algebras by Finite Groups RIMS, Kyoto University, Japan N Christopher Phillips 7 16 December 2011 University of Oregon Research Institute
More informationApproaches to bounding the exponent of matrix multiplication
Approaches to bounding the exponent of matrix multiplication Chris Umans Caltech Based on joint work with Noga Alon, Henry Cohn, Bobby Kleinberg, Amir Shpilka, Balazs Szegedy Simons Institute Sept. 7,
More informationDifferential Calculus
Differential Calculus Mariusz Wodzicki December 19, 2015 1 Vocabulary 1.1 Terminology 1.1.1 A ground ring of coefficients Let k be a fixed unital commutative ring. We shall be refering to it throughout
More informationAdequate and Ehresmann semigroups
Adequate and Ehresmann semigroups NSAC2013: June 8th, 2013, Novi Sad Victoria Gould University of York What is this talk about? Classes of semigroups with semilattices of idempotents inverse ample adequate
More informationInstitut für Mathematik, Universität Wien, Strudlhofgasse 4, A-1090 Wien, Austria.
Letters in Math. Phys. 28 (1993), 251 255 A QUANTUM GROUP LIKE STRUCTURE ON NON COMMUTATIVE 2 TORI Andreas Cap Peter W. Michor Hermann Schichl Institut für Mathematik, Universität Wien, Strudlhofgasse
More informationSheet 11. PD Dr. Ralf Holtkamp Prof. Dr. C. Schweigert Hopf algebras Winter term 2014/2015. Algebra and Number Theory Mathematics department
Algebra and Number Theory Mathematics department PD Dr. Ralf Holtkamp Prof. Dr. C. Schweigert Hopf algebras Winter term 014/015 Sheet 11 Problem 1. We consider the C-algebra H generated by C and X with
More informationAbstract Algebra II Groups ( )
Abstract Algebra II Groups ( ) Melchior Grützmann / melchiorgfreehostingcom/algebra October 15, 2012 Outline Group homomorphisms Free groups, free products, and presentations Free products ( ) Definition
More informationIntroduction to Restriction Categories
Introduction to Restriction Categories Robin Cockett Department of Computer Science University of Calgary Alberta, Canada robin@cpsc.ucalgary.ca Estonia, March 2010 Defining restriction categories Examples
More informationIn the beginning God created tensor... as a picture
In the beginning God created tensor... as a picture Bob Coecke coecke@comlab.ox.ac.uk EPSRC Advanced Research Fellow Oxford University Computing Laboratory se10.comlab.ox.ac.uk:8080/bobcoecke/home en.html
More informationClifford Algebras and Spin Groups
Clifford Algebras and Spin Groups Math G4344, Spring 2012 We ll now turn from the general theory to examine a specific class class of groups: the orthogonal groups. Recall that O(n, R) is the group of
More informationCategorical techniques for NC geometry and gravity
Categorical techniques for NC geometry and gravity Towards homotopical algebraic quantum field theory lexander Schenkel lexander Schenkel School of Mathematical Sciences, University of Nottingham School
More informationSPECTRAL THEORY EVAN JENKINS
SPECTRAL THEORY EVAN JENKINS Abstract. These are notes from two lectures given in MATH 27200, Basic Functional Analysis, at the University of Chicago in March 2010. The proof of the spectral theorem for
More informationDEPARTMENT OF MATHEMATIC EDUCATION MATHEMATIC AND NATURAL SCIENCE FACULTY
HANDOUT ABSTRACT ALGEBRA MUSTHOFA DEPARTMENT OF MATHEMATIC EDUCATION MATHEMATIC AND NATURAL SCIENCE FACULTY 2012 BINARY OPERATION We are all familiar with addition and multiplication of two numbers. Both
More informationA PRIMER ON SESQUILINEAR FORMS
A PRIMER ON SESQUILINEAR FORMS BRIAN OSSERMAN This is an alternative presentation of most of the material from 8., 8.2, 8.3, 8.4, 8.5 and 8.8 of Artin s book. Any terminology (such as sesquilinear form
More informationA Linear/Producer/Consumer model of Classical Linear Logic
A Linear/Producer/Consumer model of Classical Linear Logic Jennifer Paykin Steve Zdancewic February 14, 2014 Abstract This paper defines a new proof- and category-theoretic framework for classical linear
More informationExercises on chapter 1
Exercises on chapter 1 1. Let G be a group and H and K be subgroups. Let HK = {hk h H, k K}. (i) Prove that HK is a subgroup of G if and only if HK = KH. (ii) If either H or K is a normal subgroup of G
More informationREPRESENTATION THEORY WEEK 7
REPRESENTATION THEORY WEEK 7 1. Characters of L k and S n A character of an irreducible representation of L k is a polynomial function constant on every conjugacy class. Since the set of diagonalizable
More information1 Dirac Notation for Vector Spaces
Theoretical Physics Notes 2: Dirac Notation This installment of the notes covers Dirac notation, which proves to be very useful in many ways. For example, it gives a convenient way of expressing amplitudes
More informationA KOCHEN-SPECKER THEOREM FOR INTEGER MATRICES AND NONCOMMUTATIVE SPECTRUM FUNCTORS
A KOCHEN-SPECKER THEOREM FOR INTEGER MATRICES AND NONCOMMUTATIVE SPECTRUM FUNCTORS MICHAEL BEN-ZVI, ALEXANDER MA, AND MANUEL REYES, WITH APPENDIX BY ALEXANDRU CHIRVASITU Abstract. We investigate the possibility
More information1.1 Definition. A monoid is a set M together with a map. 1.3 Definition. A monoid is commutative if x y = y x for all x, y M.
1 Monoids and groups 1.1 Definition. A monoid is a set M together with a map M M M, (x, y) x y such that (i) (x y) z = x (y z) x, y, z M (associativity); (ii) e M such that x e = e x = x for all x M (e
More informationBiunitary constructions in quantum information
Biunitary constructions in quantum information David Reutter Jamie Vicary Department of Computer Science University of Oxford 14th International Conference on Quantum Physics and Logic Nijmegen, The Netherlands
More information