Baxter Algebras and Hopf Algebras
Differential Algebra Structures on Familes of Trees
functions. This was used in [1] and [2] to derive geometrically stable numerical integration algorithms, although the results are presented differently.
1
Introduction
Let k be a field, R be a commutative k -algebra, and Der(R) the Lie algebra of derivations of R. It is known that the vector space spanned by labeled rooted trees forms a Hopf algebra [4]. Let H denote the Hopf algebra of rooted trees whose non root nodes are labeled using derivations D ∈ Der(R) [4]. For such a Hopf algebra, we introduce a class of H -module algebras which we call Leibnitz, and give a construction which yields a variety of different Leibnitz H -module algebras (Theorem 3.11). We also show how Leibnitz H -module algebras are related to Nichols and Weisfeiler’s R/k -bialgebras [10], which arise in Hopf-algebra approaches to differential algebra (Theorem 4.7). In Section 5 we also give a method for describing quotients of Leibnitz H -module algebras (Theorem 5.8). Hopf algebras can be used to simplify computations of derivations [5]. In the same way, Leibnitz H -module algebras can be used to simplify the symbolic computation of derivations acting on polynomials and other algebras of 1
第十二届全国代数学术会议大会报告摘要
第十二届全国代数学术会议大会报告摘要Classical Yang-Baxter equation,its extensions and some related algebraicstructures白承铭南开大学Wefirst give a brief introduction to the classical Yang-Baxter equation which emphasizes the relationship between the tensor and operator forms.Then we give two approaches to extend the classical Yang-Baxter equation,motivated by the study of different topics like integrable systems,Rota-Baxter algebras and Lie bialgebras.Moreover,there are some interesting algebraic structures behind these two approaches.Representation type of algebras:Yesterday,today and tomorrow韩阳中国科学院数学与系统科学研究院Email:***********.cnOne task in representation theory of algebras is to classify all representations of an algebra.Before this,one needs to judge whether it is hopeful for an algebra to do so or not,namely,to determine the representation type of an algebra.In this survey,some concepts,results,ideas,methods,and problems on representation type of algebras are introduced.群环的代数K理论唐国平中科院研究生院数学科学学院报告将分为三个部分:1)本质循环群(具有指数有限的循环子群的群)的整群环的K理论。
Lie algebras, in Infinite-dimensional Lie algebras and groups, Adv. Ser. in Math. Phys. 7,
C1;1;k g ' L0;k (0)
L1;k (1)
M1;k (1): Combining Theorem 4.6 and the statement (ii), we obtain the statement (i). Q.E.D.
References
H0 (g(0; 1; 1); L0 ;k (0)
Department of Mathematics, Faculty of Science, Kyoto University, Kyoto 606-8502, Japan. Department of Mathematics, Faculty of Science, Osaka University,
[KK] Kac V.G. and Kazhdan D.A., Structure of representations with highest weight of in nite dimensional Lie algebras, Adv. in Math. 34, (1979), 97{108. [KnPZ] Knizhnik V. G., Polyakov A. M. and Zamolodchikov A.B., Fractal structure in 2D quantum gravity, Mod. Phys. Lett. A 3, (1988), 819{826. [KW1] Kac V.G. and Wakimoto M., Modular invariant representations of in nite dimensional Lie algebras and superalgebras, Proc. Natl. Acad. Soc., 35, (1988), 4956{4960. [KW2] Kac V.G. and Wakimoto M., Classi cation of modular invariant representations of ane Lie algebras, in In nite-dimensional Lie algebras and groups, Adv. Ser. in Math. Phys. 7, (1989), 138{177. [KWn] Kac V. G. and Wang W., Vertex operator superalgebras and their representations, Mathematical aspects of conformal and topological eld theories and quantum groups, 161{191, Contemp. Math. 175, Amer. Math. Soc. Providence, RI, (1994). [Mal] Malikov F.G., Verma modules over Kac-Moody algebras of rank 2, Leningrad Math. J., 2, No. 2, (1991), 269{286. [MFF] Malikov F.G., Feigin B.L. and Fuks D.B., Singular vectors in Verma modules over KacMoody algebras, Funkts. Anal. Prilozhen., 20, No. 2, (1988), 25{37. [MW] Mathieu P. and Walton M.A., Fractional-level Kac-Moody Algebras and Nonunitary Coset Conformal Theories, Prog. Theor. Phys. 102, (1990), 229-254. [MP] Moody R.V. and Pianzola A., Lie algebras with triangular decompositions, Wiley-Interscience Publ., New York, 1995. [P] Polyakov A. M., Quantum Gravity in two dimensions, Mod. Phys. Lett. A 2, (1987), 893-898. [Ray] Ray U., A Characterization of Lie superalgebras for a certain class of graded Lie superalgebras, preprint,to appear in Jour. Alg. [RW] Rocha-Caridi A. and Wallach N.R., Highest weight modules over graded Lie algebras: resolutions, ltrations and character formulas, Trans. Amer. Math. Soc. 20, (1983), 133{162. [TUY] Tsuchiya A., Ueno K. and Yamada Y., Conformal eld theory on moduli family of stable curves with gauge symmetry, in Integrable systems in quantum eld theory and statistical mechanics, Adv. Stud. Pure Math. 19, (1989), 459-566. [V] Verlinde E., Fusion rules and modular transformations in 2D conformal eld theory, Nucl. Phys. B 300, (1998), 360-376. (K. Iohara) (Y. Koga)
Algebras and Hopf Algebras in Braided Categories
a rXiv:q -alg/95923v122Se p1995July 1993Published in Advances in Hopf Algebras,Marcel Dekker Lec.Notes Pure and Applied Maths 158(1994)55-105.ALGEBRAS AND HOPF ALGEBRAS IN BRAIDED CATEGORIES 1SHAHN MAJID 2Department of Applied Mathematics &Theoretical Physics University of Cambridge,Cambridge CB39EW,U.K.ABSTRACT This is an introduction for algebraists to the theory of algebras and Hopf algebras in braided categories.Such objects generalise super-algebras and super-Hopf algebras,as well as colour-Lie algebras.Basic facts about braided categories C are recalled,the modules and comodules of Hopf algebras in such categories are studied,the notion of ‘braided-commutative’or ‘braided-cocommutative’Hopf algebras (braided groups)is reviewed and a fully diagrammatic proof of the reconstruction theorem for a braided group Aut (C )is given.The theory has important implications for the theory of quasitriangular Hopf algebras (quantum groups).It also includes important examples such as the degenerate Sklyanin algebra and the quantum plane.One of the main motivations of the theory of Hopf algebras is that they provide a gener-alization of groups.Hopf algebras of functions on groups provide examples of commutativeHopf algebras,but it turns out that many group-theoretical constructions work just as well when the Hopf algebra is allowed to be non-commutative.This is the philosophy associated to some kind of non-commutative (or so-called quantum)algebraic geometry.In a Hopf algebra context one can say the same thing in a dual way:group algebras and enveloping algebras are cocommutative but many constructions are not tied to this.This point of view has been highly successful in recent years,especially in regard to the quasitriangular Hopf algebras of Drinfeld[11].These are non-cocommutative but the non-cocommutativity is controlled by a quasitriangular structure R .Such objects are commonly called quantum ing out of physics,notably associated to solutions of the Quantum Yang-Baxter Equations (QYBE)is a rich supply of quantum groups.Here we want to describe some kind of rival or variant of these quantum groups,which we call braided groups[44]–[52].These are motivated by an earlier revolution that was very popular some decades ago in mathematics and physics,namely the theory of super orZ2-graded algebras and Hopf algebras.Rather than make the algebras non-commutative etc one makes the notion of tensor product⊗non-commutative.The algebras remain commutative with respect to this new tensor product(they are super-commutative).Under this point of view one has super-groups,super-manifolds and super-differential geometry. In many ways this line of development was somewhat easier than the notion of quantum geometry because it is conceptually easier to make an entire shift of category from vector spaces to super-vector spaces.One can study Hopf algebras in such categories also(super-quantum groups).In this second line of development an obvious(and easy)step was to generalise such constructions to the case of symmetric tensor categories[27].These have a tensor product ⊗and a collection of isomorphismsΨgeneralizing the transposition or super-transposition map but retaining its general properties.In particular,one keepsΨ2=id so that these generalized transpositions still generate a representation of the symmetric group.Since only such general properties are used in most algebraic constructions,such as Hopf algebras and Lie algebras,these notions immediately(and obviously)generalise to this setting.See for example Gurevich[19],Pareigis[61],Scheunert[67]and numerous other authors.On the other hand,the theory is not fundamentally different from the super-case.Rather more interesting is the further generalization to relax the condition thatΨ2=id. NowΨandΨ−1must be distinguished and are more conveniently represented by braid-crossings rather than by permutations.They generate an action of the Artin braid group on tensor products.Such quasitensor or braided-tensor categories have been formally in-troduced into category theory in[24]and also arise in the representation theory of quantum groups.The study of algebras and Hopf algebras in such categories is rather more non-trivial than in the symmetric case.It is this theory that we wish to describe here.It has been introduced by the author under the heading‘braided groups’as mentioned above. Introduced were the relevant notions(not all of them obvious),the basic lemmas(such as a braided-tensor product analogous to the super-tensor product of super-algebras)and a construction leading to a rich supply of examples.On the mathematical level this project of‘braiding’all of mathematics is,I believe, a deep one(provided one goes from the symmetric to the truly braided case).Much of mathematics consists of manipulating symbols,making transpositions etc.The situation appears to be that in many constructions the role of permutation group can(with care) be played equally well by the braid group.Not only the algebras and braided groups to be described here,but also braided differential calculus,braided-binomial theorems and braided-exponentials are known[57]as well as braided-Lie algebras[58].Much more can be expected.Ultimately we would like some kind of braided geometry comparable to the high-level of development in the super case.Apart from this long-term philosophical motivation,one can ask what are the more immediate applications of this kind of braided geometry?I would like to mentionfive of them.1.Many algebras of interest in physics such as the degenerate Sklyanin algebra,quantumplanes and exchange algebras are not naturally quantum groups but turn out to be braided ones[52][56].There are braided-matrices B(R)and braided-vectors V(R′) associated to R-matrices.2.The category of Hopf algebras is not closed under quotients in a good sense.Forexample,if H⊂H1is covered by a Hopf algebra projection then H1∼=B>⊳H whereB is a braided-Hopf algebra.This is the right setting for Radford’s theorem as wehave discovered and explained in detail in[52].3.Braided groups are best handled by means of braid diagrams in which algebraicoperations‘flow’along strings.This means deep connections with knot theory and is also useful even for ordinary Hopf algebras.For example,you can dualise theorems geometrically by turning the diagram-proof up-side-down andflip conventions by viewing in a mirror.4.A useful tool in the theory of quasitriangular Hopf algebras(quantum groups)via aprocess of transmutation.By encoding their non-cocommutativity as braiding in a braided category they appear‘cocommutative’.Likewise,dual quasitriangular Hopf algebras are rendered‘commutative’by this process[45][49].5.In particular,properties of the quantum groups O q(G)and U q(g)are most easilyunderstood in terms of their braided versions B q(G)and BU q(g).This includes an Ad-invariant‘Lie algebra-like’subspace L⊂U q(g)and an isomorphism B q(G)∼=U q(g)[50][52].An outline of the paper is the following.In Section1we recall the basic notions of braided tensor categories and how to work in them,and some examples.We recall basic facts about quasitriangular and dual quasitriangular Hopf algebras and the braided cate-gories they generate.In Section2we do diagrammatic Hopf-algebra theory in this setting. In Section3we give a new diagrammatic proof of our generalised Tannaka-Krein-type re-construction theorem.In Section4we explain the results about ordinary quantum groups obtained from this braided theory.In Section5we end with basic examples of braided matrices etc associated to an R-matrix.Although subsequently of interest in physics,the braided matrices arose quite literally from the Tannaka-Krein theorem mentioned above. This is an example of pure mathematics feeding back into physics rather than the other way around(for a change).Our work on braided groups(or Hopf algebras in braided categories)was presented to the Hopf algebra community at the Euler Institute in Leningrad,October1990and at the Biannual Meeting of the American Maths Society in San Francisco,January1991and published in[48][49].The result presented at these meetings was the introduction of Hopf algebras living in the braided category of comodules of a dual quasitriangular Hopf algebra. The connection between crossed modules(also called Drinfeld-Yetter categories)and the quantum double as well as the connection with Radford’s theorem were introduced in[38] in early1990.The braided interpretation of Radford’s theorem was introduced in detail in[52]and circulated at the start of1992.Dual quasitriangular(or coquasitriangular) Hopf algebras themselves were developed in connection with Tannaka-Krein ideas in[36, Sec.4][48][49,Appendix](and earlier in other equivalent forms).A related Tannaka-Krein theorem in the quasi-associative dual quasitriangular setting was obtained in[43]at the Amherst conference and circulated infinal form in the Fall of1990.It is a pleasure to see that some of these ideas have subsequently proven of interest in Hopf algebra circles(directly or indirectly).I would also like to mention some constructions of Lyubashenko[30][31]relating to our joint work[32].Also in joint work with Gurevich[21] the transmutation construction is related to Drinfeld’s process of twisting[13].Several otherpapers can be mentioned here.On the whole I have resisted the temptation to give a full survey of all results obtained so far.Instead,the aim here is a more pedagogical exposition of the more elementary results,with proofs.Throughout this paper we assume familiarity with usual techniques of Hopf algebras such as in the book of Sweedler[69].In this sense the style(and also the motivation)is somewhat different from our braided-groups review article for physicists[42].We work over afield k.With more care one can work here with a ring just as well.When working with matrix or tensor components we will use the convention of summing over repeated indices.Some of the elementary quantum groups material should appear in more detail in my forthcoming book.1Braided CategoriesHere we develop the braided categories within which we intend to work,namely those coming from(co)modules of quantum groups.In fact,the theory in Sections2,3is not tied to quantum groups and works in any braided category.The material in the present section is perfectly standard by now.1.1Definition and General ConstructionsSymmetric monoidal(=tensor)categories have been known for some time and we refer to [27]for details.The model is the category of k-modules.The notion of braided monoidal (=braided tensor=quasitensor)category is a small generalization if this.Briefly,a monoidal category means(C,⊗,ΦV,W,Z,1for the tensor product and associated functorial isomorphisms l V:V→1for all objects V,which we likewise suppress.A monoidal category C is rigid(=has left duals)if for each object V,there is an object V∗and morphisms ev V:V∗⊗V→1→V⊗V∗such that→(V⊗V∗)⊗V∼=V⊗(V∗⊗V)ev→V(1)V coev→V∗⊗(V⊗V∗)∼=(V∗⊗V)⊗V∗ev→V∗(2)V∗coevcompose to id V and id V∗respectively.A single object has a left dual if V∗,ev V,coev V exist. The model is that of afinite-dimensional vector space(orfinitely generated projective module when k is a ring).Finally,the monoidal category is braided if it has a quasisymmetry or‘braiding’Ψgiven as a natural transformation between the two functors⊗and⊗op(with opposite product) from C×C→C.This is a collection of functorial isomorphismsΨV,W:V⊗W→W⊗V obeying two‘hexagon’coherence identities.In our suppressed notation these areΨV⊗W,Z=ΨV,Z◦ΨW,Z,ΨV,W⊗Z=ΨV,Z◦ΨV,W(3)while identities such asΨV,1,V (4)can be deduced.If Ψ2=id then one of the hexagons is superfluous and we have an ordinary symmetric monoidal category.Let us recall that the functoriality of maps such as those above means that they commute in a certain sense with morphisms in the category.For example,functoriality of ΨmeansΨZ,W (φ⊗id)=(id ⊗φ)ΨV,W ∀φV ↓Z ,ΨV,Z (id ⊗φ)=(φ⊗id)ΨV,W ∀φW↓Z .(5)These conditions(3)-(5)are just the obvious properties that we take for granted when transposing ordinary vector spaces or super-vector spaces.In these cases Ψis the twist map ΨV,W (v ⊗w )=w ⊗v or the supertwistΨV,W (v ⊗w )=(−1)|v ||w |w ⊗v (6)on homogeneous elements of degree |v |,|w |.The form of Ψin these familiar cases does not depend directly on the spaces V,W so we often forget this.But in principle there is a different map ΨV,W for each V,W and they all connect together as explained.In particular,note that for any two V,W we have two morphisms ΨV,W ,Ψ−1W,V :V ⊗W →W ⊗V and in the truly braided case these can be distinct.A convenient notation in this case is to write them not as permutations but as braid crossings.Thus we write morphisms pointing downwards (say)and instead of a usual arrow,we use the shorthandV WW V ΨW,V Ψ-1==V W W V V,W .(7)In this notation the hexagons (3)appear as==Z V W Z V W (8)The doubled lines refer to the composite objects V ⊗W and W ⊗Z in a convenient ex-tension of the notation.The coherence theorem for braided categories can be stated very simply in this notation:if two series of morphisms built from Ψ,Φcorrespond to the same braid then they compose to the same morphism.The proof is just the same as Mac Lane’s proof in the symmetric case with the action of the symmetric group replaced by that of the Artin braid group.This notation is a powerful one.We can augment it further by writing any other morphisms as nodes on a string connecting the inputs down to the outputs.Functoriality(5)then says that a morphism φ:V →Z say can be pulled through braid crossings,V W V W=V W V W =φφφφ(9)Similarly for Ψ−1with inverse braid crossings.An easy lemma using this notation is that for any braided category C there is another mirror-reversed braided monoidal category ¯C with the same monoidal structure but with braiding¯ΨV,W =Ψ−1W,V (10)in place of ΨV,W ,i.e with the interpretation of braid crossings and inverse braid crossings interchanged.Finally,because of (4)we can suppress the unit object entirely so the evaluation and co-evaluation appear simply as ev =∪and coev =∩.Then (1)-(2)appear as=V ev = coev =V V* VV V*=V V V V V* V*.(11)There is a similar notion of right duals V ˇand ¯ev V ,¯coev V for which the mirror-reflected double-bend here can be likewise straightened.Example 1.1Let R ∈M n (k )⊗M n (k )be invertible and obey the QYBER 12R 13R 23=R 23R 13R 12then the monoidal category C (V,R )generated by tensor products of V =C n is braided.Proof This is an elementary exercise (and extremely well-known).The notation is R 12=R ⊗id and R 23=id ⊗R in M ⊗3n .The braiding on basis vectors {e i }isΨ(e i ⊗e j )=e b ⊗e a R a i b j (12)extended to tensor products according to (3).The morphisms in the category are linear maps such that Ψis functorial with respect to them in the sense of (5).The associativity Φis the usual one on vector spaces.⊔⊓If R obeys further conditions then C (V,V ∗,R )generated by V,V ∗is rigid.One says that such an R is dualizable .For this there should exist among other things a ‘second-inverse’R =((R t 2)−1)t 2(13)where t 2is transposition in the second M n factor.This defines one of the mixed terms in the braidingΨV ∗,V ∗(f i ⊗f j )=R i a j b f b ⊗f a(14)ΨV,V∗(e i⊗f j)= R a i j b f b⊗e a(15)ΨV∗,V(f i⊗e j)=e a⊗f b R−1i b a j(16) where V∗={f i}is a dual basis.The evaluation and coevaluation are given by the usual morphismsev V(f i⊗e j)=δi j,coev V(1)= i e i⊗f i.(17)One needs also the second-inverse R−1forΨto be invertible.In this way one translates the various axioms into a linear space setting.We see in particular that the QYBE are nothing other than the braid relations in matrix form.We turn now to some general categorical constructions.One construction in[37][40] is based on the idea that a pair of monoidal categories C→V connected by a functor behaves in many ways like a bialgebra with⊗in C something like the product.In some cases this is actually true as we shall see in Section3in the form of a Tannaka-Krein-type reconstruction theorem,but we can keep it in general as motivation.Motivated by this we showed that for every pair C→V of monoidal categories there is a dual one C◦→V where C◦is the Pontryagin dual monoidal category[37].This generalised the usual duality for Abelian groups and bialgebras to the setting of monoidal categories.We also proved such things as a canonical functorC→◦(C◦).(18) Of special interest to us now is the case C→C where the functor is the identity one.So associated to every monoidal category C is another monoidal category C◦of‘representations’of⊗.This special case can also be denoted by C◦=Z(C)the‘center’or‘inner double’of C for reasons that we shall explain shortly.This case was found independently by V.G. Drinfeld who pointed out that it is braided.Proposition1.2[37][10]Let C be a monoidal category.There is a braided monoidal category C◦=Z(C)defined as follows.Objects are pairs(V,λV)where V is an object of C andλV is a natural isomorphism in Nat(V⊗id,id⊗V)such thatλV,1Proof The monoidal structure was found in the author’s paper[37]where full proofs were also given.We refer to this for details.Its preprint was circulated in the Fall of1989. The braiding was pointed out by Drinfeld[10]who had considered the construction from a very different and independent point of view to our duality one,namely in connection with the double of a Hopf algebra as we shall explain below.Another claim to the construction is from the direction of tortile categories[25].See also[40]for further work from the duality point of view.⊔⊓The‘double’point of view for this construction is based on the following example cf[10]. Example1.3Let H be a bialgebra over k and C=H M the monoidal category of H-modules.Then an object of Z(C)is a vector space V which is both a left H-module and an invertible left H-comodule such thath(1)v¯(1)⊗h(2)⊲v¯(2)= (h(1)⊲v)¯(1)h(2)⊗(h(1)⊲v)¯(2),∀h∈H,v∈V.In this form Z(H M)coincides with the category H H M of H-crossed modules[72]with an additional invertibility condition.The braiding isΨV,W(v⊗w)= v¯(1)⊲w⊗v¯(2).The invertibility condition on the comodules ensures thatΨ−1exists,and is automatic if the bialgebra H has a skew-antipode.Proof The proof is standard from the point of view of Tannaka-Krein reconstruction methods(which we shall come to later).From C we can reconstruct H as the representing object for a certain functor.This establishes a bijection Lin(V,H⊗V)∼=Nat(V⊗id,id⊗V) under whichλV corresponds to a map V→H⊗V.ThatλV represents⊗corresponds then to the comodule property of this map.ThatλV is a collection of morphisms corresponds to the stated compatibility condition between this coaction and the action on V as an object in C.To see this in detail let H L denote H as an object in C under the left action.Given λV a natural transformation we definev¯(1)⊗v¯(2)=λV,H L(v⊗1)(19) and check(id⊗λV,HL )(λV,HL⊗id)(v⊗1⊗1)=λV,HL⊗H L(v⊗(1⊗1))=λV,HL⊗H L(v⊗∆(1))=(∆⊗id)◦λV,HL(v⊗1)where thefirst equality is the fact thatλV‘represents’⊗and the last is thatλV is functorialunder the morphism∆:H L→H L⊗H L.The left hand side is the map V→H⊗V in (19)applied twice so we see that this map is a left coaction.Moreover,h(1)v¯(1)⊗h(2)⊲v¯(2)=h⊲λV,H L(v⊗1)=λV,H L(h⊲(v⊗1))= λV,H L(h(1)⊲v⊗R h(2)(1))= (λV,H L(h(1)⊲v⊗1))(h(2)⊗1) where thefirst equality is the definition(19)and the action of H on H L⊗V.The secondequality is thatλV,HLis a morphism in C.Thefinal equality uses functoriality underthe morphism R h(2):H L→H L given by right-multiplication to obtain the right handside of the compatibility condition.The converse directions are easier.Given a coaction V→H⊗V defineλV,W(v⊗w)= v¯(1)⊲w⊗v¯(2).This also implies at once the braiding Ψ=λas stated.Finally we note that in Proposition1.2the definition assumes that theλV are invertible. If we were to relax this then we would have a monoidal category which is just that of crossed modules as in[72],but thenΨwould not necessarily be invertible and hence would not be a true braiding.The invertibleλV correspond to left comodules which are invertible in the following sense:there exists a linear map V→V⊗H sending v to v[2]⊗v[1]say,suchthatv[2]¯(1)v[1]⊗v[2]¯(2)=1⊗v= v¯(2)[1]v¯(1)⊗v¯(2)[2],∀v∈V.(20) One can see that if such an‘inverse’exists,it is unique and a right comodule.Moreover, it is easy to see that the invertible comodules are closed under tensor products.They correspond toλ−1V in a similar way to(19)and withλ−1V,W(w⊗v)= v[2]⊗v[1]⊲w for the converse direction.In thefinite-dimensional case they provide left duals V∗with left coactionβV∗(f)(v)= v[1]f(v[2]).If the bialgebra H has a skew-antipode then every left comodule is invertible by composing with the skew-antipode.So in this case the condition becomes empty.From the categorical point of view in Proposition1.2,if C has right duals then everyλV,W is invertible,cf[37].The inverse is the right-adjoint ofλV,Wˇ,namelyλ−1V,W=(¯ev W⊗id)◦λV,Wˇ◦(id⊗¯coev W).When C=H M then thefinite-dimensional left modules have right duals if the bialgebra H has a skew-antipode,so in this case the invertibility ofλV is automatic.On the other hand,we do not need to make these suppositions here.This completes our computation of Z(H M).Apart from the invertibility restriction we see that it consists of compatible module-comodule structures as stated.⊔⊓Note that the notion of a crossed module is an immediate generalisation of the notion of a crossed G-module[71]with H=kG,the group algebra of afinite group G.In this case the category of crossed G-modules is well-known to be braided[18].Moreover,because the objects can be identified with underlying vector spaces,we know by the Tannaka-Krein reconstruction theorem[66]that there must exist a bialgebra coD(H)such that our braided-category is equivalent to that of right coD(H)-comodulesM coD(H)f.d.=H H M f.d.(21) Here we take the modules to befinite-dimensional as a sufficient(but not necessary)con-dition for a Tannaka-Krein reconstruction theorem to apply and the co-double coD(H)to exist.In the nicest case the category is also D(H)M f.d.for some D(H).This is an abstract definition of Drinfeld’s quantum double and works for a bialgebra.If it happens that H is a Hopf algebra with invertible antipode then one can see from the above that H H M f.d.is rigid and so coD(H)and D(H)will be Hopf algebras.The categorical reason is that H M f.d.is rigid and this duality extends to Z(C)with the dual ofλV defined by the left-adjoint ofλ−1V,W,namelyλV∗,W=(ev V⊗id)◦λ−1V,W◦(id⊗coev V). We will study details about categories of modules and comodules and the reconstruction theorems later in this section and in Section3.The point is that these categorical methods are very powerful.Proposition1.4[33]cf[11]If H is afinite-dimensional Hopf algebra then D(H)(the quan-tum double Hopf algebra of H)is built on H∗⊗H as a coalgebra with the product(a⊗h)(b⊗g)= b(2)a⊗h(2)g<Sh(1),b(1)><h(3),b(3)>,h,g∈H,a,b∈H∗where<,>denotes evaluation.Proof The quantum double D(H)was introduced by Drinfeld[11]as a system of genera-tors and relations built from the structure constants of H.The formula stated on H∗⊗H is easily obtained from this as done in[33].We have used here the conventions introduced in[38]that avoid the use of the inverse of the antipode.Also in[38]we showed that the modules of the double were precisely the crossed modules category as required.To see this simply note that H and H∗op are sub-Hopf algebras and hence a left D(H)-module is a left H-module and a suitably-compatible right H∗-module.The latter is equally well a left H-comodule compatible as in Example1.3.See[38]for details.⊔⊓In[33]we introduced a further characterization of the quantum double as a member of a class of double cross product Hopf algebras H1⊲⊳H2(in which H i are mutually acting on each other).Thus,D(H)=H∗op⊲⊳H where the actions are mutual coadjoint actions. In this form it is clear that the role of H∗can be played by H◦in the infinite dimensional Hopf algebra case.We will not need this further here.1.2Quasitriangular Hopf AlgebrasWe have already described one source of braided categories,namely as modules of the double D(H)(or comodules of the codouble)of a bialgebra.Abstracting from this one has the notion,due to Drinfeld,of a quasitriangular Hopf algebra.These are such that their category of modules is braided.Definition1.5[11]A quasitriangular bialgebra or Hopf algebra is a pair(H,R)where H is a bialgebra or Hopf algebra and R∈H⊗H is invertible and obeys(∆⊗id)R=R13R23,(id⊗∆)R=R13R12.(22)τ◦∆h=R(∆h)R−1,∀h∈H.(23) Here R12=R⊗1and R23=1⊗R etc,andτis the usual twist map.Thus these Hopf algebras are like cocommutative enveloping algebras or group algebras but are cocommutative now only up to an isomorphism implemented by conjugation by an element R.Some elementary(but important)properties areLemma1.6[12]If(H,R)is a quasitriangular bialgebra then R as an element of H⊗H obeys(ǫ⊗id)R=(id⊗ǫ)R=1.(24)R12R13R23=R23R13R12(25) If H is a Hopf algebra then one also has(S⊗id)R=R−1,(id⊗S)R−1=R,(S⊗S)R=R(26)∃S−1,u,v,S2(h)=uhu−1,S−2(h)=vhv−1∀h∈H(27)Proof For(24)applyǫto(22),thus(ǫ⊗id⊗id)(∆⊗id)R=R23=(ǫ⊗id⊗id)R13R23so that(since R23is invertible)we have(ǫ⊗id)R=1.Similarly for the other side.For(25)compute(id⊗τ◦∆)R in two ways:using the second of axioms(22)directly or usingaxiom(23),and then the second of(22).For(26)consider R(1)(1)S R(1)(2)⊗R(2)=1by the property of the antipode and equation(24)already proven,but equals R(S⊗id)R by axiom(22).Similarly for the other side,hence(S⊗id)R=R−1.Similarly for(id⊗S)R−1=Ronce we appreciate that(∆⊗id)(R−1)=(R13R23)−1=R−123R−113etc,since∆is an algebrahomomorphism.For(27)the relevant expressions areu= (S R(2))R(1),u−1= R(2)S2R(1),v=Suwhich one can verify to have the right properties.In addition one can see that∆u=(R21R12)−1(u⊗u)and similarly for v so that uv−1is group-like(and implements S4).Fordetails of the computations see[12]or reviews by the author.⊔⊓Here(25)is the reason that Physicists call R the‘universal R-matrix’(compare Ex-ample1.1).Indeed,in anyfinite-dimensional representation the image of R is such anR-matrix.There are well-known examples such as U q(sl2)and U q(g)[11][23].Here we giveperhaps the simplest known quasitriangular Hopf algebrasExample1.7[47]Let Z n=Z/n Z be thefinite cyclic group of order n and k Z n its groupalgebra with generator g.Let q be a primitive n-th root of unity.Then there is a quasitri-angular Hopf algebra Z′n consisting of this group algebra and∆g=g⊗g,ǫg=1,Sg=g−1,R=n−1n−1a,b=0q−ab g a⊗g b.(28)Proof We assume that k is of suitable characteristic.To verify the non-trivial quasitrian-gular structure we use that n−1 n−1b=0q ab=δa,0.Then R13R23=n−2 q−(ab+cd)g a⊗g c⊗g b+d =n−2 q−b(a−c)q−cb′g a⊗g c⊗g b′=n−1 q−ab′g a⊗g a⊗g b′=(∆⊗id)R where b′=b+d was a change of variables.Similarly for the second of(22).The remaining axiom(23)is automatic because the Hopf algebra is both commutative and cocommutative.⊔⊓Example1.8[2][54]Let G be afinite Abelian group and k(G)its function Hopf algebra. Then a quasitriangular structure on k(G)means a function R∈H⊗H obeying R(gh,f)=R(g,f)R(h,f),R(g,hf)=R(g,h)R(g,f),R(g,e)=1=R(e,g)for all g,h,f in G and e the identity element.I.e.,a quasitriangular structure on k(G) means precisely a bicharacter of G.Proof We identify k(G)⊗k(G)with functions on G×G,with pointwise multiplication. Using the comultiplication given by multiplication in G we have at once that(22)corre-sponds to thefirst two displayed equations.Axiom(23)becomes hg R(g,h)=R(g,h)gh and so is automatic because the group is Abelian.Given thesefirst two of the stated conditions,the latter two hold iffR is invertible.⊔⊓The Z′n example here also has an immediate generalization to the group algebra kG of afinite Abelian group equipped with a bicharacter onˆG.This just coincides with the last example applied to k(ˆG)=kG.Finally,we return to our basic construction,。
algebra 词根
"Algebra" 这个词的词根源自阿拉伯数学传统。
它的起源可以追溯到阿拉伯数学家、科学家和学者穆罕默德·本·穆萨·昂瓦尔·赞杜(Muhammad ibn Musa al-Khwarizmi)的名字,他生活在9世纪。
赞杜的一本书"Al-Kitab al-Mukhtasar fi Hisab al-Jabr wal-Muqabala"(关于恢复和平方根的摘要书)对代数学的发展起到了重要作用。
因此,"algebra" 这个词的词根"al-" 实际上是来源于穆罕默德·本·穆萨·昂瓦尔·赞杜的名字"Al-Khwarizmi"。
这个词根表明"algebra" 最初是指阿拉伯数学家所发展的代数学体系。
代数学是数学的一个分支,涉及数字、符号、变量和数学运算,用于解决未知数的方程和问题。
"Algebra" 一词在数学领域广泛使用,用于描述代数学的研究领域和相关的数学概念。
此外,它还被广泛用于描述和命名与代数学有关的数学课程和教材。
Basic concepts of ternary Hopf algebras
a rX iv:mat h /3628v1[mat h.QA ]12J un23BASIC CONCEPTS OF TERNARY HOPF ALGEBRAS ANDRZEJ BOROWIEC,WIESŁAW A.DUDEK,AND STEVEN DUPLIJ A BSTRACT .The theory of ternary semigroups,groups and algebras is reformulated in the abstract arrow language.Then using the reversing arrow ansatz we define ternary comultiplication,bialgebras and Hopf algebras and investigate their properties.The main property ”to be binary derived”is considered in detail.The co-analog of Post theorem is formulated.It is shown that there exist 3types of ternary coassociativity,3types of ternary counits and 2types of ternary antipodes.Some examples are also presented.Ternary and n -ary generalizations of algebraic structures is the most natural way for further development and deeper understanding of their fundamental properties.Firstly ternary algebraic operations were introduced already in the XIX-th century by A.Cayley.As the development of Cayley’s ideas it were considered n -ary generalization of matrices and their determinants [29,15]and general theory of n -ary algebras [19,4]and ternary rings [20](for physical applications in Nambu mechanics,supersymmetry,Yang-Baxter equation,etc.see [18,31]as surveys).The notion of an n -ary group was introduced in 1928by W.D¨o rnte [7](inspired by E.N¨o ther)which is a natural generalization of the notion of a group and a ternary group considered by Certaine [5]and Kasner [16].For many applications of n -ary groups and quasigroups see [25,32]and [3]respectively.From another side,Hopf algebras [1,30]and their generalizations [23,22,13,21]play a basic role in the quantum group theory (see e.g.[6,17,27]).In the first part of this paper we reformulate necessary material on ternary semigroups,groups and algebras [3,25]in the abstract arrow language.Then according to the general scheme [1]using systematic reversing order of arrows,we define ternary bialgebras and Hopf algebras,investigate their properties and present examples.T ERNARY SEMIGROUPS A non-empty set G with one ternary operation []:G ×G ×G →G is called a ternary groupoid and is denoted by (G,[])or G,m (3) .We will present some results using second notation,because it allows to reverse arrows in the most clear way.In proofswe will mostly use the first notation due to convenience and for short.If on G there is a binary operation ⊙(or m (2))such that [xyz ]=(x ⊙y )⊙zor(1)m (3)=m (3)der =m (2)◦ m (2)×id for all x,y,z ∈G ,then we say that []or m (3)der is derived from ⊙or m (2)and denote thisfact by (G,[])=der (G,⊙).If[xyz ]=((x ⊙y )⊙z )⊙b2ANDRZEJ BOROWIEC,WIESŁAW A.DUDEK,AND STEVEN DUPLIJholds for all x,y,z ∈G and some fixed b ∈G ,then a groupoid (G,[]is b -derived from (G,⊙).In this case we write (G,[])=der b (G,⊙)(cf.[9,10]).We say that (G,[]is a ternary semigroup if the operation []is associative ,i.e.if(2)[[xyz ]uv ]=[x [yzu ]v ]=[xy [zuv ]]holds for all x,y,z,u,v ∈G ,or (3)m (3)◦ m (3)×id ×id =m (3)◦ id ×m (3)×id =m (3)◦ id ×id ×m(3) Obviously,a ternary operation m (3)der derived from a binary associative operation m (2)is also associative in the above sense,but a ternary groupoid (G,[])b -derived (b is a cansellative element)from a semigroup (G,⊙)is a ternary semigroup if and only if b lies in the center of (G,⊙).Fixing in a ternary operation m (3)one element a we obtain a binary operation m (2)a .A binary groupoid (G,⊙)or G,m (2)a ,where x ⊙y =[xay ]or(4)m (2)a =m (3)◦(id ×a ×id)for some fixed a ∈G is called a retract of (G,[])and is denoted by ret a (G,[]).In some special cases described in [9,10]we have (G,⊙)=ret a (der b (G,⊙))or (G,⊙)=der c (ret d (G,[])).Lemma 1.If in the ternary semigroup (G,[])or G,m (3) there exists an element e suchthat for all y ∈G we have [eye ]=y ,then this semigroup is derived from the binary semigroup G,m (2)e,where (5)m (2)e =m(3)◦(id ×e ×id)In this case (G,[])=der (ret e (G,[]).Proof.Indeed,if we put x ⊛y =[xey ],then (x ⊛y )⊛z =[[xey ]ez ]=[x [eye ]z ]=[xyz ]and x ⊛(y ⊛z )=[xe [yez ]]=[x [eye ]z ]=[xyz ],which completes the proof.The same ternary semigroup G,m (3) can be derived from two different semigroups(G,⊛)or G,m (2)e and (G,⋄)or G,m (2)a .Indeed,if in G there exists a =e such that[aya ]=y for all y ∈G ,then by the same argumentation we obtain [xyz ]=x ⋄y ⋄z for x ⋄y =[xay ].In this case for ϕ(x )=x ⋄e =[xae ]we havex ⊛y =[xey ]=[x [aea ]y ]=[[xae ]ay ]=(x ⋄e )⋄y =ϕ(x )⋄yandϕ(x ⊛y )=[[xey ]ae ]=[[x [aea ]y ]ae ]=[[xae ]a [yae ]]=ϕ(x )⋄ϕ(y ).Thus ϕis a binary homomorphism such that ϕ(e )=a .Moreover for ψ(x )=[eax ]we haveψ(ϕ(x ))=[ea [xae ]]=[e [axa ]e ]=x,ϕ(ψ(x ))=[[eax ]ae ]=[e [axa ]e ]=xandψ(x ⋄y )=[ea [xay ]]=[ea [x [eae ]y ]]=[[eax ]e [aey ]]=ψ(x )⊛ψ(y ).Hence semigroups (G,⊛)and (G,⋄)are isomorphic.BASIC CONCEPTS OF TERNARY HOPF ALGEBRAS3 Definition2.An element e∈G is called a middle identity or a middle neutral element of (G,[])if for all x∈G we have[exe]=x or(6)m(3)◦(e×id×e)=id.An element e∈G satisfying the identity[eex]=x or(7)m(3)◦(e×e×id)=id.is called a left identity or a left neutral element of(G,[]).By the symmetry we define a right identity.An element which is a left,middle and right identity is called a ternary identity(briefly:identity).There are ternary semigroups without left(middle,right)neutral elements,but there are also ternary semigroups in which all elements are identities[25,24].Example.In ternary semigroups derived from the symmetric group S3all elements of order 2are left and right(but no middle)identities.Example.In ternary semigroup derived from Boolean group all elements are ternary identi-ties,but ternary semigroup1-derived from the additive group Z4has no left(right,middle) identities.Lemma3.For any ternary semigroup(G,[])with a left(right)identity there exists a binary semigroup(G,⊙)and its endomorphismµsuch that[xyz]=x⊙µ(y)⊙zfor all x,y,z∈G.Proof.Let e be a left identity of(G,[]).It is not difficult to see that the operation x⊙y= [xey]is associative.Moreover,forµ(x)=[exe],we haveµ(x)⊙µ(y)=[[exe]e[eye]]=[[exe][eey]e]=[e[xey]e]=µ(x⊙y)and[xyz]=[x[eey][eez]]=[[xe[eye]]ez]=x⊙µ(y)⊙z.The case of right identity the proof is analogous. Definition4.We say that a ternary groupoid(G,[])is:a left cancellative if[abx]=[aby]=⇒x=y,a middle cancellative if[axb]=[ayb]=⇒x=y,a right cancellative if[xab]=[yab]=⇒x=yholds for all a,b∈G.A ternary groupoid which is left,middle and right cancellative is called cancellative. Theorem5.A ternary groupoid is cancellative if and only if it is a middle cancellative,or equivalently,if and only if it is a left and right cancellative.Proof.Assume that a ternary semigroup(G,[])is a middle cancellative and[xab]=[yab]. Then[ab[xab]]=[ab[yab]]and in the consequence[a[bxa]b]=[a[bya]b]which implies x=y.Conversely if(G,[])is a left and right cancellative and[axb]=[ayb]then[a[axb]b]= [a[ayb]b]and[[aax]bb]=[[aay]bb]which gives x=y.The above theorem is a consequence of the general result proved in[12].4ANDRZEJ BOROWIEC,WIESŁAW A.DUDEK,AND STEVEN DUPLIJDefinition6.A ternary groupoid(G,[])is semicommutative if[xyz]=[zyx]for all x,y,z∈G.If the value of[xyz]is independent on the permutation of elements x,y,z, viz.(8)[x1x2x3]= xσ(1)xσ(2)xσ(3)or m(3)=m(3)◦σ,then(G,[])is a commutative ternary groupoid.Ifσisfixed,then a ternary groupoid satisfying(8)is calledσ-commutative.The group S3is generated by two transpositions;(12)and(23).This means that(G,[]) is commutative if and only if[xyz]=[yxz]=[xzy]holds for all x,y,z∈G.As a simple consequence of Theorem5from[11]we obtainCorollary7.If in a ternary semigroup(G,[])satisfying the identity[xyz]=[yxz]there are a,b such that[axb]=x for all x∈G,then(G,[])is commutative.Proof.According to the above remark it is sufficient to prove that[xyz]=[xzy].We have [xyz]=[a[xyz]b]=[ax[yzb]]=[ax[zyb]]=[a[xzy]b]=[xzy].Mediality in the binary case(x⊙y)⊙(z⊙u)=(x⊙z)⊙(y⊙u)can be presentedas a matrix⇓⇓⇒x y⇒z uand for groups coincides with commutativity.Definition8.A ternary groupoid(G,[])is medial if it satisfies the identity [[x11x12x13][x21x22x23][x31x32x33]]=[[x11x21x31][x12x22x32][x13x23x33]]or(9)m(3)◦ m(3)×m(3)×m(3) =m(3)◦ m(3)×m(3)×m(3) ◦σmedial, whereσmedial= 123456789147258369 ∈S9.It is not difficult to see that a semicommutative ternary semigroup is medial.An element x such that[xxx]=x is called an idempotent.A groupoid in which all elements are idempotents is called an idempotent groupoid.A left(right,middle)identity is an idempotent.T ERNARY GROUPS AND ALGEBRASDefinition9.A ternary semigroup(G,[])is a ternary group if for all a,b,c∈G there are x,y,z∈G such that[xab]=[ayb]=[abz]=c.One can prove[24]that elements x,y,z are uniquely determined.Moreover,according to the suggestion of[24]one can prove(cf.[8])that in the above definition,under the assumption of the associativity,it suffices only to postulate the existence of a solution of [ayb]=c,or equivalently,of[xab]=[abz]=c.In a ternary group the equation[xxz]=x has a unique solution which is denoted by z=·)◦D(3)=id,where D(3)(x)=(x,x,x)is a ternary diagonal map.As a consequence of results obtained in[7]we haveBASIC CONCEPTS OF TERNARY HOPF ALGEBRAS5 Theorem10.In any ternary group(G,[])for all x,y,z∈G the following relations take place[xx x x]=[x]=[y x y]=[[xyz]=[yx=x for all x,an idempotent ternary group is semicommutative.From results obtained in[8](see also[11])for n=3we obtain Theorem11.A ternary semigroup(G,[])with a unary operation−:x→x]=[x·×id)◦ D(2)×id =Pr2,m(3)◦(id×id×x]=yor[a is its identity.x−1(in(G,⊛)is[x axa]is an automorphism of(G,⊛).The easy calculation proves that the above formula holds for b=[a6ANDRZEJ BOROWIEC,WIESŁAW A.DUDEK,AND STEVEN DUPLIJ One can prove that the group(G,⊛)is unique up to isomorphism.From the proof of Theorem3in[14]it follows that any medial ternary group satisfies the identityx z],which together with our previous results shows that in such groups we have[xyz].But x=x.Hence,any medial ternary group is semicommutative.Thus any retract of such group is a commutative group.Moreover,forϕfrom the proof of the above theorem we haveϕ(ϕ(x))=[axa]a]=[a a]]=xCorollary15.Any medial ternary group(G,[])has the form[xyz]=x⊙ϕ(y)⊙z⊙b,where(G,⊙)is a commutative group,ϕits automorphism such thatϕ2=id and b∈G is fixed.Corollary16.A ternary group is medial if and only if it is semicommutative. Corollary17.A ternary group is semicommutative(medial)if and only if[xay]=[yax] holds for all x,y∈G and somefixed a∈G.Corollary18.A commutative ternary group is b-derived from some commutative group.Indeed,ϕ(x)=[a]=x.Theorem19(Post).For any ternary group(G,[])there exists a binary group(G∗,⊛) and H⊳G∗,such that G∗ H≃Z2and[xyz]=x⊛y⊛zfor all x,y,z∈G.Proof.Let c be afixed element in G and let G∗=G×Z2.In G∗we define binary operation⊛putting(x,0)⊛(y,0)=([xyc,1)is its neutral element. The inverse element(in G∗)has the form:(x,0)−1=(c c],1)Thus G∗is a group such that H={(x,1):x∈G}⊳G∗.Obviously the set G can be identified with G×{0}and[xyz]=((x,0)⊛(y,0))⊛(z,0)=([xyc]cz],0)=([xy[BASIC CONCEPTS OF TERNARY HOPF ALGEBRAS7Definition21.Autodistributivity in a ternary group is[[xyz]ab]=[[xab][yab][zab]].Let us consider ternary algebras.Take2ternary operations{,,}and[,,],then distributivity is{[xyz]ab}=[{xab}{yab}{zab}],and additivity is[{x+z}ab]=[xab]+[zab].Definition22.Ternary algebra is a pair A,m(3) ,where A is a linear space and m(3)is a linear mapm(3):A⊗A⊗A→Acalled ternary multiplication which is associativem(3)◦ m(3)⊗id⊗id =m(3)◦ id⊗m(3)⊗id =m(3)◦ id⊗id⊗m(3) .T ERNARY COALGEBRASLet C is a linear space over afield K.Definition23.Ternary comultiplication∆(3)is a linear map over afixedfield K∆(3):C→C⊗C⊗C.For convenience we also use the short-cut Sweedler-type notations[30](11)∆(3)(a)=ni=1a′i⊗a′′i⊗a′′′i=a(1)⊗a(2)⊗a(3).Now we discuss various properties of∆(3)which are in sense(dual)analog of the above ternary multiplication m(3).First consider different possible types of ternary coassociativity.(1)Standard ternary coassociativity(12)(∆(3)⊗id⊗id)◦∆(3)=(id⊗∆(3)⊗id)◦∆(3)=(id⊗id⊗∆(3))◦∆(3),In the Sweedler notationsa(1) (1)⊗ a(1) (2)⊗ a(1) (3)⊗a(2)⊗a(3)=a(1)⊗ a(2) (1)⊗ a(2) (2)⊗ a(2) (3)⊗a(3) =a(1)⊗a(2)⊗ a(3) (1)⊗ a(3) (2)⊗ a(3) (3)≡a(1)⊗a(2)⊗⊗a(3)⊗a(4)⊗a(5).(2)Nonstandard ternaryΣ-coassociativity(Gluskin-type—positional operatives)(∆(3)⊗id⊗id)◦∆(3)=(id⊗ σ◦∆(3) ⊗id)◦∆(3),whereσ◦∆(3)(a)=∆(3)σ(a)=a(σ(1))⊗a(σ(2))⊗a(σ(3))andσ∈Σ⊂S3.(3)Permutational ternary coassociativity(∆(3)⊗id⊗id)◦∆(3)=π◦(id⊗∆(3)⊗id)◦∆(3),whereπ∈Π⊂S5.8ANDRZEJ BOROWIEC,WIESŁAW A.DUDEK,AND STEVEN DUPLIJ Ternary comediality is∆(3)⊗∆(3)⊗∆(3) ◦∆(3)=σmedial◦ ∆(3)⊗∆(3)⊗∆(3) ◦∆(3),whereσmedial is defined in(9).Ternary counit is defined as a mapε(3):C→K.In general,ε(3)=ε(2)satisfying one of the conditions below.If∆(3)is derived,then maybeε(3)=ε(2),but another counits may exist.Example.Define[xyz]=(x+y+z)|mod2for x,y,z∈Z2.It is seen that here there are 2ternary counitsε(3)=0,1.There are3types of ternary counits:(1)Standard(strong)ternary counit(13)(ε(3)⊗ε(3)⊗id)◦∆(3)=(ε(3)⊗id⊗ε(3))◦∆(3)=(id⊗ε(3)⊗ε(3))◦∆(3)=id,(2)Two sequensional(polyadic)counitsε(3)1andε(3)2(14)(ε(3)1⊗ε(3)2⊗id)◦∆=(ε(3)1⊗id⊗ε(3)2)◦∆=(id⊗ε(3)1⊗ε(3)2)◦∆=id,(3)Four long ternary counitsε(3)1–ε(3)4satisfying(15) id⊗ε(3)3⊗ε(3)4 ◦∆(3)◦ (id⊗ε(3)1⊗ε(3)2)◦∆(3) =idBy analogy with(8)σ-cocommutativity is defined asσ◦∆(3)=∆(3).Definition24.Ternary coalgebra is a pair C,∆(3) ,where C is a linear space and∆(3) is a ternary comultiplication which is coassociative in one of the above senses.We will consider below onlyfirst standard type of associativity(12).Let A,m(3) is a ternary algebra and C,∆(3) is a ternary coalgebra and f,g,h∈Hom K(C,A).Definition25.Ternary convolution product is=m(3)◦(f⊗g⊗h)◦∆(3)(16)[f,g,h]∗(a)= f a(1) g a(2) h a(3) .or[f,g,h]∗Definition26.Ternary coalgebra is called derived,if there exists a binary(usual,see e.g. [1,30])coalgebra∆(2):C→C⊗C such that(cf.1))= id⊗∆(2) ⊗∆(2).(17)∆(3)derThe derived ternary and n-ary coalgebras were considered e.g.in[26]and[2]respec-tively.T ERNARY H OPF ALGEBRASDefinition27.Ternary bialgebra B is triple B,m(3),∆(3) for which B,m(3) is a ternary algebra and B,∆(3) is a ternary coalgebra and(18)∆(3)◦m(3)=m(3)◦∆(3)One can distinguish four kinds of ternary bialgebrs with respect to a”being derived”property”:BASIC CONCEPTS OF TERNARY HOPF ALGEBRAS9 (1)∆-derived ternary bialgebra∆(3)=∆(3)der= id⊗∆(2) ◦∆(2)(2)m-derived ternary bialgebram(3)der =m(3)der=m(2)◦ m(2)⊗id(3)Derived ternary bialgebra is simultaneously m-derived and∆-derived ternary bial-gebra.(4)Full ternary bialgebra is not derived.Now we define possible types of ternary antipodes using analogy with binary coalge-bras.Definition28.Skew ternary antipod ism(3)◦(S(3)skew ⊗id⊗id)◦∆(3)=m(3)◦(id⊗S(3)skew⊗id)◦∆(3)=m(3)◦(id⊗id⊗S(3)skew)◦∆(3)=idor in terms of the ternary convolution product(16)S(3)skew,id,id∗= id,S(3)skew,id ∗= id,id,S(3)skew ∗=id.Definition29.Strong ternary antipod ism(2)⊗id ◦(id⊗S(3)strong⊗id)◦∆(3)=1⊗id,id⊗m(2) ◦(id⊗id⊗S(3)strong)◦∆(3)=id⊗1,where1is a unit of algebra.Definition30.Ternary coalgebra is derived,if∆(3)is derived.Lemma31.If in a ternary coalgebra C,∆(3) there exists a linear mapε(3):C→K satisfying(19) ε(3)⊗id⊗ε(3) ◦∆(3)=id,then∃∆(2)such that∆(3)=∆(3)der= id⊗∆(2) ⊗∆(2)Definition32.If in ternary coalgebra∆(3)◦S=τ13◦(S⊗S⊗S)◦∆(3),whereτ13= 123321 ,then it is called skew-involutive.Definition33.Ternary Hopf algebra is a ternary bialgebra with a ternary antipod of the corresponding type,i.e. H,m(3),e(3),∆(3),S(3) .REMARK.There are8types of associative ternary Hopf algebras and4types of medial Hopf algebras.Also it can happen that there are several ternary units e(3)i and several ternary counitsε(3)i(see(13)–(15)),which makes number of possible ternary Hopf algebras enormous.10ANDRZEJ BOROWIEC,WIESŁAW A.DUDEK,AND STEVEN DUPLIJTheorem 34.For any a ternary Hopf algebra there exists a binary Hopf algebra,auto-morphism φand a linear map λ,such that (20)∆(3)=(id ⊗φ⊗id)◦ ∆(2)⊗idProof.The binary coproduct is ∆(2)=(id ⊗λ⊗id)◦∆(3)and ∆(3)=(id ⊗id ⊗id ⊗λ)◦ ∆(2)⊗∆(2) ◦∆(2).The co-analog of the Post Theorem 19is Theorem 35.For any ternary Hopf algebra H,∆(3) there exists a binary Hopf algebra H ∗,∆(2) and ∆(3)=∆(3)der |H ,such that H H ∗≃k (Z 2)and (21)(id ⊗id ⊗id)◦∆(3)= id ⊗∆(2) ◦∆(2).E XAMPLESExample.Ternary dual pair k (G )(push-forward)and F (G )(pull-back)which are related by k ∗(G )∼=F (G ).Here k (G )=span (G )is a ternary group (G has a ternary product[]G or m (3)G )algebra over a field k .If u ∈k (G )(u =u i x i ,x i ∈G ),then [uvw ]k =u i v j w l [x i x j x l ]G is associative,and so (k (G ),[]k )becomes a ternary algebra.Define aternary coproduct ∆(3)k :k (G )→k (G )⊗k (G )⊗k (G )by ∆(3)k (u )=u i x i ⊗x i ⊗x i (derive and associative),then ∆(3)k ([uvw ]k )= ∆(3)k (u )∆(3)k (v )∆(3)k (w ) k ,and k (G )is a ternary bialgebra.If we define a ternary antipod by S (3)k =u i ¯x i ,where ¯x i is askew element of x i ,then k (G )becomes a ternary Hopf algebra.In the dual case offunctions F (G ):{ϕ:G →k }a ternary product []F or m (3)F (derive and associative)acts on ψ(x,y,z )as m (3)F ψ (x )=ψ(x,x,x ),and so F (G )is a ternary algebra.Let F (G )⊗F (G )⊗F (G )∼=F (G ×G ×G ),then we define a ternary coproduct ∆(3)F :F (G )→F (G )⊗F (G )⊗F (G )as ∆(3)F ϕ (x,y,z )=ϕ([xyz ]F ),which is derive and associative.Thus we can obtain ∆(3)F ([ϕ1ϕ2ϕ3]F )= ∆(3)F (ϕ1)∆(3)F (ϕ2)∆(3)F (ϕ3) F,and therefore F (G )is a ternary bialgebra.If we define a ternary antipod byS (3)F (ϕ)=ϕ(¯x ),where ¯x is a skew element of x ,then F (G )becomes a ternary Hopf algebra.Example.Matrix representation.Possible non-derived matrix representations of the ternary product can be done only by four-rank tensors:twicely covariant and twicely contravariant and allow only 2possibilities A oi jk B jl oo C ko il and A ij ok B ol io C ko il (where o is any index).Acknowledgments .One of the authors (S.D.)would like to thank Jerzy Lukierski for kind hospitality at the University of Wrocław,where this work was initiated and begun.R EFERENCES[1]E.Abe,Hopf Algebras ,Cambridge Univ.Press,Cambridge,1980.[2]A.Ballesteros and O.Ragnisco,A systematic construction of completely integrable Hamiltonians fromcoalgebras ,J.Phys.A31(1998),3791–3813.[3]V .D.Belousov,n -ary Quasigroups ,Shtintsa,Kishinev,1972.[4]R.Carlsson,Cohomology of associative triple systems ,Proc.Amer.Math.Soc.60(1976),1–7.[5]J.Certaine,The ternary operation (abc )=ab −1c of a group ,Bull.Amer.Math.Soc.49(1943),869–877.[6]E.E.Demidov,Quantum Groups ,Factorial,Moscow,1998.BASIC CONCEPTS OF TERNARY HOPF ALGEBRAS11[7]W.D¨o rnte,Unterschungen¨u ber einen verallgemeinerten Gruppenbegriff,Math.Z.29(1929),1–19.[8]W.A.Dudek,K.Głazek,and B.Gleichgewicht,A note on the axioms of n-groups,in Coll.Math.Soc.J.Bolyai.29.Universal Algebra,Esztergom(Hungary),1977,pp.195–202.[9]W.A.Dudek and J.Michalski,On a generalization of Hossz´u theorem,Demonstratio Math.15(1982),437–441.[10]———,On retract of polyadic groups,Demonstratio Math.17(1984),281–301.[11]W.A.Dudek,Remarks on n-groups,Demonstratio Math.13(1980),165–181.[12]———,Autodistributive n-groups,Annales Sci.Math.Polonae,Commentationes Math.23(1993),1–11.[13]S.Duplij and F.Li,On regular solutions of quantum Yang-Baxter equation and weak Hopf algebras,Journalof Kharkov National University,ser.Nuclei,Particles and Fields521(2001),15–30.[14]K.Głazek and B.Gleichgewicht,Abelian n-groups,in Coll.Math.Soc.J.Bolyai.29.Universal Algebra,Esztergom(Hungary),1977,pp.321–329.[15]M.Kapranov,I.M.Gelfand,and A.Zelevinskii,Discriminants,Resultants and Multidimensional Determi-nants,Birkh¨a user,Berlin,1994.[16]E.Kasner,An extension of the group concept,Bull.Amer.Math.Soc.10(1904),290–291.[17]C.Kassel,Quantum Groups,Springer-Verlag,New York,1995.[18]R.Kerner,Ternary algebraic structures and their applications in physics,Univ.P.&M.Curie preprint,Paris,2000.[19]wrence,Algebras and triangle relations,in Topological Methods in Field Theory,(J.Mickelson andO.Pekonetti,eds.),World Sci.,Singapore,1992,pp.429–447.[20]W.G.Lister,Ternary rings,Trans.Amer.Math.Soc.154(1971),37–55.[21]F.Li and S.Duplij,Weak Hopf algebras and singular solutions of quantum Yang-Baxter equation,Commun.Math.Phys.225(2002),191–217.[22]D.Nikshych and L.Vainerman,Finite quantum groupoids and their applications,Univ.California preprint,math.QA/0006057,Los Angeles,2000.[23]F.Nill,Axioms for weak bialgebras,Inst.Theor.Phys.FU preprint,math.QA/9805104,Berlin,1998.[24]E.L.Post,Polyadic groups,Trans.Amer.Math.Soc.48(1940),208–350.[25]S.A.Rusakov,Some Applications of n-ary Group Theory,Belaruskaya navuka,Minsk,1998.[26]A.E.Santana and R.Muradian,Hopf structures in Nambu-Lie n-algebras,Theor.Math.Phys.114(1998),67–72.[27]S.Shnider and S.Sternberg,Quantum Groups,International Press,Boston,1993.[28]E.I.Sokolov,On the theorem of Gluskin-Hossz´u on D¨o rnte groups,Mat.Issled.39(1976),187–189.[29]N.P.Sokolov,Introduction to the Theory of Multidimensional Matrices,Naukova Dumka,Kiev,1972.[30]M.E.Sweedler,Hopf Algebras,Benjamin,New York,1969.[31]L.Vainerman and R.Kerner,On special classes of n-algebras,J.Math.Phys.37(1996),2553–2565.[32]G.ˇCupona,N.Celakoski,S.Markovski,and D.Dimovski,Vector valued groupoids,semigroups and groups,in Vector Valued Semigroups and Groups,(B.Popov,G.ˇCupona,and N.Celakoski,eds.),Macedonian Acad.Sci.,Skopje,1988,pp.1–79.I NSTITUTE OF T HEORETICAL P HYSICS,U NIVERSITY OF W ROCŁAW,P L.M AXA B ORNA9,50-204 W ROCŁAW,P OLANDE-mail address:borow@ift.univ.wroc.plI NSTITUTE OF M ATHEMATICS,T ECHNICAL U NIVERSITY OF W ROCŁAW,W YBRZEZE W YSPIANSKIEGO 27,50-370W ROCŁAW,P OLANDE-mail address:dudek@im.pwr.wroc.plD EPARTMENT OF P HYSICS AND T ECHNOLOGY,K HARKOV N ATIONAL U NIVERSITY,K HARKOV61001, U KRAINEE-mail address:Steven.A.Duplij@univer.kharkov.uaURL:http://www.math.uni-mannheim.de/˜duplij。
ON TWISTED TENSOR PRODUCTS OF ALGEBRAS
The Erwin Schrodinger International Institute for Mathematical Physics
Pasteurgasse 6/7 A-1090 Wien, Austria
On Twisted Tensor Products of Algebras
Andreas Cap Hermann Schichl Jir Vanzura
2. Twisted tensor products
Throughout this paper we x some commutative ring K with unit. Later on when we will study deformations we will specialize to K = R or C . We assume all algebras to be unital and all homomorphisms to preserve units. 2.1. De nition. Let A and B be algebras over K . A twisted tensor product of A and B is an algebra C together with two injective algebra homomorphisms iA : A ! C and iB : B ! C such that the canonical linear map (iA ; iB ): A K B ! C de ned by (iA ; iB )(a b) := iA(a) iB (b) is a linear isomorphism. An isomorphism of twisted tensor products is an isomorphism of algebras which respects the inclusions of A and B. 2.2. There is a simple way to construct candidates for twisted tensor products as follows: Let : B A ! A B be a K {linear mapping, such that (b 1) = 1 b and (1 a) = a 1. Then on A B de ne a multiplication by := ( A B). We write A B for idA idB . This is also justi ed by B ) (A the fact that this is the functor A B applied to the map . Next de ne iA : A ! A B by iA (a) := a 1 and likewise iB : B ! A B. These are algebra homomorphisms by the conditions on . Obviously, if the multiplication is associative, then (A B; ) is a twisted tensor product of A and B. Now the associativity of the multiplication can be characterized in terms of as follows: 2.3. Proposition/De nition. Suppose that (b 1) = 1 b and (1 a) = a 1. Then the multiplication is associative if and only if we have: ( B
素特征域上Witt代数及极大子代数的2-局部导子
浙江大学学报(理学版)Journal of Zhejiang University (Science Edition )http :///sci第 48 卷第 2 期2021年3月Vol. 48 No. 2Mar. 2021DOI : 10.3785/j.issn.1008-9497.2021.02.006素特征域上Witt 代数及极大子代数的2-局部导子姚裕丰,王惠(上海海事大学文理学院:上海201306)摘要:李代数的导子代数对李代数结构的研究有重要作用。
特征零的代数闭域上有限维半单李代数的导子都是内导子,该类李代数同构于其导子代数。
作为导子的自然推广,李代数的2-局部导子对李代数局部性质的研究,具有重要作用,研究了素特征域上李代数的2-局部导子。
设F 是特征p >3的代数闭域,g 是域F 上p _维Witt 代 数,g 0是g 的极天子代数,讨论了 g 和g 0的2-局部导子的性质,证明了 g 和g 0的所有2-局部导子均为导子。
关键词:Witt 代数;导子;2-局部导子中图分类号:O 151.26文献标志码:A 文章编号:10()8-9497(2()21)02-174-()6YAO Yufeng, WANG Hui ( College of A rts and Sciences , Shanghai Maritime University Shanghai 201306, China)2-local derivations of the Witt algebra and its maximal subalgebra over a field of prime characteristic . Journal ofZhejiang University (Science Edition), 2021,48(2):174-179Abstract : The derivation algebra of a Lie algebra plays an important role to study of the structure of the Lie algebra. Allderivations of finite dimensional semisimple Lie algebras over an algebraically closed field are inner. So the Lie algebrasof this kind are isomorphic to their derivation algebras. As a natural generalization of derivation , 2-local derivation of aLie algebra plays an important role in study of local properties of the Lie algebra.This paper is devoted to study 2-localderivations of Lie algebras over fields of prime characteristic. Let g be the p dimensional Witt algebra over analgebraically closed field of characteristic p > 3, g ()be its maximal subalgebra. We investigate the properties of 2-localderivations on g and g 0,and show that all 2-local derivations on g and g 0 are derivations.Key Words : Witt algebra ; derivation ; 2-local derivation代数的导子指该代数上满足Leibniz 法则的线 性变换。
斯普林格数学研究生教材丛书
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一些代数同态群的结构
代数 H4 ꎬA 是交换代数ꎬ则 Alg( H4 ꎬA) 是交换群ꎬ且
Alg( H4 ꎬA) 中的元素除单位元外阶均为 2ꎮ
类似 于 定 理 1 的 证 明 方 法ꎬ 当 H 为 量 子 群
A) 的结构ꎬ从而可以刻画代数同态群 Alg( HꎬA) 的
是群同构ꎬ 其中 f( K) = aꎬf( K -1 ) = a -1 ꎬf( E) =
则有 f( x ) = f ( x) = a = 0ꎮ又有 f( gx) = f( qxg)
从 H 的结构可知 H 是交换群ꎬ且 H 中元素的阶
到 A 的代数同态ꎬ设 f( x) = aꎬ根据 H n2 的代数结构ꎬ
为深入的研究并取得了相应的成果
[1 -4]
ꎮ然而并不是
所有代数系统的单位群的结构都是容易研究的ꎬ如卷
积代数 Hom(CꎬA)(其中 C 为余代数ꎬA 为代数) 的单
位群 的 研 究 具 有 一 定 的 难 度ꎮ 近 些 年ꎬ 卷 积 代 数
Hom(CꎬA) 的研究也较为广泛ꎬ尤其当余代数 C 和代
数 A 具有特殊结构时ꎬ性质较多
若 H 为 Pointed Hopf 代数ꎬ则存在
Hopf 理想 Iꎬ使得 H = I kG( H) ꎬ其中 G( H) 为 H
的群样元之集ꎮ
引理2 [11] 设 H 为 Pointed Hopf 代数ꎬA 为交换
代数ꎬI 为 H 的 Hopf 理想且满足 H = I kG( H) ꎬ令
U q ( f m ( K) ) 下的卷积代数 Hom( HꎬA) 的代数同态
因此只需确定生成元在代数同态 f 下的象ꎬ令 f( g)
有限维幂零 Hom-李代数的分类
有限维幂零 Hom-李代数的分类陈雪;韩伟【摘要】首先研究了幂零和可解 Hom-李代数的一些性质,将经典有限维李代数的可解和幂零的一些结果推广到 Hom-李代数上,其次分类了四维和五维幂零Hom-李代数,根据 Hom-李代数的半中心的维数,可以将四维和五维幂零Hom-李代数分为3种和4种不同类型。
%Some properties on nilpotent and solvable Hom-Lie algebras are presented in this paper.The results on solvability and nilpotency of classical finite dimensional Lie algebras are generalized to Hom-Lie algebras.Furthermore,four dimensional and five dimensional nilpotent Hom-Lie algebras are classified. By the dimension of the half center of Hom-Lie algebras,four dimensional and five dimensional nilpotent Hom-Lie algebras can be divided into three and four different classes.【期刊名称】《西北师范大学学报(自然科学版)》【年(卷),期】2016(052)006【总页数】7页(P6-12)【关键词】Hom-李代数;幂零性;分类【作者】陈雪;韩伟【作者单位】厦门理工学院应用数学学院,福建厦门 361024;上海交通大学数学科学学院,上海 200240【正文语种】中文【中图分类】O152.52006年,Hartwig等为了构造Witt 和 Virasoro代数的形变,引入了Hom-李代数的结构[1].一个Hom-李代数就是一个三元对(g,[·,·],α),其中α是g上的线性映射,反对称双线性运算[·,·]满足α-扭不变的Jacobi等式,称为Hom-Jacobi等式.当α是恒等映射时,Hom-Jacobi等式退化为一般的Jacobi等式,此时g就是一个李代数.由于Hom-李代数在离散和形变向量场、微积分、Yang-Baxter方程等方面有很多应用,因此最近关于Hom-李代数的研究越来越深入[2-7].Yau研究了Hom-李代数的包络代数的构造及其性质[7].Jin等研究了半单李代数上的Hom-李代数结构,他们指出有限维单李代数没有任何非平凡的Hom-李代数结构,并且给出了有限维半单李代数具有非平凡Hom-李代数结构的充要条件[8].后来Benayadi等[2]又构造了具有对称不变非退化双线性型的Hom-李代数.Hom-李代数表示部分的研究也有了很大进展,Sheng[3]研究了Hom-李代数的伴随和平凡表示.本文的目的是研究幂零Hom-李代数.主要结构如下:第1部分列出了一些关于Hom-李代数的基本定义;第2部分给出幂零和可解Hom-李代数的一些性质;第3部分分类了四维幂零Hom-李代数;第4部分分类了部分五维幂零Hom-李代数.本文如非特别说明,所有代数都是有限维的,并且定义在特征为零的代数闭域C上. 定义1[1-9] Hom-李代数是一个三元对(g,[·,·],α),由线性空间g,双线性映射[·,·]:g×g→g,及线性映射α:g→g组成,满足下列条件:(1)[x,y]=-[y,x] (反对称性),(2)对所有x,y,z∈g,有Hom-Jacobi等式,在上述定义中,若α是代数同态,即,对任意x,y∈g,有α([x,y])=[α(x),α(y)],则称(g,[·,·],α)为保积Hom-李代数.定义2 设(g,[·,·],α)是一个Hom-李代数,η是g的一个子空间,若α(η)⊆η, [η,η]⊆η,则称(η,[·,·],α)为Hom-李子代数.特别地,若[η,g]⊆η,则Hom-李子代数(η,[·,·],α)称为(g,[·,·],α)的理想.若对任意x,y∈g,有[x,y]=0,则称(g,[·,·],α)为交换Hom-李代数.定义3 设,∀y∈g},称C(g)是Hom-李代数(g,[·,·],α)的中心.命题1 设(g,[·,·],α)是一个保积Hom-李代数,则(Ker(α),[·,·],α)是一个理想.证明显然对任意x∈Ker(α),有α(x)=0∈Ker(α).由于对任意x∈Ker(α),y∈g,有α([x,y])=[α(x),α(y)]=[0,α(y)]=0,得到[x,y]∈Ker(α),因此(Ker(α),[·,·],α)是(g,[·,·],α)的一个理想. 】定义4[8] 设(g1,[·,·],α)和(g2,[·,·],β)是两个Hom-李代数,设φ:g1→g2是一个线性映射,如果对任意x,y∈g1,有则称φ是一个Hom-李代数同态.特别地,当φ是一个双射时,Hom-李代数(g1,[·,·]1,α)和(g2,[·,·]2,β)同构.定义5 设(g,[·,·],α)是一个Hom-李代数,如果(g,[·,·],α)没有非平凡理想并且[g,g]=g,则称(g,[·,·],α)为单Hom-李代数.如果(g,[·,·],α)可以分解为一些单理想的直和,则称(g,[·,·],α)为半单Hom-李代数.定义6 设(g,[·,·],α)是一个Hom-李代数,η是g的一个子空间,若[η,η]⊆η,则称η为(g,[·,·],α)的一个半子代数.特别地,若[η,g]⊆η,则η称为(g,[·,·],α)的半理想.定义7 设,∀y∈g},称Z(g)为Hom-李代数(g,[·,·],α)的半中心.显然C(g)⊆Z(g),那么何时C(g)=Z(g)成立呢?下面的命题给出了答案.命题2 设(g,[·,·],α)是一个Hom-李代数,给出C(g)=Z(g)成立的充分条件,(1)对任意x,y∈g,α([x,y])=[α(x),y];(2)[g,g]=g;(3)α是(g,[·,·],α)的一个自同构;(4)α是(g,[·,·],α)的一个自同态,并且g=Z(g)+Im(α).证明显然由(1)可以推出C(g)=Z(g)成立.(2)对任意x∈Z(g),y∈g,存在u,v∈Z(g)使得[u,v]=y,则[α(x),y]=[α(x),[u,v]]=-[α(u),[v,x]]-[α(v),[x,u]]=0,因此x∈C(g).(3)对任意x∈Z(g),y∈g,由于[α(x),y]=α([x,α-1(y)])=0,于是有x∈C(g).(4)对任意x∈Z(g),y∈g,存在u∈g,v∈Z(g),使得y=α(u)+v,则[α(x),y]=[α(x),α(u)+v]=α([x,u])=0,因此x∈C(g). 】定义8 设(g,[·,·],α)是一个Hom-李代数,定义导出列:g(0)=g,g(1)=[g,g],g(2)=[g(1),g(1)],…,g(i)=[g(i-1),g(i-1)].如果存在g(n)=0,则称Hom-李代数(g,[·,·],α)是可解的.定义降中心列:g0=g,g1=[g,g],g2=[g,g1],…,gj=[g,gi-1].如果存在gn=0,则称Hom-李代数(g,[·,·],α)是幂零的.显然幂零Hom-李代数是可解的,而且导出列和降中心列的各项以及Z(g)都是半理想.对Hom-李代数(g,[·,·],α),由于可解性和幂零性都是用运算[·,·]定义的,没有用到线性映射α,那么我们能够很自然地将有限维李代数的可解和幂零的一些结果推广到Hom-李代数上.命题3 设(g,[·,·],α)是一个Hom-李代数,(1)如果(g,[·,·],α)是可解的,则g的所有半子代数和同态像也是可解的.(2)如果η是g的一个可解的半理想并且g/η可解,则g也是可解的.(3)如果η1和η2是g的一个可解的半理想,则η1+η2也是可解的.命题4 设(g,[·,·],α)是一个Hom-李代数,(1)如果(g,[·,·],α)是幂零的,则g的所有半子代数和同态像也是幂零的.(2)如果g/Z(g)是幂零的,则g也是幂零的.(3)如果g是幂零的且非零,则Z(g)≠0.本部分我们总是假设(g,[·,·],α)是四维幂零Hom-李代数,则根据命题4(3)知道Z(g)≠0.因此根据dim(Z(g)),四维幂零Hom-李代数至多可以分为3类:(Ⅰ)dim(Z(g))=4(或3);(Ⅱ)dim(Z(g))=2;(Ⅲ)dim(Z(g))=1.定理1 设dim(Z(g))=4(或3),则四维幂零Hom-李代数(g,[·,·],α)是交换的.设(g1,[·,·],α)和(g2,[·,·],β)是2个四维幂零Hom-李代数且dim(Z(g1))=dim(Z(g2))=4(或3),设A(或B)是α(或β)在g1(或g2)的任意一组基下对应的矩阵,则2个四维幂零Hom-李代数(g1,[·,·],α)和(g2,[·,·],β)同构当且仅当A和B是相似矩阵.证明显然由假设条件可以得到结论. 】定理2 设dim(Z(g))=2.(1)对四维幂零Hom-李代数(g,[·,·],α),可以选择一组基{x1,x2,x3,x4},使得方括号运算满足[x3,x4]=x1,其余为零.(2)设g=Cx1⊕Cx2⊕Cx3⊕Cx4是一个复数域上的向量空间,定义方括号运算:[x3,x4]=x1,其余为零,则对g上的任意线性映射α,(g,[·,·],α)是四维幂零Hom-李代数.(3)由向量空间g,(2)中方括号运算和g上的线性映射α1和α2定义的四维幂零Hom-李代数(g,[·,·],α1)和(g,[·,·],α2)同构当且仅当存在φ∈Ψ,使得φ∘α1=α2∘φ,其中Ψ={φ是g上的可逆线性映射:证明 (1)当dim(Z(g))=2,显然可以得到dim([g,g])=1,并且[g,g]⊆Z(g).因此可以选择两个非零向量x1∈[g,g],x2∈Z(g)使得{x1,x2}线性无关,然后将{x1,x}扩充为g的一组基{x1,x2,x3,x4}使得方括号运算为[x3,x4]=x1,其余为零.(2)对g上的任意线性映射α,显然Hom-Jacobi等式成立,因此(g,[·,·],α)是Hom-李代数,由方括号运算,显然g2=0,所以(g,[·,·],α)是幂零的.(3)由(2),对g上的任意线性映射α1和α2,(g,[·,·],α1)和(g,[·,·],α2)都是四维幂零Hom-李代数.设φ是g上的可逆线性映射,容易验证对任意x,y∈g,φ([x,y])=[φ(x),φ(y)],当且仅当其中.因此φ是(g,[·,·],α1)到(g,[·,·],α2)的同构当且仅当φ∈Ψ并且φ∘α1=α2∘φ. 】定理3 设dim(Z(g))=1.(1)则dim([g,g])=2,可以选择四维幂零Hom-李代数(g,[·,·],α)的一组基{x1∈Z(g),x2,x3,x4},使得方括号运算满足[x2,x3]=x1,[x3,x4]=x2,其余为零.(2)设g=Cx1⊕Cx2⊕Cx3⊕Cx4是复数域上的向量空间,定义方括号运算:[x2,x3]=x1,[x3,x4]=x2,其余为零.则对任意α∈Φ,(g,[·,·],α)是一个四维幂零Hom-李代数,其中Φ={α是g上的线性映射:*表示任意复数}.(3)由向量空间g,(2)中方括号运算以及g上的线性映射α1和α2(α1,α2∈Φ)定义的四维幂零Hom-李代数(g,[·,·],α1)和(g,[·,·],α2)同构,当且仅当存在φ∈Γ,使得φ∘α1=α2∘φ,其中Γ={φ是g上的可逆线性映射:证明 (1)当dim(Z(g))=1,显然dim([g,g])≤3,如果dim([g,g])=3,则g不是幂零的,与已知条件矛盾.如果dim([g,g])=1,则由g的幂零性可以推出[g,g]=Z(g).因此可以选择非零向量x1∈Z(g)并将{x1}扩充为g的一组基{x1,y1,y2,y3}.设[y1,y2]=k2x1,[y2,y3]=k2x1, [y3,y1]=k3x1,其,假设k1≠0,则.另外显然x1与线性无关,这与dim(Z(g))=1矛盾.如果dim([g,g])=2,则根据g的幂零性,显然有Z(g)⊂[g,g].因此可以选择[g,g]的一组基{x1∈Z(g),x2}并将其扩充为g的一组基{x1,x2,x3,x4}.设其中,并且d≠0.假设a≠0,用替换x2,x3,x4,并且仍然用x2,x3,x4的记号,则方括号运算简化为[x2,x3]=x1, [x3,x4]=x2,其余为零.(2)设α是g上的一个线性映射,显然α只需要对x1,x3,x4和x2,x3,x4满足Hom-Jacobi等式即可,即由方括号运算,上面的算式可以化简为因此则α满足Hom-Jacobi等式当且仅当α∈Φ,所以推出(g,[·,·],α)是Hom-李代数,另外g3=0,故g是幂零的.(3) 由(2),对线性映射α1,α2∈Φ,(g,[·,·],α1)和(g,[·,·],α2)都是四维幂零Hom-李代数.设φ是g上的可逆线性映射,容易验证对任意x,y∈g,φ([x,y])=[φ(x),φ(y)]当且仅当其中a11a22≠0.因此φ是(g,[·,·],α1)到(g,[·,·],α2)的同构,当且仅当φ∈Γ并且φ∘α1=α2∘φ. 】本部分假设(g,[·,·],α)是一个五维幂零Hom-李代数,则根据命题4(3),知道Z(g)≠0.因此根据dim(Z(g)),五维幂零Hom-李代数至多可以分为4类:(Ⅰ)dim(Z(g))=5(或4);(Ⅱ)dim(Z(g))=3;(Ⅲ)dim(Z(g))=2,(Ⅳ)dim(Z(g))=1.定理4 设dim(Z(g))=5(或4),则五维幂零Hom-李代数(g,[·,·],α)是交换的.设(g1,[·,·]1,α)和(g2,[·,·]2,β)是2个五维幂零Hom-李代数,且dim(Z(g1))=dim(Z(g2))=5(或4),设A(或B)是α(或β)在g1(或g2)的任意一组基下对应的矩阵,则2个五维幂零Hom-李代数(g1,[·,·]1,α)和(g2,[·,·]2,β)同构,当且仅当A和B是相似矩阵.证明显然由假设条件可以得到结论. 】定理5 设dim(Z(g))=3.(1)对五维幂零Hom-李代数(g,[·,·],α),可以选择一组基{x1∈[g,g],x2,x3,x4,x5},使得方括号运算满足[x4,x5]=x1,其余为零.(2)设g=Cx1⊕Cx2⊕Cx3⊕Cx4⊕Cx5是一个复数域上的向量空间,定义方括号运算:[x4,x5]=x1,其余为零,则对g上的任意线性映射α,(g,[·,·],α)是五维幂零Hom-李代数.(3)由向量空间g,(2)中方括号运算和g上的线性映射α1和α2定义的五维幂零Hom-李代数(g,[·,·],α1)和(g,[·,·],α2)同构当且仅当存在φ∈Π,使得φ∘α1=α2∘φ,其中Π={φ是g上的可逆线性映射:证明 (1)当dim(Z(g))=3,显然可以得到dim([g,g])=1并且[g,g]⊆Z(g).因此可以选择2个非零向量x1∈[g,g],x2,x3∈Z(g)使得{x1,x2,x3}线性无关,然后将{x1,x2,x3}扩充为g的一组基{x1,x2,x3,x4,x5}使得方括号运算为[x4,x5]=x1,其余为零.(2)对g上的任意线性映射α,显然Hom-Jacobi等式成立,因此(g,[·,·],α)是Hom-李代数,由方括号运算,显然g2=0,所以(g,[·,·],α)是幂零的.(3)由(2),对g上的任意线性映射α1和α2,(g,[·,·],α1)和(g,[·,·],α2)都是五维幂零Hom-李代数.设φ是g上的可逆线性映射,容易验证对任意x,y∈g,φ([x,y])=[φ(x),φ(y)],当且仅当其中.因此φ是(g,[·,·],α1)到(g,[·,·],α2)的同构当且仅当φ∈Π并且φ∘α1=α2∘φ. 】定理6 设dim(Z(g))=2.(1)五维幂零Hom-李代数按方括号运算的形式可分为互不同构的3类:设{{x1,x2}∈Z(g),x3,x4,x5}是一组基(a)[x3,x4]=x1,[x3,x5]=x2,其余为零;(b)[x3,x4]=x1,[x4,x5]=x3,其余为零;(c)[x3,x4]=x1,[x3,x5]=x2,[x4,x5]=x3,其余为零.(2)设g=Cx1⊕Cx2⊕Cx3⊕Cx4⊕Cx5是复数域上的向量空间,定义上述(a),(b)或(c)型方括号运算.则对任意线性映射α(α∈T1或α∈T2),(g,[·,·],α)是一个五维幂零Hom-李代数,其中*表示任意复数}.*表示任意复数}.(3)由向量空间g,(2)中(a),(b)或(c)型方括号运算以及g上的线性映射α1和α2(α1,α2∈T1,或α1,α2∈T2)定义的五维幂零Hom-李代数(g,[·,·],α1)和(g,[·,·],α2)同构当且仅当存在φ∈Π1 (ψ∈Π2或η∈Π3),使得φ∘α1=α2∘φ(ψ∘α1=α2∘ψ或η∘α1=α2∘η),其中Π1={φ是g上的可逆线性映射:证明 (1)当dim(Z(g))=2,显然dim([g,g])≤4,如果dim([g,g])=4,则g不是幂零的,与已知条件矛盾.如果dim([g,g])=1,则由g的幂零性可以推出[g,g]⊆Z(g).因此可以选择Z(g)的一组基{x1∈[g,g],x2}并将其扩充为g的一组基{x1,x2,x3,x4,x5}.设[x3,x4]=k1x1,[x4,x5]=k2x1,[x5,x3]=k3x1,其中,假设k1≠0,则.另外显然线性无关,这与dim(Z(g))=2矛盾.如果dim([g,g])=2,则分为2种情况,[g,g]=Z(g)和[g,g]≠Z(g).(Ⅰ)当[g,g]=Z(g)时,可以选择g的一组基{x1,x2,x3,x4,x5}使得方括号运算满足:[x3,x4]=x1, [x3,x5]=x2,其余为零,这就是(a)型;(Ⅱ)当[g,g]≠Z(g),可以选择非零向量x1∈Z(g)∩[g,g],x2∈Z(g),x3∈[g,g]使得{x1,x2,x3}线性无关,再将其扩充为g的一组基{x1,x2,x3,x4,x5}.设其中并且k≠0.不失一般性,假设m≠0,用替换x3,x4,x5,并且仍然记为x3,x4,x5,则方括号运算简化为[x3,x4]=x1,[x4,x5]=x3,其余为零,这就是(b)型.(Ⅲ)如果dim([g,g])=3,则由g的幂零性可以得到Z(g)⊆[g,g].因此可以选择g的一组基{x1∈Z(g),x2∈Z(g),x3∈[g,g],x4,x5}使得方括号运算为[x3,x4]=x1,[x3,x5]=x2, [x4,x5]=x3,其余为零,这就是(c)型.(2)对(a)型,显然Hom-Jacobi等式对g上的任意线性映射α都成立,而且由方括号运算得g3=0,所以(g,[·,·],α)是一个五维幂零Hom-李代数.对(b)型,设α是g上的一个线性映射,则只要证明α对{x1,x4,x5},{x2,x4,x5},{x3,x4,x5}满足Hom-Jacobi等式即可,即由方括号运算,上面的算式可以化简为因此,则α满足Hom-Jacobi等式当且仅当α∈T1,故推出(g,[·,·],α1)是Hom-李代数,由于g3=0,所以g是幂零的.(c)型的证明与(b)型类似,我们在此省略.(3)对(a)型,由(2),对g上的任意线性映射α1和α2,(g,[·,·],α1)和(g,[·,·],α2)都是五维幂零Hom-李代数.设φ是g上的可逆线性映射,容易验证对任意x,y∈g,φ[x,y]=[φ(x),φ(y)]当且仅当其中:因此φ是(g,[·,·],α1)到(g,[·,·],α2)的同构当且仅当φ∈Π1,并且φ∘α1=α2∘φ.类似于(a)型的证明,我们很容易验证(b)型和(c)型,因此(b)型和(c)型的证明省略. 】注:当dim(Z(g))=1时,五维幂零Hom-李代数的分类更加复杂,对这种类型以及更一般的n维幂零Hom-李代数的分类,我们将在以后的论文中给出.E-mail:****************.cn【相关文献】[1] HARTWIG J T,LARSSON D,SILVESTROV S D.Deformations of Lie algebras using-derivations[J].J Algebra,2006,295:314.[2] BENAYADI S, MAKHLOUF A.Hom-Lie algebras with symmetric invariant nondegenerate bilinear forms[J].J of Geometry and Phys,2014,76:38.[3] SHENG Y H. Representations of Hom-Lie algebras[J].Algebra RepresentTheory,2012,15(6):1081.[4] MAKHLOUF A,SILVESTROV S.Notes on formal deformations of Hom-associative and Hom-Lie algebras[J].Forum Math,2010,22(4):715.[5] YAU D.Hom-Yang-Baxter equation,Hom-Lie algebras,and quasi-triangular bialgebras[J].J Phys A:Math Theor,2009,42(16):1076.[6] YAU D.Hom-algebras and homology[J].J Lie Theory,2009,19(2):409.[7] YAU D.Enveloping algebras of Hom-Lie algebras[J].J Gen Lie Theory Appl,2008,2:95.[8] JIN Q Q,LI X C. Hom-Lie algebra structures on semi-simple Lie algebras[J].J Algebra,2008,319(4):1398.[9] MAKHLOUF A,SILVESTROV S. Hom-algebra structures[J].J Gen Lie TheoryAppl,2008,2(2):51.。
算子代数书籍
算子代数书籍全文共四篇示例,供读者参考第一篇示例:算子代数(Book on Operator Algebra)算子代数作为数学领域里一个重要的分支,涉及到代数学、泛函分析、拓扑学等多个学科的交叉领域,是现代数学的一个基础且重要的研究方向。
算子代数的研究内容主要是以算子(线性变换)为基本对象的代数结构,在量子力学、控制理论、信号处理等领域有广泛的应用。
在算子代数的研究中,书籍是学习和研究最重要的工具之一。
下面我们将介绍一些经典且值得读者深入研究的算子代数书籍。
我们推荐David Blackadar的著作《Operator Algebras:Theory of C*-Algebras and von Neumann Algebras》。
这本书是算子代数领域的经典之作,内容涵盖了C*-代数和von Neumann代数的理论及相关应用。
书中以清晰的逻辑结构和详细的数学推导为特点,适合有一定数学基础的读者阅读。
除了以上几本书籍外,还有许多其他优秀的算子代数书籍,如Bruce Blackadar的《K-Theory for Operator Algebras》、John B. Conway的《A Course in Operator Theory》等,都值得读者关注和研究。
第二篇示例:算子代数是一门研究线性算子及其代数性质的数学分支,是数学中一个重要且广泛应用的领域。
算子代数的概念最早可以追溯到20世纪初,随着数学理论的深入探索和发展,算子代数的研究范围不断拓展,应用领域也越来越广泛,成为现代数学中一个不可或缺的领域。
在算子代数的学习和研究中,一本好的教材或参考书籍是必不可少的。
一本优秀的算子代数书籍应该具备清晰的逻辑结构、深入浅出的讲解、充分的实例和习题以及最新的研究成果和发展动态。
今天我们就来推荐一些值得一读的算子代数书籍,希望能够帮助学习者更好地掌握这一领域的知识。
首先推荐的是《Introduction to Operator Algebras》这本书。
Hopf Algebroids
a rXiv:085.386v1[mat h.Q A]25M a y28HOPF ALGEBROIDSGABRIELLA B ¨OHM Contents 1.Introduction 12.R -rings and R -corings 32.1.R -rings 42.2.R -corings 52.3.Duality 63.Bialgebroids 73.1.Right and left bialgebroids 73.2.Examples 103.3.Duality 113.4.Construction of new bialgebroids from known ones 123.5.The monoidal category of modules 153.6.The monoidal category of comodules 173.7.Algebra extensions by bialgebroids.Galois extensions 184.Hopf algebroids 224.1.Examples and constructions 234.2.Basic properties of Hopf algebroids odules of Hopf algebroids 254.4.Integral theory 304.5.Galois theory of Hopf algebroids 334.6.Alternative notions 40Acknowledgement 42References 421.IntroductionIf it should be formulated in one sentence what a Hopf algebroid is,it should be described as a generalisation of a Hopf algebra to a non-commutative base algebra.More precisely,the best known examples of Hopf algebroids are Hopf algebras.Clearly,the notion of a Hopf algebroid turns out to be a successful generalisation only if a convincing amount of results about Hopf algebras extend to Hopf algebroids.But one expects more:working with Hopf algebroids should be considered to be useful if in this way one could solve problems that could not be solved in terms of Hopf algebras.Hopf algebroids provide us with results of both types,ones which extend known results about Hopf algebras and also ones which are conceptually new.Hopf algebras have been intensively studied,and successfully applied in various fields of math-ematics and even physics,for more than fifty years.Without aiming at a complete list,let us mention a few applications.Hopf algebras were used to construct invariants in topology and knot theory.In connection with solutions of the quantum Yang-Baxter equation,quantum groups i.e.certain Hopf algebras play a central role.In (low dimensional)quantum field theory Hopf alge-bras are capable of describing internal symmetry of some models.In non-commutative differential geometry (faithfully flat)Galois extensions by a Hopf algebra are interpreted as non-commutative2GABRIELLA B¨OHMprincipal bundles.Although the theory of Hopf algebras was(is!)extremely successful,in the 1990’s there arose more and more motivations for a generalisation.Originally the term‘Hopf algebroid’was used for cogroupoid objects in the category of com-mutative algebras.These are examples of Hopf algebroids in our current note,with commutative underlying algebra structure.They found an application e.g.in algebraic topology[50].As a tool of a study of the geometry of principalfiber bundles with groupoid symmetry,recently more gen-eral,non-commutative Hopf algebroids have been used,but still over commutative base algebras [51].For some applications it is still not the necessary level of generality.In Poisson geometry, solutions of the dynamical Yang-Baxter equation correspond to dynamical quantum groups,which are not Hopf algebras[31],[53],[46],[74],[30],[42].In topology,invariants obtained in[52]do notfit the Hopf algebraic framework.In transverse geometry extensions of Hopf algebras by non-commutative base algebras occurred[26].In low dimensional quantumfield theories non-integral values of the statistical(also called quantum-)dimensions in some models exclude a Hopf algebra symmetry[12].Anotherfield where important questions could not be answered in the framework of Hopf algebras is non-commutative geometry,i.e.Hopf Galois theory.Thinking about classical Galois extensions offields by afinite group,such an extension can be characterised without explic-itly mentioning the Galois group.A(unique,upto isomorphism)Galois group is determined by a Galoisfield extension.In the case of Hopf Galois extensions no such intrinsic characterisation, without explicit use of a Hopf algebra,is known.Also,although the Hopf algebra describing the symmetry of a given Hopf Galois extension is known to be non-unique,the relation between the possible choices is not known.These questions have been handled by allowing for non-commutative base algebras[4],[40].On the other hand,as the study of Hopf algebroids has a quite short past, there are many aspects of Hopf algebras that have not yet been investigated how to extend to Hopf algebroids.It has to be admitted that almost nothing has been done yet e.g.towards a classification and structure theory of Hopf algebroids.What does it mean that the base algebra R of a Hopf algebroid is non-commutative?Recall that a bialgebra over a commutative base ring k is a k-module,with compatible algebra and coalgebra structures.By analogy,in a bialgebroid the coalgebra structure is replaced by a coring over any not necessarily commutative k-algebra R.Also the algebra structure is replaced by a ring over a non-commutative base algebra.However,in order to formulate the compatibility between the ring and coring structures,the base algebra of the ring has to be not R but R⊗k R op.A Hopf algebra is a bialgebra with an additional antipode map.In the Hopf algebroid case,the antipode relates two different bialgebroid structures,over the base algebras R and R op,respectively.In these notes we arrive at the notion of a Hopf algebroid after considering all constituent structures.In Section2R-rings and R-corings are introduced.They are seen to generalise algebras and coalgebras,respectively.Emphasis is put on their duality.Section3is devoted to a study of bialgebroids,generalising bialgebras.Several equivalent descriptions are given and examples are collected.In particular,constructions of new bialgebroids from known ones are presented.Some of them change the base algebra of a bialgebroid,so they have no counterparts for bialgebras. Although bialgebroid axioms are not manifestly self-dual,duals offinitely generated and projective bialgebroids are shown to be bialgebroids.Key properties of a bialgebroid are monoidality of the categories of modules and comodules.This is explained in some detail.Section3is closed by a most important and most successful application,Galois theory of bialgebroids.Hopf algebroids are the subject of Section4.After presenting the definition,listing some examples and deriving some immediate consequences of the axioms,we discuss the theory of comodules.Since in a Hopf algebroid there are two bialgebroids(hence corings)present,comodules of the Hopf algebroid comprise comodule structures of both.The relation between the categories of comodules of a Hopf algebroid,and comodules of the constituent bialgebroids,is investigated.The category of comodules of a Hopf algebroid is proven to be monoidal,what is essential from the point of view of Galois theory.Next we turn to a study of the theory of integrals.It is a good example of results that are obtained by using some new ideas,but that extend analogous results for Hopf algebras in a reassuring way.The structure of Galois extensions by Hopf algebroids is investigated. Useful theorems are presented about situations when surjectivity of a canonical map implies GaloisHOPF ALGEBROIDS3 property.They extend known results about Hopf Galois extensions.While there seems to be anaccord in the literature that the right generalisation of a bialgebra to a non-commutative base isa bialgebroid,there is some discussion about the right generalisation of a Hopf algebra.We close these notes by collecting and comparing notions suggested by various authors.In order to keep the list of references perspicuous,we do not refer in these notes to papers containing classical results about Hopf algebras,which are generalised hereby.We believe it ismore useful to give here a detailed bibliography of those papers which deal with structures overnon-commutative base.A very good and detailed bibliography of the literature of Hopf algebras can be found e.g.in Chapter“Hopf Algebras”of Handbook of Algebra[24].Notations and conventions.Throughout k is an associative and commutative unital ring. All algebras are associative and unital k-algebras.A k-algebra is denoted by A and the underlying k-module is denoted by A.On elements of A,multiplication is denoted by juxtaposition.Unitelement is denoted by1A.For an algebra A,with multiplication(a,a′)→aa′,A op denotes the opposite of A.As a k-module it is equal to A and multiplication is(a,a′)→a′a.The category ofright(resp.left)modules of an algebra A is denoted by M A(resp.A M).Hom sets are denoted by Hom A(−,−)(resp.A Hom(−,−)).The category of A-bimodules is denoted by A M A and its hom sets by A Hom A(−,−).Often we identify left A-modules with right A op-modules,but in everysuch case it is explicitly said.Action on a(say right)module M of a k-algebra A,if evaluated onelements m∈M and a∈A,is denoted by̺M:m⊗a→m·a.For coproducts in a coalgebra and,more generally,in a coring C,Sweedler’s index notation isused.That is,for an element c∈C,we write c→c(1)⊗c(2)(or sometimes c→c(1)⊗c(2))for the coproduct,where implicit summation is understood.Similarly,for a(say right)coaction on a comodule M of a coring,evaluated on an element m∈M,the notation̺M:m→m[0]⊗m[1] (or m→m[0]⊗m[1])is used,where implicit summation is understood.The category of right (resp.left)comodules of a coring C is denoted by M C(resp.C M).Hom sets are denoted by Hom C(−,−)(resp.C Hom(−,−)).In any category A,the identity morphism at an object A is denoted by the same symbol A.Hom sets in A are denoted by Hom A(−,−).In a monoidal category(M,⊗,U)we allow for non-trivial coherence isomorphisms(−⊗−)⊗−∼=−⊗(−⊗−)and−⊗U∼=−∼=U⊗−,but do not denote them explicitly.(Such monoidal categories are called in the literature sometimes lax monoidal.)The opposite of a monoidal category (M,⊗,U),denoted by(M,⊗,U)op,means the same category M with opposite monoidal product.A functor F between monoidal categories(M,⊗,U)and(M′,⊗′,U′)is said to be monoidal ifthere exist natural transformations F2:F(−)⊗′F(−)→F(−⊗−)and F0:U′→F(U),satisfying usual compatibility conditions.F is said to be op-monoidal if there exist compatible natural transformations F2:F(−⊗−)→F(−)⊗′F(−)and F0:F(U)→U′.A monoidal functor (F,F2,F0)is strong monoidal if F2and F0are isomorphisms,and it is strict monoidal if F2and F0 are identity morphisms.2.R-rings and R-coringsA monoid in a monoidal category(M,⊗,U)is a triple(A,µ,η).Here A is an object and µ:A⊗A→A andη:U→A are morphisms in M,satisfying associativity and unitality conditions(2.1)µ◦(µ⊗A)=µ◦(A⊗µ)andµ◦(η⊗A)=A=µ◦(A⊗η).The morphismµis called a multiplication(or product)andηis called a unit.An algebra over a commutative ring k can be described as a monoid in the monoidal category(M k,⊗k,k)of k-modules.A right module of a monoid(A,µ,η)is a pair(V,ν),where V is an object andν:V⊗A→V is a morphism in M,such thatν◦(V⊗µ)=ν◦(ν⊗A)andν◦(V⊗η)=V.Left modules are defined symmetrically.4GABRIELLA B¨OHMReversing all arrows in the definition of a monoid,we arrive at the dual notion of a comonoid.A comonoid in a monoidal category(M,⊗,U)is a triple(C,∆,ǫ).Here C is an object and ∆:C→C⊗C andǫ:C→U are morphisms in M,satisfying coassociativity and counitality conditions(2.2)(∆⊗C)◦∆=(C⊗∆)◦∆and(ǫ⊗C)◦∆=C=(C⊗ǫ)◦∆.The morphism∆is called a comultiplication(or coproduct)andǫis called a counit.A coalgebra over a commutative ring k can be described as a comonoid in the monoidal category(M k,⊗k,k) of k-modules.Dualising the definition of a module of a monoid,one arrives at the notion of a comodule of a comonoid.Many aspects of the theory of algebras and their modules,or coalgebras and their comodules, can be extended to monoids or comonoids in general monoidal categories.Here we are interested in monoids and comonoids in a monoidal category(R M R,⊗R,R)of bimodules over a k-algebra R.These monoids and comonoids are called R-rings and R-corings,respectively.2.1.R-rings.Generalising algebras over commutative rings,we study monoids in bimodule cat-egories.Definition2.1.For an algebra R over a commutative ring k,an R-ring is a triple(A,µ,η).Here A is an R-bimodule andµ:A⊗R A→A andη:R→A are R-bimodule maps,satisfying the associativity and unit conditions(2.1).A morphism of R-rings f:(A,µ,η)→(A′,µ′,η′)is an R-bimodule map f:A→A′,such that f◦µ=µ′◦(f⊗R f)and f◦η=η′.For an R-ring(A,µ,η),the opposite means the R op-ring(A op,µop,η).Here A op is the same k-module A.It is understood to be a left(resp.right)R op-module via the right(resp.left) R-action.Multiplication isµop(a⊗R op a′):=µ(a′⊗R a)and unit isη.A most handy characterisation of R-rings comes from the following observation.Lemma2.2.There is a bijective correspondence between R-rings(A,µ,η)and k-algebra homomor-phismsη:R→A.Indeed,starting with an R-ring(A,µ,η),a multiplication map A⊗k A→A is obtained by composing the canonical epimorphism A⊗k A→A⊗R A withµ.Conversely,starting with an algebra mapη:R→A,an R-bilinear associative multiplication A⊗R A→A is obtained by using the universality of the coequaliser A⊗k A→A⊗R A.An R-ring(A,µ,η)determines monads on the categories of right and left R-modules(i.e. monoids in the monoidal categories of endofunctors on M R and R M,respectively).They are given by−⊗R A:M R→M R and A⊗R−:R M→R M,respectively.Definition2.3.A right module for an R-ring(A,µ,η)is an algebra for the monad−⊗R A on the category M R.A right module morphism is a morphism of algebras for the monad−⊗R A.A left module for an R-ring(A,µ,η)is an algebra for the monad A⊗R−on the category R M.A left module morphism is a morphism of algebras for the monad A⊗R−.Left modules of an R-ring are canonically identified with right modules for the opposite R op-ring.Analogously to Lemma2.2,modules for R-rings can be characterised as follows.Lemma2.4.A k-module M is a(left or right)module of an R-ring(A,µ,η)if and only if it is a (left or right)module of the corresponding k-algebra A in Lemma2.2.Furthermore,a k-module map f:M→M′is a morphism of(left or right)modules of an R-ring(A,µ,η)if and only if it is a morphism of(left or right)modules of the corresponding k-algebra A in Lemma2.2.The situation when the(left or right)regular R-module extends to a(left or right)module of an R-ring(A,µ,η)is of particular interest.Lemma2.5.The right regular module of a k-algebra R extends to a right module of an R-ring (A,µ,η)if and only if there exists a k-module mapχ:A→R,obeying the following properties.(i)χ(aη(r))=χ(a)r,for a∈A and r∈R(right R-linearity),(ii)χ(aa′)=χ((η◦χ)(a)a′),for a,a′∈A(associativity),HOPF ALGEBROIDS5(iii)χ(1A)=1R(unitality).The mapχobeying these properties is called a right character on the R-ring(A,µ,η).In terms of a right characterχ,a right A-action on R is given by r·a:=χ(η(r)a).Conversely,in terms of a right A-action on R,a right character is constructed asχ(a):=1R·a.Symmetrically, one can define a left character on an R-ring(A,µ,η)via the requirement that the left regular R-module extends to a left module for(A,µ,η).Definition2.6.Let(A,µ,η)be an R-ring possessing a right characterχ:A→R.The invariants of a right module(M,̺M)with respect toχare the elements of the k-submoduleMχ:={m∈M|̺M(m⊗R a)=̺M(m⊗R(η◦χ)(a)),∀a∈A}∼=Hom A(R,M),where the isomorphism Mχ→Hom A(R,M)is given by m→(r→m·η(r)).In particular,the invariants of R are the elements of the subalgebraB:=Rχ={b∈R|χ(η(b)a)=bχ(a),∀a∈A}.Associated to a characterχ,there is a canonical map(2.3)A→B End(R),a→ r→χ(η(r)a)).The R-ring(A,µ,η)is said to be a Galois R-ring(with respect to the characterχ)provided that the canonical map(2.3)is bijective.2.2.R-corings.The theory of R-corings is dual to that of R-rings.A detailed study can be found in the monograph[20].Definition2.7.For an algebra R over a commutative ring k,an R-coring is a triple(C,∆,ǫ). Here C is an R-bimodule and∆:C→C⊗R C andǫ:C→R are R-bimodule maps,satisfying the coassociativity and counit conditions(2.2).A morphism of R-corings f:(C,∆,ǫ)→(C′,∆′,ǫ′)is an R-bimodule map f:C→C′,such that∆′◦f=(f⊗R f)◦∆andǫ′◦f=ǫ.For an R-coring(C,∆,ǫ),the co-opposite means the R op-coring(C cop,∆cop,ǫ).Here C cop is the same k-module C.It is understood to be a left(resp.right)R op-module via the right(resp.left) ultiplication is∆cop(c):=c(2)⊗R op c(1)and counit isǫ.An R-coring(C,∆,ǫ)determines comonads on the categories of right and left R-modules(i.e. comonoids in the monoidal categories of endofunctors on M R and R M,respectively).They are given by−⊗R C:M R→M R and C⊗R−:R M→R M,respectively.Definition2.8.A right comodule for an R-coring(C,∆,ǫ)is a coalgebra for the comonad−⊗R C on the category M R.That is,a pair(M,̺M),where M is a right R-module and̺M:M→M⊗R C is a right R-module map satisfying the coassociativity and counit conditions(2.4)(̺M⊗R C)◦̺M=(M⊗R∆)◦̺M and(M⊗Rǫ)◦̺M=M.A right comodule morphism f:(M,̺M)→(M′,̺M′)is a morphism of coalgebras for the comonad −⊗R C.That is,a right R-module map f:M→M′,satisfying̺M′◦f=(f⊗R C)◦̺M. Symmetrically,a left comodule is a coalgebra for the comonad C⊗R−on the category R M.A left comodule morphism is a morphism of coalgebras for the comonad C⊗R−.Left comodules of an R-coring are canonically identified with right comodules for the co-opposite R op-coring.The situation when the(left or right)regular R-module extends to a(left or right)comodule of an R-coring(C,∆,ǫ)is of particular interest,see[16,Lemma5.1].Lemma2.9.The(left or right)regular R-module extends to a(left or right)comodule of an R-coring(C,∆,ǫ)if and only if there exists an element g∈C,obeying the following properties.(i)∆(g)=g⊗R g.(ii)ǫ(g)=1R.The element g obeying these properties is called a grouplike element in the R-coring(C,∆,ǫ).6GABRIELLA B¨OHMHaving a grouplike element g in an R-coring(C,∆,ǫ),a right coaction on R is constructed as a map R→C,r→g·r.Conversely,a right coaction̺R:R→C determines a grouplike element ̺R(1R).Definition2.10.Let(C,∆,ǫ)be an R-coring possessing a grouplike element g∈C.The coin-variants of a right comodule(M,̺M)with respect to g are the elements of the k-submoduleM g:={m∈M|̺M(m)=m⊗Rg}∼=Hom C(R,M),where the isomorphism M g→Hom C(R,M)is given by m→(r→m·r).In particular,the coinvariants of R are the elements of the subalgebraB:=R g={b∈R|b·g=g·b}.Associated to a grouplike element g,there is a canonical map(2.5)R⊗B R→C,r⊗Br′→r·g·r′.The R-coring(C,∆,ǫ)is said to be a Galois R-coring(with respect to the grouplike element g) provided that the canonical map(2.5)is bijective.Let(C,∆,ǫ)be an R-coring possessing a grouplike element g.Put B:=R g.For any right C-comodule M,M g is a right B-module.Furthermore,any right C-comodule map M→M′restricts to a right B-module map M g→M′g.There is an adjoint pair of functors(2.6)−⊗BR:M B→M C and(−)g:M C→M B.If(C,∆,ǫ)is a Galois coring(with respect to g),then M C is equivalent to the category of de-scent data for the extension B⊆R.Hence the situation,when the functors(2.6)establish an equivalence,is interesting from the descent theory point of view.2.3.Duality.Beyond the formal duality between algebras and coalgebras,it is well known that the k-dual of a coalgebra over a commutative ring k possesses a canonical algebra structure.The converse is true whenever a k-algebra isfinitely generated and projective as a k-module.In what follows we recall analogues of these facts for rings and corings over an arbitrary algebra R. Proposition2.11.Let R be an algebra over a commutative ring k.(1)For an R-coring(C,∆,ǫ),the left dual∗C:=R Hom(C,R)possesses a canonical R-ringstructure.Multiplication is given by(φψ)(c):=ψ c(1)·φ(c(2)) ,forφ,ψ∈∗C and c∈C.Unit map is R→∗C,r→ǫ(−)r.(2)For an R-ring(A,µ,η),which is afinitely generated and projective right R-module,theright dual A∗:=Hom R(A,R)possesses a canonical R-coring structure.In terms of a dual basis({a i∈A},{αi∈A∗}),comultiplication is given byξ→ iξ(a i−)⊗Rαi,which is independent of the choice of a dual basis.Counit is A∗→R,ξ→ξ(1A).(3)For an R-coring(C,∆,ǫ),which is afinitely generated and projective left R-module,thesecond dual(∗C)∗is isomorphic to C as an R-coring.(4)For an R-ring(A,µ,η),which is afinitely generated and projective right R-module,thesecond dual∗(A∗)is isomorphic to A as an R-ring.Applying Proposition2.11to the co-opposite coring and the opposite ring,analogous correspon-dences are found between right duals of corings and left duals of rings.Proposition2.12.Let C be a coring over an algebra R.(1)Any right C-comodule(M,̺M)possesses a right module structure for the R-ring∗C,(2.7)m·φ:=m[0]·φ(m[1]),for m∈M,φ∈∗C.Any right C-comodule map becomes a∗C-module map.That is,there is a faithful functor M C→M∗C.(2)The functor M C→M∗C is an equivalence if and only if C is afinitely generated andprojective left R-module.HOPF ALGEBROIDS7 There is a duality between Galois rings and Galois corings too.Proposition2.13.Let C be an R-coring which is afinitely generated and projective left R-module. For an element g∈C,introduce the mapχg:∗C→R,φ→φ(g).The following statements hold.(1)The element g∈C is grouplike if and only ifχg is a right character on the R-ring∗C.(2)An element b∈R is a coinvariant of the right C-comodule R(with coaction induced by agrouplike element g)if and only if b is an invariant of the right∗C-module R(with respect to the right characterχg).(3)The R-coring C is a Galois coring(with respect to a grouplike element g)if and only ifthe R-ring∗C is a Galois ring(with respect to the right characterχg).3.BialgebroidsIn Section2we generalised algebras and coalgebras over commutative rings to monoids and comonoids in bimodule categories.We could easily do so,the category of bimodules over any k-algebra R is a monoidal category,just as the category of k-modules.If we try to generalise bialgebras to a non-commutative base algebra R,however,we encounter difficulties.Recall that a k-bialgebra consists of an algebra(B,µ,η),and a coalgebra(B,∆,ǫ)defined on the same k-module B.They are subject to compatibility conditions.Unit and multiplication must be coalgebra maps or,equivalently,counit and comultiplication must be algebra maps.This means in particular that, for any elements b and b′in B,multiplication and comultiplication satisfy the condition (3.1)(bb′)(1)⊗k(bb′)(2)=b(1)b′(1)⊗k b(2)b′(2).Note that(3.1)is formulated in terms of the symmetry tw in M k.For any k-modules M and N, the twist map tw M,N:M⊗k N→N⊗k M maps m⊗k n to n⊗k m.Precisely,(3.1)is equivalent to∆◦µ=(µ⊗k µ)◦(B⊗ktw B,B⊗k B)◦(∆⊗k∆).In the literature one canfind generalisations when tw is replaced by a braiding[73],[47],[60].(For an approach when tw is replaced by a mixed distributive law,see[48].)However,general bimodule categories are neither symmetric nor braided.There is no natural way to formulate an analogue of(3.1)in a bimodule category.In fact,more sophisticated ideas are needed.The notion which is known today as a(left)bialgebroid,was introduced(independently)by several authors.Thefirst definition is due to Takeuchi,who used the name×R-bialgebra in[71]. Some twenty years later,with motivation coming from Poisson geometry,in[46]Lu proposed an equivalent definition.The term bialgebroid is due to her.A third equivalent set of axioms was invented by Xu in[74].The equivalence of the listed definitions is far from obvious.It was proven by Brzezi´n ski and Militaru in[18].Symmetrical notions of left and right bialgebroids were formulated and studied by Kadison and Szlach´a nyi in[41].The definition presented here is a slightly reformulated version of the one in[46]or[41].3.1.Right and left bialgebroids.In contrast to the definition of a bialgebra,in this sectiona bialgebroid is not described as a compatible monoid and comonoid in some monoidal category (of bimodules).The ring and coring structures of a bialgebroid are defined over different base algebras:they are a monoid and a comonoid in different monoidal categories.Recall from Lemma 2.2that an R⊗k R op-ring A(for some algebra R over a commutative ring k)is described by a k-algebra mapη:R⊗k R op→A.Equivalently,instead ofη,we can consider its restrictions (3.2)s:=η(−⊗k1R):R→A and t:=η(1R⊗k−):R op→A,which are k-algebra maps with commuting ranges in A.The maps s and t in(3.2)are called the source and target maps of an R⊗k R op-ring A,respectively.In what follows,an R⊗k R op-ring will be given by a triple(A,s,t),where A is a k-algebra(with underlying k-module A)and s and t are algebra maps with commuting ranges as in(3.2).8GABRIELLA B¨OHMDefinition3.1.Let R be an algebra over a commutative ring k.A right R-bialgebroid B consists of an R⊗k R op-ring(B,s,t)and an R-coring(B,∆,ǫ)on the same k-module B.They are subject to the following compatibility axioms.(i)The bimodule structure in the R-coring(B,∆,ǫ)is related to the R⊗k R op-ring(B,s,t)via(3.3)r·b·r′:=bs(r′)t(r),for r,r′∈R,b∈B.(ii)Considering B as an R-bimodule as in(3.3),the coproduct∆corestricts to a k-algebra map from B to(3.4)B×R B:={ i b i⊗R b′i| i s(r)b i⊗R b′i= i b i⊗R t(r)b′i,∀r∈R},where B×R B is an algebra via factorwise multiplication.(iii)The counitǫis a right character on the R-ring(B,s).Remarks3.2.The bialgebroid axioms in Definition3.1have some immediate consequences.(1)Note that the k-submodule B×R B of B⊗R B is defined in such a way that factorwisemultiplication is well defined on it.B×R B is called the Takeuchi product.In fact, it has more structure than that of a k-algebra:it is an R⊗k R op-ring with unit map R⊗k R op→B×R B,r⊗k r′→t(r′)⊗R s(r).The(corestriction of the)coproduct is easily checked to be an R⊗k R op-bimodule map B→B×R B.(2)Axiom(iii)is equivalent to the requirement that the counitǫis a right character on theR op-ring(B,t).(3)Yet another equivalent formulation of axiom(iii)is the following.The mapθ:B→End k(R)op,b→ r→ǫ(s(r)b) is a k-algebra map,where End k(R)op is an algebra via opposite composition of endomorphisms.The mapθis called an anchor map in[74].Recall that in a bialgebra over a commutative ring,replacing the algebra with the opposite one, or replacing the coalgebra with the co-opposite one,one arrives at bialgebras again.Analogously, the co-opposite of a right R-bialgebroid B with structure maps denoted as in Definition3.1,is the following right R op-bialgebroid B cop.R op⊗k R-ring structure is(B,t,s),R op-coring structure is (B cop,∆cop,ǫ).However,the R⊗k R op-ring(B op,t,s)and the R-coring(B,∆,ǫ)do not satisfy the same axioms in Definition3.1.Instead,they are subject to a symmetrical version of Definition 3.1.Definition3.3.Let R be an algebra over a commutative ring k.A left R-bialgebroid B consists of an R⊗k R op-ring(B,s,t)and an R-coring(B,∆,ǫ)on the same k-module B.They are subject to the following compatibility axioms.(i)The bimodule structure in the R-coring(B,∆,ǫ)is related to the R⊗k R op-ring(B,s,t)via(3.5)r·b·r′:=s(r)t(r′)b,for r,r′∈R,b∈B.(ii)Considering B as an R-bimodule as in(3.5),the coproduct∆corestricts to a k-algebramap from B to (3.6)B R×B:={ib i⊗R b′i|ib i t(r)⊗Rb′i= i b i⊗R b′i s(r),∀r∈R},where B R×B is an algebra via factorwise multiplication.(iii)The counitǫis a left character on the R-ring(B,s).Since in this note left and right bialgebroids are considered simultaneously,we use two versions of Sweedler’s index notation.In a left bialgebroid we use lower indices to denote components of the coproduct,i.e.we write b→b(1)⊗R b(2).In a right bialgebroid we use upper indices to denote components of the coproduct,i.e.we write b→b(1)⊗R b(2).In both cases implicit summation is understood.。
“巴拿赫空间与算子理论”研究方向部分课程及参考书
“巴拿赫空间与算子理论”研究方向部分课程及参考书一、《线性算子谱理论》参考书:1.P.Aiena. Fredholm and Local Spectral Theory, with Applications to multipliers,20042. H.R.Dowson. Spectral theory of linear operators.19783. T.Kato. Perturbation theory for linear operators.19844.S.R.Caradus, W.E.Pfaffenberger, Bertram Yood. Calkin Algebras and Algebras of Operators on Banach Spaces, 19745. 童裕孙. 泛函分析教程.复旦大学出版社.2003.6. 孙炯、王忠. 线性算子的谱分析. 北京:科学出版社, 2005.7. 安世全、孙佑民. 线性算子的谱分析. 北京:科学出版社, 1995.8. 邹承祖. 线性算子的谱分解理论. 吉林大学出版社,1987.9. Ion Colojoara and Ciprian Foias著,孙佑民、安世全译. 广义谱算子理论. 北京:科学出版社, 1992.二、《Banach空间理论》参考书:1.俞鑫泰. Banach空间几何理论.上海:华东师范大学出版社,19862.俞鑫泰. Banach空间选论.上海:华东师范大学出版社,19923.J.Lindenstrauss and L.Tzafriri. Classical Banach spaces I, II. 19774.I.Singer. Bases in Banach spaces, I , II. 19805. R.B.Holmes, Geometric Functional Analysis and its Applications,1975三、《空间结构与算子理想》参考书:1.钟怀杰. 巴拿赫空间结构和算子理想.北京:科学出版社, 2005.2.赵俊峰. Banach空间结构理论.武汉:武汉大学出版社,1993.3. A.Pietsch. Operator ideals.1980.4. J.Lindenstrauss and L.Tzafriri. Classical Banach spaces I, II. 19775. I.Singer. Bases in Banach spaces, I , II. 1980四、《Banach代数》、《算子代数》参考书:1.李炳仁. Banach代数.北京:科学出版社,1992.2.李炳仁. 算子代数.北京:科学出版社,19863.R.G. Douglas. Banach algebra techniques in operator theory.1972,1998(第二版)4.S.R.Caradus, W.E.Pfaffenberger and Bertram Yood. Calkin algebras and algebras ofoperators on Banach spaces.1974.5. 定光桂. 巴拿赫空间引论. 北京:科学出版社, 1999.C--Algebras. 2000 . 6. M.Rordam, rsen, ustsen.. An introduction to K-theory for *C--Algebras and operator theory.1990.7.Gerard J.Murphy. *五、《算子半群及其应用》参考书:1.郑权. 强连续线性算子半群. 武汉:华中理工大学出版社,1994.2. A.Pazy. Semigroups of linear operators and applications to partial differentialequations.19833.童裕孙. 泛函分析教程. 复旦大学出版社.2003.4.夏道行、严绍宗、舒五昌、童裕孙. 泛函分析第二教程. 高等教育出版社.1987。
Deformed boson algebras and the quantum double construction
Recently there has been an increasing interest in the deformation of Lie (super)algebras[1, 2, 3, 4, 5, 6] and their quasitriangular Hopf algebra nature[7], mainly because of there wide applications in mathematical physics. Parallel attempts to consistently q -deform the boson algebra also appeared[8, 9, 10, 11, 12, 13, 14, 15, 16] both independently and in connection with quantum group realizations, addressing also their possible Hopf algebra nature[17, 18]. The main aim of this letter is, on the one hand to point out the ambigious validity of an R-matrix obtained from a definition of q -boson algebra endowed with a Hopf algebra structure[17], and on the other to demonstrate the quantum double construction[1, 19, 20] for this algebra which will lead to an unambiguously valid R-matrix. The q -deformed boson algebras, denoted here by L, that have been considered are usually taken to be generated by a, a† and N subject to the following commutation relations: [N, a] = −a, [N, a† ] = a† , together with one out of the following list of additional relations: [a, a† ] = [N + I ]q − [N ]q , aa† − q −1 a† a = q N , aa† − qa† a = q −N , a† a = [N ], and aa† = [N + I ], (2) (3) (4) (5) (1)
三维单李代数sl(2,F)上的Yang-Baxter方程
三维单李代数sl(2,F)上的Yang-Baxter方程高岩【摘要】刻画了特征p≠2的代数闭域上三维单李代数上的Yang-Baxter方程.【期刊名称】《哈尔滨师范大学自然科学学报》【年(卷),期】2013(029)005【总页数】3页(P7-9)【关键词】三维单李代数;Yang-Baxter方程【作者】高岩【作者单位】哈尔滨师范大学【正文语种】中文0 引言Baxter代数由Baxter于1960年提出,源于Glen Baxter概率论中波动理论积分方程[1].Rota在90年代对Baxter算子进行了更深入的研究.[2]近年来,Baxter代数在理论物理和数学物理方面得到了广泛而显著的应用,许多学者刻画了低维代数上的Rota-Baxter算子.例如,文献[3]给出了维数小于等于3时权0的结合代数上的Rota-Baxter算子,文献[4]给出了维数小于等于3时权1的Rota-Baxter算子,而文献[5]对权0的二阶矩阵构成的四维结合代数上的Rota-Baxter算子进行了研究.代数闭域F上权0的Rota-Baxter算子称为Yang-Baxter方程.该文刻画了三维单李代数sl(2,F)上的Yang-Baxter方程.1 基本概念该文规定F为特征p≠2的代数闭域,L是域F上的李代数,用[,]表示李乘.定义1[6]设L是域F上的一个李代数,若R是L×L→L的线性算子,满足则称R是一个权为λ的Rota-Baxter算子,L是一个权为λ的Rota-Baxter代数,当λ=0时称上式为Yang-Baxter方程.令{e1,…,en}是李代数L的一组固定基,设,其中∈F.L上的任意Rota-Baxter算子R都可以写成矩阵(rij)形式,其中rij由唯一确定,易见rij满足如下方程(λ=0):2 Yang-Baxter方程记L=sl(2,F)是域F上的一个三维单李代数,其中L的标准基为:规定基元素间的乘法表:[x,y]=h,[h,x]=2x,[h,y]=-2y.命题1 三维单李代数L上Yang-Baxter方程的解共有9个(任何参数属于代数闭域F,且 a,b≠0):证明由定义可知三维单李代数L上Yang-Baxter方程的解即为权0时的Rota-Baxter算子.根据L的标准基,则L上任意Rota-Baxter算子R能够由矩阵(rij)表示,且 R(x),R(y),R(h)满足(1)式,由 L的基的乘法表可以得到以下9个等式:则上述命题的证明能够分成以下六种情况:则在以下的六个引理中分别考虑这些情况.引理1 当r32=0,r12=0,r23≠0时,L上的Yang-Baxter方程的解由上述命题中的R1与R2给出.证明由(13)推出r22=0,由(11)对r13=0进行分类讨论:(i)当r13=0时,通过计算可得命题1中的R1和R2.(ii)当r13≠0时,通过计算可知此情况下Yang-Baxter方程无解.引理2 当 r32=0,,r12=0,r23=0时,L上的Yang-Baxter方程的解由上述命题中的R3与R4给出.证明由(13)推出r12r21=代入(8)有r22(r11-r22)=r11r33+r22r33(*),由(13)且r12≠0推出2r33+r11=r22推出r11-r22=-2r33代入(*)推出-2r33r22=(r11+r22)r33,则下对r33进行分类讨论:(i)当r33≠0时,通过计算可知此情况下Yang-Baxter方程无解.(ii)当r33=0时,可得命题1中的R3和R4. 引理3 当 r32=0,,r12=0,r23=0时,L上的Yang-Baxter方程的解由上述命题中的R5与R7给出.证明由(13)推出r22=0,由(8)推出r11r33=0,下分类讨论:(i)当r11=0,r33≠0时,计算可得命题1中的R5.(ii)当r11≠0,r33=0,时,由(11)推出r13=0,由(9)推出 r11=0,与r11≠0矛盾,故此种情形不存在.(iii)当r11=r33=0时,可得命题1中的R6与R7.引理4 当r32≠0,r12=0,r23≠0时,L上的Yang-Baxter方程的解由上述命题中的R8给出.证明由(10)推出r32=-2r13,令r13=a≠0,推出r32=-2a≠0,由(11)推出r33=0,由(7)推出r11=-r22=b≠0,代入(6)推出r21=0,由(8)推出,由(9)推出r=31,则可得命题1中R8.引理5 当r32≠0,r12≠0,r23≠0时,L上的Yang-Baxter方程无解.证明由(7)推出r11=-r22=a≠0,由(8)推出r12r21=-a2,推出,由(8)推出r13=0,又由于 r32≠0,故令 r32=1,则由(9)推出,由(10)推出,但这些未知元的值不满足方程(12)和(14),故此时L上的Yang-Baxter方程无解.引理6 当r32≠0,r12=0,r23=0时,L上的Yang-Baxter方程的解由上述命题中的R9给出.证明由(10)推出 r32=-2r13=a≠0,推出,由(7)推出r=-r,由(8)1122推出r11r22=0推出 r11=r22=0,由(11)推出r33=0,由(13)推出 r31=0,由(6)推出r21=0,由(12)推出r31=0,则可得命题1中的R9.参考文献[1] Baxter G.An analytic problem whose solution follows from a simple algebraic identity[J].Pacific J Math,1960,10:731-742.[2] Rota G C.Baxter algebras and combinatorial I[J].Bull AMS,1969,5:325-329.[3] Li X X,Hou D P,Bai C M.Rota-Baxter operators on pre-Lie algebras [J].J Nonlinear Math Phys,2007,14:269-289.[4] Huihui A,Bai C M.From Rota-Baxter algebras to pre-Lie algebras [J].J Phys A:Math Theor,2008,41:015201-015219.[5]孙琼.一类Baxter代数及其应用.黑龙江大学硕士论文,2012:4-11. [6]苏育才,卢才辉,崔一敏.有限维半单李代数简明教程.北京:科学出版社,2008.。
The quantum bialgebra associated with the eight-vertex R-matrix
a r X i v :h e p -t h /9302139v 1 26 F eb 1993The quantum bialgebra associated with the eight-vertex R-matrixD.B.Uglov1Department of Physics,State University of New York at Stony BrookStony Brook,NY 11794-3800,USAFebruary 24,1993AbstractThe quantum bialgebra related to the Baxter’s eight-vertex R-matrix is found as a quantum deformation of the Lie algebra of sl (2)-valued automorphic functions on a complex torus.1.Recent years witnessed an extensive developement of the theory of quantum groups and their quasiclassical limits-Lie bialgebras.Although since the work of Belavin and Drinfel’d[3]it is known,that solutions of the Classical Yang-Baxter equation can be clas-sified into three categories:the rational,the trigonometric and the elliptic ones,the main developement took place in the rational and the trigonometric cases.The underlying alge-braic structures in these cases were found to be the affine Kac-Moody Lie algebras(classical case)and the Yangians and the quantum affine Kac-Moody algebras(quantum case)[5,6]. One of the major developements in the elliptic case was the discovery of the Sklyanin alge-bra[4].This algebra,however,has no coproduct and thus it is not a bialgebra.Another important work had been done by Reyman and Semenov-Tyan-Shanskii[2],who found the Lie bialgebras associated with the elliptic solutions of the Classical Yang-Baxter equation. The simplest example of their alge bras is the Lie algebra of sl(2)-valued automorphic mero-morphic functions on a complex torus.The Lie bialgebra structure of this algebra is given by the classical r-matrix of the Landau-Lifshitz model[2].In the work[7]the generators and the defining relations of this Lie algebra had been found.In the present letter we address the problem of quantization of the above Lie bialgebra.The result is a quantum bialgebra related to the eight-vertex R-matrix.We use the term“quantum bialgebra“to designate a Hopf algebra without the antipode.2.In[7]it is shown,that the Lie algebra of sl(2)-valued automorphic meromorphic functions on a complex torus which we denote by E k,ν±is afinitely generated(infinite-dimensional)C-Lie algebra defined upon the six generators{x±k}k=1,2,3by the relations( i,j,k below is any cyclic permutation of1,2,3):[x±i,[x±j,x±k]]=0,(1)[x±i,[x±i,x±k]]−[x±j,[x±j,x±k]]=J ij x±k,(2)[x+i,x−i]=0,(3)[x±i,x∓j]=√sn(u,k);w2(u)=dnsn(u,k),u∈T.The structure of a Lie bialgebra upon E k,ν±is defined by the classical r-matrix of the Landau-Lifshitz model[2].A certain trigonometric limit k→0of E k,ν±coincides with the loop algebra A(1)′1/(centre)[7].3.To define a quantum deformation of the Lie algebra(1-4)we introduce a deformation parameterη∈C and recall the definition of the Baxter’s eight-vertex R-matrix[1]:R(u)=I⊗I+ 3k=1w k(u+iη)T±ab,a,b∈{1,2}.The defining relations of E k,ν±,ηhave the following form:T±3(H34−H32)T±3+T±2(H23−H21)T±4=0,(5)T±1=1I1,(6)R12(ν∓−ν±)T±1T∓2=T∓2T±1R12(ν∓−ν±).(7) We adopt the standard convention:T±n means a matrix with E k,ν±,η-valued entries,which acts nontrivially only in the n−th factor of C⊗m(m=4in(5),m=2in(7))and coincides there with T±ab.PROPOSITION E k,ν±,ηis a bialgebra,i.e.there exist a coproduct∆:E k,ν±,η→E k,ν±,η⊗E k,ν±,ηand a counitε:E k,ν±,η→C,such,that:∆(ab)=∆(a)∆(b),a,b∈E k,ν±,η(8)(ε⊗id)∆(a)=(id⊗ε)∆(a)=a,a∈E k,ν±,η.(9)Explicit expressions for∆,andεare given by the following formulae:∆(T±ab)=3c=1T±ac⊗T±cb,∆(T±cb⊗T±ab)=δab,ε(1)=1.(11)In the quasiclassical limitη→0,which is described as follows:T±=I+2iη3k=1x±kσk+O(η2),x±kσk+O(η2),(12)one recovers from the defining relations(5-7)the defining relations(1-4)for the generators {x±k}k=1,2,3in E k,ν±.Note,that from(6)it follows thatT±)=1D(u−ν±)R(−u+ν±),(13)D(u)=1−3k=1w k(u+iη)w k(u−iη)2K′,ν−=i12.Reyman,A.G.and Semenov-Tyan-Shanskii,M.A.,Journ.Sov.Math.46,1631(1989).3.Belavin,A.A.and Drinfel’d V.G.,Funct.Anal.Appl.17,220(1984).4.Sklyanin,E.K.,Funct.Anal.Appl.16,263(1983).5.Drinfel’d V.G.,Proceedings of the ICM,Berkeley,CA U.S.A.,798(1986).6.Chari,V.and Pressley,A.,L’Enseignement Math´e matique36,267(1990);Comm.Math. Phys.142,261(1991).7.Uglov,D.B.,to be published.。
General+Double+Quantum+Groups
GENERAL DOUBLE QUANTUM GROUPS
Tianshui Ma and Shuanhong Wang
Department of Mathematics, Southeast University, Nanjing, Jiangsu, China
We introduce the concept of a twisted tensor biproduct, generalizing the general product given in Caenepeel et al. [1]. We give necessary and sufficient conditions for the new object to be a bialgebra and study the case of ∗-bialgebras. We describe all braided structures on the twisted tensor biproduct and introduce the notion of a general double quantum group. As an application, the special cases and examples are given. Key Words: Braided Hopf algebra; Braided monoidal category; General double quantum group; Twisted tensor biproduct. 2000 Mathematics Subject Classification: 16W30.
646
MA AND WANG
In Section 2, we study the twisted tensor biproduct AT R B, where B is a bialgebra and A is only an algebra and a coalgebra connected by a twisted map R B ⊗ A −→ A ⊗ B and a cotwisted map T A ⊗ B −→ B ⊗ A. We find in Theorem 2.1 necessary and sufficient conditions for the new object AT R B to be a bialgebra and study in Theorem 2.3 the case of ∗-bialgebras. In Section 3, we describe in Theorem 3.12 all braided structures on the twisted tensor biproduct AT R B. We study the relations between the existence of braided structures on A and B and the ones on AT R B (see Theorem 3.13). Finally, in Section 4 we conclude by describing its applications and examples. 1. PRELIMINARIES Throughout, k is the fixed field, and is the complex numbers field. Unless otherwise stated, all vector spaces are over k and all maps are k-linear. For vector spaces U and V over k, we drop the subscript k from U ⊗k V and Homk U V and write U ⊗ V and Hom U V instead. The linear map U V U ⊗ V −→ V ⊗ U defined by U V u ⊗ v = v ⊗ u for all u ∈ U and v ∈ V is the flip map. The identity map of U is denoted by iU . Our basic reference on Hopf algebras is Sweedler [15], on braided Hopf algebras Larson and Towber [7] and on braided monoidal category theory Maclane [8]. Let C be a coalgebra with comultiplication C −→ C ⊗ C . We follow the widely used convention of representing c ∈ C ⊗ C for c ∈ C symbolically by c = c1 ⊗ c2 , a notation that originates in the Heyneman–Sweedler notation c = c 1 ⊗ c 2 for the coproduct. In particular, the structure map of a left C -comodule V is denoted by v = v −1 ⊗ v0 for v ∈ V , and the structure map of a right C -comodule U is denoted by u = u0 ⊗ u 1 for u ∈ U . We write C for the category of left comodules over the coalgebra C , and A for the category of left modules over the algebra A. Recall that a ∗-algebra A over has an involution a → a∗ for all a ∈ A. An involution is an antilinear map satisfying a∗∗ = a and ab ∗ = b∗ a∗ for all a b ∈ A. If A B are ∗-algebras then the tensor product algebra A ⊗ B is again a ∗-algebra for the product defined as a ⊗ b a ⊗ b = aa ⊗ bb and the involution given by a ⊗ b ∗ = a∗ ⊗ b∗ for all a a ∈ A and b b ∈ B. Recall that a Hopf ∗-algebra A is a Hopf algebra A over with a coproduct A −→ A ⊗ A, with a counit A −→ and with an antipode S A −→ A so that and are ∗-homomorphisms and S S a ∗ ∗ = a for all a ∈ A, respectively. 1.1. The Twisted Tensor Product of ∗-Algebras Let A and B be algebras with units 1A and 1B , respectively. Suppose that R B ⊗ A −→ A ⊗ B is a linear map. The A#R B is defined to be a vector space A ⊗ B with the product given by mA#R B = mA ⊗ mB iA ⊗ R ⊗ iB or a#R b a #R b = aaR #bR b (1.1)
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∗ The first and fourth authors are supported by grants from the National Science Foundation, and the fourth author is supported by fellowships from the Alfred P. Sloan Foundation and the David and Lucile Packard Foundation.
Baxter Algebras and Hopf Algebras
George E. Andrews Department of Mathematics Pennsylvania State University University Park, PA 16802, USA (andrews@) Li Guo Department of Mathematics and Computer Science Rutgers University at Newark Newark, NJ 07102, USA (liguo@) William Keigher Department of Mathematics and Computer Science Rutgers University at Newark Newark, NJ 07102, USA (keigher@) Ken Ono Department of Mathematics University of Wisconsin Madison, WI 53706, USA (ono@) ∗
Abstract By applying a recent construction of free Baxter algebras, we obtain a new class of Hopf algebras that generalizes the classical divided power Hopf algebra.
2
Preliminaries
Here we recall some basic definitions and facts. All tensor products in this paper are taken over the fixed commutative ring C . Recall that a cocommutative C coalgebra is a triple (A, ∆, ε) where A is a C -module, ∆ : A → A ⊗ A and ε : A → C are C -linear maps that make the following diagrams commute. A ↓∆ A⊗A C ⊗A
1
1
Introduction
Hopf algebras have their origin in Hopf’s seminal works on topological groups in the 1940s, and have become fundamental objects in many areas of mathematics and physics. For example, they are crucial to the study of algebraic groups, Lie groups, Lie algebras, and quantum groups. In turn, these areas have provided many of the most important examples of Hopf algebras. In this paper we construct new examples of Hopf algebras. Our examples arise naturally in a combinatorial study of Baxter algebras. A Baxter algebra [Ba] is an algebra A with an operator P on A that satisfies the identity P (x)P (y) = P (xP (y)) + P (yP (x)) + λP (xy) for all x and y in A where λ, the weight, is a fixed element in the ground ring of the algebra A. Rota [Ro1] began a systematic study of Baxter algebras from an algebraic and combinatorial perspective and suggested that they are related to hypergeometric functions, incidence algebras and symmetric functions [Ro2, Ro3]. Free Baxter algebras were first constructed by Rota [Ro1] and Cartier [Ca] in the category of Baxter algebras with no identities (with some restrictions on the weight and the base ring). Recently, two of the authors [G-K1, G-K2] have constructed free Baxter algebras in a more general context including these classical constructions. Their construction is in terms of mixable shuffle products which generalize the well-known shuffle products of path integrals as developed by Chen [Ch] and Ree [Re]. Here we show that a special case of the construction of these new Baxter algebras provides a large supply of new Hopf algebras. The divided power Hopf algebra is one of the classical examples of a Hopf algebra, and it is not difficult to see that this algebra is the free Baxter algebra of weight zero on the empty set. The new Hopf algebras presented here generalize this classical example. In particular, the Baxter algebra of arbitrary weight on the empty set is a Hopf algebra. Here we describe the construction. Let C be a commutative algebra with def identity 1, and let λ ∈ C . Define the sextuple A = Aλ = (A, µ, η, ∆, ε, S ), where
n n −k
A → A ⊗C A, an →
k =0 i=0
(−λ)k ai ⊗ an−k −i,
(v)
ε = ελ :
(vi)
S = Sλ : A → A, an → (−1)n
n = 0, 1, λ1, n = 1, A → C, an → 0, n≥2
n v =0
n −3 v −3
ε⊗id
−→
∆⊗id
∆
A⊗A ↓ id⊗∆ A⊗A⊗A
id⊗ε
(1)
−→
←− ∼ =տ
A ⊗ A −→ ↑ ∆ ր∼ = A A ց∆
τA,A
A⊗C (2where τA,A : A ⊗ A → A ⊗ A is defined by τA,A (x ⊗ y) = y ⊗ x. The C -algebra C has a natural structure of a C -coalgebra with ∆C : C → C ⊗ C, c → c ⊗ c, c ∈ C and εC = idC : C → C. We also denote the multiplication in C by µC . Recall that a C -bialgebra is a quintuple (A, µ, η, ∆, ε) where (A, µ, η ) is a C -algebra and (A, ∆, ε) is a C -coalgebra such that µ and η are morphisms of coalgebras. In other words, we have the commutativity of the following diagrams. A⊗A (id⊗τ ⊗id)(∆⊗∆) ↓ A⊗A⊗A⊗A 3 −→ A ↓∆ µ⊗µ −→ A ⊗ A
∞
(i) (ii)
A = Aλ =
n=0
Can , is the free C −module on the set {an }n≥0, A ⊗C A → A,
m
µ = µλ :
am ⊗ an →
k =0
λk
m+n−k m
m k
am+n−k ,
(iii) (iv)