DOCSLIB.ORG

Compositionality in Categorical Quantum Computing

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
Compositionality in Categorical Quantum Computing Compositionality in Categorical Quantum Mechanics Ross Duncan Simon Perdrix Bob Coecke Kevin Dunne Niel de Beaudrap Compositionality x 3 • Plain old monoidal category theory: —— quantum computing in string diagrams • Rewriting and substitution: —— taking the syntax seriously • “Quantum theory” as a composite theory —— Lack’s composing PROPS An application: compiling for quantum architecture 1. Quantum theory as string diagrams How much quantum theory can be expressed as an internal language in some monoidal category? PAST / HEAVEN FUTURE / HELL F.D. Pure state QM • States : Hilbert spaces • Compound systems : Tensor product • Dynamics : Unitary maps • Non-degenerate measurements : O.N. Bases F.D. Pure state QM Ambient mathematical framework: †-symmetric monoidal categories • States : Hilbert spaces • Compound systems : Tensor product • Dynamics : Unitary maps • Non-degenerate measurements : O.N. Bases F.D. Pure state QM Ambient mathematical framework: †-symmetric monoidal categories • States : Hilbert spaces • Compound systems : Tensor product • Dynamics : Unitary maps • Non-degenerate measurements : O.N. Bases Choose some good generators and relations to capture this stuff Frobenius Algebras Theorem: in fdHilb orthonormal bases are in bijection with †-special commutative Frobenius algebras. ! !δ : A A Aµ: A A A ! ! ⌦ ⌦ ! ✏ : A I ⌘ : I A ! ! ! Via: ! δ :: a a a µ = δ† | ii!| ii⌦| ii ✏ :: a 1 ⌘ = ⌘† | ii! Coecke, Pavlovic, and Vicary, “A new description of orthogonal bases”, MSCS 23(3), 2013. arxiv:0810.0812 Frobenius Algebras Definition A -special commutativeFrobenius Frobenius Algebras algebra ( -SCFA) in ( , , I ) † Represent observables by †-special commutative† C ⌦ consists of: An objectFrobenius Aalgebras:, ! 2 C ! ! µ = , ⌘ = µ† = , ⌘† = satisfying... of directed equations (f2,f1) (f Õ ,fÕ ) commuting morphisms of T2 past those æ 1 2 f-1 f-2 of T1. The composite PROP T1; T2 has morphisms of the form n z m where f1 is an arrow of T1 and f2 of T2; its syntactic presentation is that of T1 + T2 with the additional equations of ⁄. Example 1.4. As a simple example we can view P as a PRO with a single generator c :2 2 quotiented by c2 = id and the usual hexagon diagrams. Let Frobenius Algebrasæ G be some any; we define G◊ to be the PRO with hom-sets G◊(n, n)= n G, and G◊(n, m)= if n = m. Composition is done component-wise in G.The ÿ ” r generators of G◊ are just the elements g :1 1 for each g G quotiented by æ œ the equations of G. We can define the composite P; G◊ via the distributive law: g1 g2 Definition ⁄ : = g2 g1 for each g andFrobeniusg in G. This yields the PROAlgebras – actually a -PROP – whose A -special commutative1 2 Frobenius algebra ( -SCFA)† in ( , , I ) morphisms n n are a permutation on n followed by an n-vector of elements of † Representæ observables by †-special commutative† C ⌦ G. It’s easy to see that this construction yields a functor P : Grp -PROP. Frobenius algebras: æ † consistsNotice of: An that objectPG is againA a groupoid,, and every morphism is unitary. ! 2 C Example 1.5.! A second cluster of examples, stolen shamelessly from [17], pro- vides the main! structures of interest of this paper. Let M denote the PROP of commutative monoids; it has two generators, µ :2 1 and ÷ :0: 1,whichwe µ = , ⌘æ = æ write graphically as and , subject to the equations: = µ† = , = = ⌘† = = (M) We can define the PROP of cocommutative comonoids as C = Mop. The gener- ators are ” :1 2 and ‘ :1 0; the equations are those of (M) but flipped æ æ satisfying...upside down. Bialgebras and Frobenius algebras combine a monoid and comonoid in different ways; both can be built using distributive laws between M and C. The PROP B of commutative bialgebras is constructed via a distributive law ⁄B : M; C C; M generated by the equations æ = = = = (B) where the dashed box represents the empty diagram. The PROP F of Frobenius algebras is also defined by distributive law, ⁄F : C; M M; C, given by the equations: æ = = = (F) = = = (F) Frobenius Algebrasæ C M M C ; ; , given by the equations: F F The PROP of Frobenius algebras is also defined by distributive law, : ⁄ where the dashed box represents the empty diagram. = = = = (B) æ M C C M B : ; ; generated by the equations Definition⁄ Frobenius Algebras B The PROP of commutative bialgebras is constructed via a distributive law M C fferent ways; both can be built using distributive laws between and . in di Represent observables by †-special commutative A -specialupside commutative down. Bialgebras and Frobenius Frobenius algebras algebra combine a monoid( -SCFA) and comonoid in ( , , I ) æ Frobeniusæ algebras: ators are :1 2 and :1 0; the equations are those of (M) but flipped ‘ † ”! † C ⌦ C M We can define the PROP of cocommutative comonoids as = . The gener- consists of: An object! A , op ! 2 C = = = (M) = µ = , ⌘ = write graphically as and , subject to the equations: æ æ commutative monoids; it has two generators, :2 1 and :0: 1,whichwe µ ÷ M vides the main structures of interest of this paper. Let denote the PROP of A second cluster of examples, stolen shamelessly from [17], pro- Example 1.5. µ† = , ⌘† = P Notice that is again a groupoid, and every morphism is unitary. G æ † P Grp PROP . It’s easy to see that this construction yields a functor : - . G æ morphisms are a permutation on followed by an -vector of elements of n n n n † 1 2 for each and in . This yields the PRO – actually a -PROP – whose g G satisfying... g : = ⁄ 2 1 g g 1 2 g g P ◊ the equations of . We can define the composite ; via the distributive law: G G æ œ ◊ generators of are just the elements :1 1 for each quotiented by G g g G r ÿ ” ◊ and ( )= if = . Composition is done component-wise in .The G n, m n m G n ◊ ◊ be some any; we define to be the PRO with hom-sets ( )= , G G G n, n G æ generator :2 2 quotiented by = id and the usual hexagon diagrams. Let c c 2 P Example 1.4. As a simple example we can view as a PRO with a single T T 1 2 + with the additional equations of . ⁄ T T 1 1 2 2 where is an arrow of and of ; its syntactic presentation is that of f f T T T 1 1 2 of . The composite PROP ; has morphisms of the form n z m - - 1 2 f f æ 1 2 T 2 1 2 Õ Õ of directed equations ( ) ( ) commuting morphisms of past those f ,f f ,f of directed equations (f2,f1) (f Õ ,fÕ ) commuting morphisms of T2 past those æ 1 2 f-1 f-2 of T1. The composite PROP T1; T2 has morphisms of the form n z m where f1 is an arrow of T1 and f2 of T2; its syntactic presentation is that of T1 + T2 with the additional equations of ⁄. Example 1.4. As a simple example we can view P as a PRO with a single generator c :2 2 quotiented by c2 = id and the usual hexagon diagrams. Let æ G be some any; we define G◊ to be the PRO with hom-sets G◊(n, n)= n G, and G◊(n, m)= if n = m. Composition is done component-wise in G.The ÿ ” r generators of G◊ are just the elements g :1 1 for each g G quotiented by æ œ the equations of G. We can define the composite P; G◊ via the distributive law: g1 g2 ⁄ : = g2 g1 for each g and g in G. This yields the PRO – actually a -PROP – whose 1 2 † morphisms n n are a permutation on n followed by an n-vector of elements of æ G. It’s easy to see that this construction yields a functor P : Grp -PROP. æ † Notice that PG is again a groupoid, and every morphism is unitary. Example 1.5. A second cluster of examples, stolen shamelessly from [17], pro- vides the main structures of interest of this paper. Let M denote the PROP of commutative monoids; it has two generators, µ :2 1 and ÷ :0: 1,whichwe æ æ write graphically as and , subject to the equations: = = = = (M) We can define the PROP of cocommutative comonoids as C = Mop. The gener- ators are ” :1 2 and ‘ :1 0; the equations are those of (M) but flipped æ æ upside down.Frobenius Bialgebras Algebras and Frobenius algebras combine a monoid and comonoid in different ways; both can be built using distributive laws between M and C. The PROP B of commutative bialgebras is constructed via a distributive law ⁄B : M; C C; M generated by the equations æ DefinitionFrobenius Algebras A -special commutative Frobenius algebra ( -SCFA) in ( , , I ) † Represent observables by †-special† commutativeC ⌦ = consists of: An object= A , = = (B) Frobenius algebras:2 C ! ! µ = , ⌘ = where the dashed! box represents the empty diagram. The PROP of Frobenius algebras is also defined by distributive law, ⁄ : F µ† = , ⌘† = F C; M M; C, given by the equations: æ satisfying... = = = (F) Call Z↵ the phases for this Frobenius algebra or, the -phases Call Z↵ the phases for this Frobenius algebra or, the -phases Observables and Phases Observables and Phases Phases , Abasis 0 1 A -SCFA Abasis 0 , 1 A -SCFA {| i | i } † { • Defn: a phase}{| isi unitary| i } map that commutes† with{ } the Frobenius algebra like this: Z↵ 0 = 0 Z↵ Z↵ 0 Z=↵ 0 Z Z | i | i = , = | i | i ↵ = , = ↵ Z 1 = 1 Z↵ Z ↵ Z↵ 1 = 1 Z↵ Z↵ ↵| i | i | i | i • Thm: the phases form an abelian group Example: Z-spin • The following define a Frobenius algebra on the qubit: 0 00 0 1 δ : ✏ : |1i 7! |11i |1i 7! 1 | i 7! | i | i 7! • Its group of phases is: 0 0 Z : ↵ |1i 7! e| i↵i 1 | i 7! | i Example: Z-spin 0 0 00 0 1 δ : ✏ : | |1i 7! |11i |1i 7! 1 | i 7! | i | i 7! 10 1 Z = ↵ 0 ei↵ | ✓ ◆ = = = = = = = – Frob.
Load more

Recommended publications
  • Information Geometry and Frobenius Algebra
    Information geometry and Frobenius algebra Ruichao Jiang, Javad Tavakoli, Yiqiang Zhao Oct 2020 Abstract We show that a Frobenius sturcture is equivalent to a dually flat sturcture in information geometry. We define a multiplication structure on the tangent spaces of statistical manifolds, which we call the statisti- cal product. We also define a scalar quantity, which we call the Yukawa term. By showing two examples from statistical mechanics, first the clas- sical ideal gas, second the quantum bosonic ideal gas, we argue that the Yukawa term quantifies information generation, which resembles how mass is generated via the 3-points interaction of two fermions and a Higgs boson (Higgs mechanism). In the classical case, The Yukawa term is identically zero, whereas in the quantum case, the Yukawa term diverges as the fu- gacity goes to zero, which indicates the Bose-Einstein condensation. 1 Introduction Amari in his own monograph [1] writes that major journals rejected his idea of dual affine connections on the grounds of their nonexistence in the mainstream Riemannian geometry. Later on, this dualistic structure turned out to be useful in information science, e.g. EM algorithms. The aim of this paper is to show the Frobenius algebra structure in information geometry and thus give a physical meaning for the Amari-Chentsov tensor. In information geometry, instead of the usual Levi-Civita connection, a non- metrical connections and its dual ∗ are used. Associated with these two connections is a mysterious∇ tensor, called∇ the Amari-Chentsov tensor (AC ten- arXiv:2010.05110v1 [math.DG] 10 Oct 2020 sor) and a one-parameter family of flat connections, called the α-connections.
    [Show full text]
  • Frobenius Algebras and Planar Open String Topological Field Theories
    Frobenius algebras and planar open string topological field theories Aaron D. Lauda Department of Pure Mathematics and Mathematical Statistics, University of Cambridge, Cambridge CB3 0WB UK email: [email protected] October 29, 2018 Abstract Motivated by the Moore-Segal axioms for an open-closed topological field theory, we consider planar open string topological field theories. We rigorously define a category 2Thick whose objects and morphisms can be thought of as open strings and diffeomorphism classes of planar open string worldsheets. Just as the category of 2-dimensional cobordisms can be described as the free symmetric monoidal category on a commutative Frobenius algebra, 2Thick is shown to be the free monoidal category on a noncommutative Frobenius algebra, hence justifying this choice of data in the Moore-Segal axioms. Our formalism is inherently categorical allowing us to generalize this result. As a stepping stone towards topological mem- brane theory we define a 2-category of open strings, planar open string worldsheets, and isotopy classes of 3-dimensional membranes defined by diffeomorphisms of the open string worldsheets. This 2-category is shown to be the free (weak monoidal) 2-category on a ‘categorified Frobenius al- gebra’, meaning that categorified Frobenius algebras determine invariants of these 3-dimensional membranes. arXiv:math/0508349v1 [math.QA] 18 Aug 2005 1 Introduction It is well known that 2-dimensional topological quantum field theories are equiv- alent to commutative Frobenius algebras [1, 16, 29]. This simple algebraic characterization arises directly from the simplicity of 2Cob, the 2-dimensional cobordism category. In fact, 2Cob admits a completely algebraic description as the free symmetric monoidal category on a commutative Frobenius algebra.
    [Show full text]
  • Arxiv:Math/9805094V2
    FROBENIUS MANIFOLD STRUCTURE ON DOLBEAULT COHOMOLOGY AND MIRROR SYMMETRY HUAI-DONG CAO & JIAN ZHOU Abstract. We construct a differential Gerstenhaber-Batalin-Vilkovisky alge- bra from Dolbeault complex of any closed K¨ahler manifold, and a Frobenius manifold structure on Dolbeault cohomology. String theory leads to the mysterious Mirror Conjecture, see Yau [29] for the history. One of the mathematical predictions made by physicists based on this con- jecture is the formula due to Candelas-de la Ossa-Green-Parkes [4] on the number of rational curves of any degree on a quintic in CP4. Recently, it has been proved by Lian-Liu-Yau [15]. The theory of quantum cohomology, also suggested by physicists, has lead to a better mathematical formulation of the Mirror Conjecture. As explained in Witten [28], there are two topological conformal field theories on a Calabi-Yau manifold X: A theory is independent of the complex structure of X, but depends on the K¨aher form on X, while B theory is independent of the K¨ahler form of X, but depends on the complex structure of X. Vafa [25] explained how two quantum cohomology rings and ′ arise from these theories, and the notion of mirror symmetry could be translatedR R into the equivalence of A theory on a Calabi-Yau manifold X with B theory on another Calabi-Yau manifold Xˆ, called the mirror of X, such that the quantum ring can be identified with ′. For a mathematicalR exposition in termsR of variation of Hodge structures, see e.g. Morrison [19] or Bertin-Peters [2]. There are two natural Frobenius algebras on any Calabi-Yau n-fold, A(X)= n Hk(X, Ωk), B(X)= n Hk(X, Ω−k), ⊕k=0 ⊕k=0 where Ω−k is the sheaf of holomorphic sections to ΛkTX.
    [Show full text]
  • Frobenius Algebras and Their Quivers
    Can. J. Math., Vol. XXX, No. 5, 1978, pp. 1029-1044 FROBENIUS ALGEBRAS AND THEIR QUIVERS EDWARD L. GREEN This paper studies the construction of Frobenius algebras. We begin with a description of when a graded ^-algebra has a Frobenius algebra as a homo- morphic image. We then turn to the question of actual constructions of Frobenius algebras. We give a, method for constructing Frobenius algebras as factor rings of special tensor algebras. Since the representation theory of special tensor algebras has been studied intensively ([6], see also [2; 3; 4]), our results permit the construction of Frobenius algebras which have representa­ tions with prescribed properties. Such constructions were successfully used in [9]. A special tensor algebra has an associated quiver (see § 3 and 4 for defini­ tions) which determines the tensor algebra. The basic result relating an associated quiver and the given tensor algebra is that the category of represen­ tations of the quiver is isomorphic to the category of modules over the tensor algebra [3; 4; 6]. One of the questions which is answered in this paper is: given a quiver J2, is there a Frobenius algebra T such that i2 is the quiver of T; that is, is there a special tensor algebra T = K + M + ®« M + . with associated quiver j2 such that there is a ring surjection \p : T —> T with ker \p Ç (®RM + ®%M + . .) and Y being a Frobenius algebra? This question was completely answered under the additional constraint that the radical of V cubed is zero [8, Theorem 2.1]. The study of radical cubed zero self-injective algebras has been used in classifying radical square zero Artin algebras of finite representation type [11].
    [Show full text]
  • On the Frobenius Manifold
    Frobenius manifolds and Frobenius algebra-valued integrable systems Dafeng Zuo (USTC) Russian-Chinese Conference on Integrable Systems and Geometry 19{25 August 2018 The Euler International Mathematical Institute 1 Outline: Part A. Motivations Part B. Some Known Facts about FM Part C. The Frobenius algebra-valued KP hierarchy Part D. Frobenius manifolds and Frobenius algebra-valued In- tegrable systems 2 Part A. Motivations 3 KdV equation : 4ut − 12uux − uxxx = 0 3 2 2 Lax pair: Lt = [L+;L];L = @ + 2 u tau function: u = (log τ)xx Bihamiltonian structure(BH): ({·; ·}2 =) Virasoro algebra) n o n o ( ) R R 3 f;~ ~g = 2 δf @ δg dx; f;~ ~g = −1 δf @ + 2u @ + 2 @ u δg dx: 1 δu @x δu 2 2 δu @x3 @x @x δu Dispersionless =) Hydrodynamics-type BH =) Frobenius manifold ······ 4 Natural generalization Lax pair/tau function/BH: KdV =) GDn / DS =) KP (other types) (N) {·; ·}2: Virasoro =) Wn algbra =) W1 algebra Lax pair/tau function/BH: dKdV =) dGDn =) dKP (N) {·; ·}2: Witt algebra =) wn algbra =) w1 algebra FM: A1 =) An−1 =) Infinite-dimensional analogue (?) 5 Other generalizations: the coupled KdV 4vt − 12vvx − vxxx = 0; 4wt − 12(vw)x − wxxx = 0: τ1 tau function: v = (log τ0)xx; w = ( )xx: τ0 R. Hirota, X.B.Hu and X.Y.Tang, J.Math.Anal.Appl.288(2003)326 BH: A.P.Fordy, A.G.Reyman and M.A.Semenov-Tian-Shansky,Classical r-matrices and compatible Poisson brackets for coupled KdV systems, Lett. Math. Phys. 17 (1989) 25{29. W.X.Ma and B.Fuchssteiner, The bihamiltonian structure of the perturbation equations of KdV Hierarchy.
    [Show full text]
  • Orbifold Frobenius Algebras, Cobordisms and Monodromies
    http://dx.doi.org/10.1090/conm/310/05402 Contemporary Mathematics Volume 310, 2002 Orbifold Frobenius Algebras, Cobordisms and Monodromies Ralph M. Kaufmann University of Southern California, Los Angeles, USA* ABSTRACT. We introduce the new algebraic structure replacing Frobenius al- gebras when one is considering functors from objects with finite group actions to Frobenius algebras, such as cohomology, the local ring of an isolated singu- larity, etc.. Our new structure called a G-twisted Frobenius algebra reflects the "stringy" geometry of orbifold theories or equivalently theories with fi- nite gauge group. We introduce this structure algebraically and show how it is obtained from geometry and field theory by proving that it parameterizes functors from the suitably rigidified version of the cobordism category of one dimensional closed manifolds with G bundles to linear spaces. We further- more introduce the notion of special G-twisted Frobenius algebras which are the right setting for studying e.g. quasi-homogeneous singularities with sym- metries or symmetric products. We classify the possible extensions of a given linear data to G-Frobenius algebras in this setting in terms of cohomological data. Introduction We consider the "stringy" geometry and algebra of global orbifold theories. They arise when one is considering the "stringy" extension of a classical functor which takes values in Frobenius algebras -such as cohomology, local ring, K-theory, etc.- in the presence of a finite group action on the objects. In physics the names of orbifold theories or equivalently theories with a global finite gauge group are associated with this type of question [DHVW, DW,DVVV,IV,V].
    [Show full text]
  • Nakayama Twisted Centers and Dual Bases of Frobenius Cellular Algebras
    NAKAYAMA TWISTED CENTERS AND DUAL BASES OF FROBENIUS CELLULAR ALGEBRAS YANBO LI Abstract. For a Frobenius cellular algebra, we prove that if the left (right) dual basis of a cellular basis is again cellular, then the algebra is symmetric. Moreover, some ideals of the center are constructed by using the so-called Nakayama twisted center. 1. Introduction Frobenius algebras are finite dimensional algebras over a field that have a certain self-dual property. These algebras appear in not only some branches of algebra, such as representation theory, Hopf algebras, algebraic geometry and so on, but also topology, geometry and coding theory, even in the work on the solutions of Yang-Baxter equation. Symmetric algebras including group algebras of finite groups are a large source examples. Furthermore, finite dimensional Hopf algebras over fields are Frobenius algebras for which the Nakayama automorphism has finite order. Cellular algebras were introduced by Graham and Lehrer in 1996. The theory of cellular algebras provides a linear method to study the representa- tion theory of many interesting algebras. The classical examples of cellular algebras include Hecke algebras of finite type, Ariki-Koike algebras, q-Schur algebras, Brauer algebras, partition algebras, Birman-Wenzl algebras and so on. We refer the reader to [2, 3, 13, 14] for details. It is helpful to point out that some cellular algebras are symmetric, including Hecke algebras of finite type, Ariki-Koike algebras satisfying certain conditions et cetera. In [8, 10, 11], Li and Xiao studied the general theory of symmetric cellular arXiv:1310.3699v1 [math.RA] 14 Oct 2013 algebras, such as dual bases, cell modules, centers and radicals.
    [Show full text]
  • Frobenius Algebra Structure in Hopf Algebras and Cohomology Ring with Poincaré Duality
    FROBENIUS ALGEBRA STRUCTURE IN HOPF ALGEBRAS AND COHOMOLOGY RING WITH POINCARÉ DUALITY SIQI CLOVER ZHENG Abstract. This paper aims to present the Frobenius algebra structures in finite-dimensional Hopf algebras and cohomology rings with Poincaré duality. We first introduce Frobenius algebras and their two equivalent definitions. Then, we give a concise construction of FA structure within an arbitrary finite- dimensional Hopf algebra using non-zero integrals. Finally, we show that a cohomology ring with Poincaré duality is a Frobenius algebra with a non- degenerate bilinear pairing induced by cap product. Contents 1. Introduction1 2. Preliminaries1 3. Frobenius Algebras3 4. Frobenius Algebra Structure in Hopf Algebras5 4.1. Existence of Non-zero Integrals6 4.2. The Converse direction 10 5. Frobenius Algebra Structure in Cohomology Ring 11 Acknowledgement 12 References 12 1. Introduction A Frobenius algebra (FA) is a vector space that is both an algebra and coal- gebra in a compatible way. Structurally similar to Hopf algebras, it is shown that every finite-dimensional Hopf algebra admits a FA structure [8]. In this paper, we will present a concise version of this proof, focusing on the construction of non- degenerate bilinear pairings. Another structure that is closely related to Frobenius algebras is cohomology ring with Poincaré duality. Using cap product, we will show there exists a natural FA structure in cohomology rings where Poincaré duality holds. To understand these structural similarities, we need to define Frobenius algebras and some compatibility conditions. 2. Preliminaries Definition 2.1. An algebra is a vector space A over a field k, equipped with a linear multiplication map µ : A ⊗ A ! A and unit map η : k ! A such that Date: October 17, 2020.
    [Show full text]
  • Introduction to Frobenius Manifolds
    INTRODUCTION TO FROBENIUS MANIFOLDS NOTES FOR THE MRI MASTER CLASS 2009 1. FROBENIUS ALGEBRAS Definition and examples. For the moment we fix a field k which contains Q, such as R, C or Q itself. To us a k-algebra is simply a k-vector space A which comes with k-bilinear map (the product) A × A A, (a; b) 7 ab which is associative ((ab)c = a(bc) for all a; b; c 2 A) and a unit element e 2 A for that product: e:a = e:1 = e for all a 2 A. We use! e to embed!k in A by λ 2 k 7 λe and this is why we often write 1 instead of e. Definition 1.1. Let A be a k-algebra that is commutative, associative and fi- nite dimensional! as a k-vector space. A trace map on A is a k-linear function I : A k with the property that the map (a; b) 2 A × A 7 g(a; b) := I(ab) is nondegenerate as a bilinear form. In other words, the resulting map ∗ a 7 !I(a:-) is a k-linear isomorphism of A onto the space! A of k-linear forms on A. The pair (A; I) is the called a Frobenius k-algebra. Remark! 1.2. This terminology can be a bit confusing: for a finite dimen- sional k-algebra A, one defines its trace Tr : A k as the map which assigns to a 2 A the trace of the operator x 2 A 7 ax 2 A.
    [Show full text]
  • Frobenius Algebras
    Frobenius algebras Andrew Baker November 2010 Andrew Baker Frobenius algebras Frobenius rings Let R be a ring and write R M , MR for the categories of left and right R-modules. More generally, for a second ring S, write R MS for the category of R − S-bimodules. A left R-module P is projective if every diagram of solid arrows in R M P ef f ~ p M / N / 0 with exact row extends to a diagram of the form shown. ∼ It is standard that every free module F = i R is projective. In fact, P is projective if and only if P is a retract of a free module, L i.e., for some Q, P ⊕ Q is free. The category R M has enough projectives, i.e., for any left R-module M there is an epimorphism P ։ M with P projective. Andrew Baker Frobenius algebras There are similar notions for right R-modules and R − S-bimodules. Dually, A left R-module I is injective if every diagram of solid arrows in R M > I ge O g o o M j N 0 with exact row extends to a diagram of the form shown. It is not immediately obvious what injectives there are. For R = Z (or more generally any pid) a module is injective if and only if it is divisible. Thus Q and Q/Z are injective Z-modules. In fact R M has enough injectives, i.e.,for any left R-module M there is a monomorphism M ֌ I with I injective.
    [Show full text]
  • A New Description of Orthogonal Bases
    A new description of orthogonal bases Bob Coecke, Dusko Pavlovic and Jamie Vicary Oxford University Computing Laboratory Abstract We show that an orthogonal basis for a finite-dimensional Hilbert space can be equivalently characterised as a commutative †-Frobenius monoid in the category FdHilb, which has finite-dimensional Hilbert spaces as objects and continuous linear maps as morphisms, and tensor product for the monoidal structure. The basis is normalised exactly when the corresponding commutative †-Frobenius monoid is special. Hence orthogonal and orthonormal bases can be axiomatised in terms of composition of operations and tensor product only, without any explicit reference to the underlying vector spaces. This axiomatisation moreover admits an operational interpretation, as the comultiplication copies the basis vectors and the counit uniformly deletes them. That is, we rely on the distinct ability to clone and delete classical data as compared to quantum data to capture basis vectors. For this reason our result has important implications for categorical quantum mechanics. 1 Introduction Given any orthonormal basis {|φii}i in a finite dimensional Hilbert space H we can always define the linear maps arXiv:0810.0812v1 [quant-ph] 5 Oct 2008 δ : H → H ⊗ H :: |φii 7→ |φii ⊗ |φii (1) and ǫ : H → C :: |φii 7→ 1 . (2) It was observed in [6] that the triple (H,δ,ǫ) is a so-called commutative special †-Frobenius comonoid in the category FdHilb of finite dimensional Hilbert spaces and linear maps with the tensor product as monoidal structure. Meanwhile, this fact that orthonormal bases can be encoded as commutative special †-Frobenius monoids has resulted in many important 1 applications in the area of categorical quantum mechanics, for example, for describing the flow of classical information in quantum informatic protocols [6], for defining complementarity and special quantum logic gates in quantum computational schemes [4] and for constructing discrete models for quantum reasoning [5].
    [Show full text]
  • Types, Codes and Tfts
    Types, Codes and TFTs Roland Friedrich∗ May 8, 2018 Abstract We establish a relation between fully extended 2-dimensional TQFTs and recognisable weighted formal languages, rational biprefix codes and lattice TFTs. We show the equiva- lence of 2D closed TFTs and rational exchangeable series and we discuss the important special case of finite groups. Finally, we outline a reformulation in terms of a restricted version of second order monadic logic. Contents 1 Preliminaries 1 1.1 Rational series . .2 1.2 Codes . .3 1.3 Frobenius algebras . .4 1.4 Bicategories . .4 1.5 Automaticity . .5 2 Fully extended two-dimensional TFTs6 2.1 Group algebras . .8 arXiv:1805.02286v1 [math.RA] 6 May 2018 3 Two-cobordism and second order monadic logic8 1 Preliminaries Let k be a field of characteristic zero. We consider the following categories: Algk, of associative and unital k-algebras, cAlgk, associative, commutative and unital k-algebras and fGrp, of finite groups. We assume all algebras to be unital and, if necessary, k also to be algebraically closed, which we shall indicate. ∗Saarland University, [email protected] 1 1.1 Rational series We recall a few facts about formal series and rational languages from [3,4,7, 19]. Let X be a finite set, called alphabet, and X∗ the free monoid generated by X, i.e. the set of all possible words w ∗ over X, including the empty word 1. A map S : X ! k, w 7! S(w) =: Sw is called a formal series, and the k-algebra of all formal series is khhXii.
    [Show full text]