Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach

Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach

The Yangian of the strange Lie superalgebras in Drinfel'd realization is defined. The current system generators and defining relations are described.

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Дата:2007
Автор: Stukopin, V.
Формат: Стаття
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Опубліковано: Інститут математики НАН України 2007
Назва видання:Symmetry, Integrability and Geometry: Methods and Applications
Онлайн доступ:http://dspace.nbuv.gov.ua/handle/123456789/147370
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Назва журналу:Digital Library of Periodicals of National Academy of Sciences of Ukraine
Цитувати:Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach / V. Stukopin // Symmetry, Integrability and Geometry: Methods and Applications. — 2007. — Т. 3. — Бібліогр.: 18 назв. — англ.

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spelling irk-123456789-1473702019-02-15T01:25:09Z Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach Stukopin, V. The Yangian of the strange Lie superalgebras in Drinfel'd realization is defined. The current system generators and defining relations are described. 2007 Article Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach / V. Stukopin // Symmetry, Integrability and Geometry: Methods and Applications. — 2007. — Т. 3. — Бібліогр.: 18 назв. — англ. 1815-0659 2000 Mathematics Subject Classification: 17B37 http://dspace.nbuv.gov.ua/handle/123456789/147370 en Symmetry, Integrability and Geometry: Methods and Applications Інститут математики НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
description The Yangian of the strange Lie superalgebras in Drinfel'd realization is defined. The current system generators and defining relations are described.
format Article
author Stukopin, V.
spellingShingle Stukopin, V.
Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach
Symmetry, Integrability and Geometry: Methods and Applications
author_facet Stukopin, V.
author_sort Stukopin, V.
title Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach
title_short Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach
title_full Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach
title_fullStr Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach
title_full_unstemmed Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach
title_sort yangian of the strange lie superalgebra of qn₋₁ type, drinfel'd approach
publisher Інститут математики НАН України
publishDate 2007
url http://dspace.nbuv.gov.ua/handle/123456789/147370
citation_txt Yangian of the Strange Lie Superalgebra of Qn₋₁ Type, Drinfel'd Approach / V. Stukopin // Symmetry, Integrability and Geometry: Methods and Applications. — 2007. — Т. 3. — Бібліогр.: 18 назв. — англ.
series Symmetry, Integrability and Geometry: Methods and Applications
work_keys_str_mv AT stukopinv yangianofthestrangeliesuperalgebraofqn1typedrinfeldapproach
first_indexed 2025-07-11T01:56:13Z
last_indexed 2025-07-11T01:56:13Z
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fulltext Symmetry, Integrability and Geometry: Methods and Applications SIGMA 3 (2007), 069, 12 pages Yangian of the Strange Lie Superalgebra of Qn−1 Type, Drinfel’d Approach? Vladimir STUKOPIN Don State Technical University, 1 Gagarin Square, Rostov-na-Donu, 344010 Russia E-mail: stukopin@math.rsu.ru Received November 01, 2006, in final form May 06, 2007; Published online May 22, 2007 Original article is available at http://www.emis.de/journals/SIGMA/2007/069/ Abstract. The Yangian of the strange Lie superalgebras in Drinfel’d realization is defined. The current system generators and defining relations are described. Key words: Yangian; strange Lie superalgebra; Drinfel’d realization; Hopf structure; twisted current bisuperalgebra 2000 Mathematics Subject Classification: 17B37 1 Introduction In this paper, following Drinfel’d, we define the Yangian of the strange Lie superalgebra of Qn−1 type. Recall that the Yangian of the simple Lie algebra was defined by V. Drinfel’d as a quantization of the polynomial currents Lie bialgebra (with values in this simple Lie algebra) with coalgebra structure defined by rational Yang r-matrix [1, 2, 3, 5]. The Yangian of the reductive Lie algebra can be given the same definition in special cases. The object dual to Yangian (of the general linear Lie algebra gl(n))) was studied before by L. Faddeev and others while working on Quantum Inverse Scatering Method (QISM). We call this definition of Yangian the RFT approach. V. Drinfel’d shows this object to be isomorphic to the Yangin of gl(n). It is the RFT approach that is usual for papers devoted to Yangians and defines the Yangian as the algebra generated by matrix elements of Yangians irreducible representations according to Drinfel’d (see [4] and [6, 7, 8] for Yangians of the Lie superalgebras). More precisely, the Yangian can be viewed as the Hopf algebra generated by matrix elements of a matrix T (u) (so-called transfer matrix) with the commutation defining relations: R(u− v)T1(u)T2(v) = T2(v)T1(u)R(u− v), where T1(u) = T (u) ⊗ E, T2(v) = E ⊗ T (v), E is an identity matrix R(u) is some rational matrix-function (with the values in End (V ⊗ V )). R(u) is called a quantum R-matrix (see [4]). The RFT approach is used in the paper [14] (see also [6, 7, 8]) to define the Yangian of basic Lie superalgebra, while the Drinfel’d’s one is used in papers [10, 11, 13]. We cannot use directly Drinfel’d approach for defining the Yangian of strange Lie superalgebra [16] as this Lie superalgebra does not have nonzero invariant bilinear forms. Hence we cannot define the Lie bisuperalgebra’s structure on the polynomial currents Lie superalgebra with values in the strange Lie superalgebra. M. Nazarov noted that this structure can be defined on the twisted current Lie superalgebra and used the RFT approach to do it (see [15]). In this paper we use Nazarov’s idea to define the Yangian of strange Lie superalgebra according to Drinfel’d. Our definition can be used for further research of the Yangian of strange Lie superalgebra. It is quite convenient to study such problems as exact description of the quantum double of Yangian ?This paper is a contribution to the Vadim Kuznetsov Memorial Issue ‘Integrable Systems and Related Topics’. The full collection is available at http://www.emis.de/journals/SIGMA/kuznetsov.html mailto:stukopin@math.rsu.ru http://www.emis.de/journals/SIGMA/2007/069/ http://www.emis.de/journals/SIGMA/kuznetsov.html 2 V. Stukopin of strange Lie superalgebra and computation of Universal R-matrix of quantum double. Our method can also be extended on the other twisted current Lie algebras and Lie superalgebra quantization description. As a result, we obtain so-called the twisted Yangians without a Hopf (super)algebra structure (in general) but being comodule over some Hopf (super)algebras. Note that the Yangian of the basic Lie superalgebra A(m,n) was defined according to Drin- fel’d in [10] where the Poincaré–Birkgoff–Witt theorem (PBW-theorem) and the theorem on existence of pseudotriangular structure on Yangian (or the theorem on existence of the universal R-matrix) are also proved. Further, in [11, 13] the quantum double of the Yangian of the Lie superalgebra A(m,n) is described, and the multiplicative formulas for the universal R-matrices (for both quantum double of the Yangian and Yangian) are obtained. This paper is the con- sequence of [10, 12] and extension of some of their results on the Yangian of the “strange” Lie superalgebra. Following Drinfel’d, we define the Yangian of the strange Lie superalgebra of Qn−1 type and describe the current system of Yangian generators and defining relations, which is an analogue of the same system from [3]. The problem of the equivalency between our definition and Nazarov’s one is not resolved yet. The problem of constructing of the explicit formulas defining the isomorphism between the above realization (as in [9] in the case of sln) is open and seems very interesting. This will be discussed in further papers. 2 Twisted current bisuperalgebras Let V = V0 ⊕ V1 be a superspace of superdimension (n, n), i.e. V be a Z2-graded vector space, such that dim(V0) = dim(V1) = n. The set of linear operators End (V ) acting in the V be an associative Z2-graded algebra (or superalgebra), End (V ) = (End (V ))0 ⊕ (End (V ))1, if the grading defined by formula: (End (V ))k = {g ∈ End (V ) : gVi ⊂ Vi+k}. Let {e1, . . . , en, en+1, . . . , e2n} be a such base in V that {e1, . . . , en} be a basis in V0, {en+1, . . ., e2n} be a basis in V1. Then we can identify End (V ) with the superalgebra of (2n × 2n)- matrices gl(n, n) (see also [16, 17]). Let us define on the homogeneous components of gl(n, n) the commutator (or supercommutator) by the formula: [A,B] = AB − (−1)deg(A) deg(B)BA, where deg(A) = i for A ∈ gl(n, n)i, i ∈ Z2. Then gl(n, n) turns into the Lie superalgebra. Further, we will numerate the vectors of the base of V by integer numbers ±1, . . . ,±n, i.e. {e1, . . . , en, e−1, . . . , e−n} is a basis in V , {e1, . . . , en} is a basis in V0, {e−1, . . . , e−n} is a basis in V1. Then matrices from gl(n, n) are indexed by numbers: ±1, . . . ,±n, also. Note that gl(n, n)0 = {( A 0 0 B ) : A,B ∈ gl(n) } , gl(n, n)1 = {( 0 C D 0 ) : C,D ∈ gl(n) } . Let A = ( A11 A12 A21 A22 ) , Aij ∈ gl(n). By definition, put: str (A) = tr (A11)− tr (A22). The str (A) is called the supertrace of A. Define superalgebra sl(n, n) by the formula: sl(n, n) = {A ∈ gl(n, n) : str (A) = 0}. Yangian of the Strange Lie Superalgebra of Qn−1 Type, Drinfel’d Approach 3 Let us also denote sl(n, n) by Ã(n − 1, n − 1). The Lie superalgebra Ã(n − 1, n − 1) has 1- dimensional center Z. Then A(n− 1, n− 1) := Ã(n− 1, n− 1)/Z is a simple Lie superalgebra. Let π : Ã(n− 1, n− 1) → A(n− 1, n− 1) be a natural projection. Consider the isomorphism σ′ : Ã(n− 1, n− 1) → Ã(n− 1, n− 1), which is defined on matrix units Ei,j by the formula σ(Ei,j) = E−i,−j . As σ′(Z) = Z, then σ′ induces the involutive automorphism σ : A(n − 1, n − 1) → A(n − 1, n − 1). Let g = A(n − 1, n − 1). As σ2 = 1, then eigenvalues of σ equal ±1. Let ε = −1, j ∈ Z2 = {0, 1}. Let us set gj = Ker (σ − εjE), g = g0 ⊕ g1. We emphasize that g0 = gσ is a set of fixed points of automorphism σ. It is clear that gσ is a Lie subsuperalgebra of Lie superalgebra g. By definition Qn−1 = gσ is a strange Lie superalgebra. Its inverse image in Ã(n− 1, n− 1) we denote by Q̃n−1. We will use the following properties of the Lie superalgebra Qn−1. The root system ∆ of the Lie superalgebra Qn−1 coincides with root system of the Lie algebra An−1 = sl(n), but the non- zero roots of Qn−1 are both even and odd. We will use the following notations: A = (aij)n−1 i,j=1 is a Cartan matrix of sl(n), (αi, αj) = aij for simple roots αi, αj (i, j ∈ {1, . . . , n− 1}). Define the generators of the Lie superalgebra Qn−1 x±i , x̂±i , hi, ki, i = 1, . . . , n − 1 and elements x±i, x̂±i, hi, ki of g1 by formulas hi = π((Ei,i − Ei+1,i+1) + (Ei,i − E−i−1,−i−1)), hi = π((Ei,i − Ei+1,i+1)− (Ei,i − E−i−1,−i−1)), x+ i = π(Ei,i+1 + E−i,−i−1), x+i = π(Ei,i+1 − E−i,−i−1), x−i = π(Ei+1,i + E−i−1,−i), x−i = π(Ei+1,i − E−i−1,−i), ki = π((Ei,−i − Ei+1,−i−1) + (E−i,i − E−i−1,i+1)), ki = π((Ei,−i − Ei+1,−i−1)− (E−i,i − E−i−1,i+1)), x̂+ i = π(Ei,−i−1 + E−i,i+1), x̂+i = π(Ei,−i−1 − E−i,i+1), x̂−i = π(Ei+1,−i + E−i−1,i), x̂−i = π(Ei+1,−i − E−i−1,i). The Lie superalgebra Qn−1 can be defined as superalgebra generated by generators hi, ki, x±i , x̂±i , i ∈ {1, . . . , n− 1}, satisfying the commutation relations of Cartan–Weyl type (see [17]). We will use notations x±αi = x±i , x̂±αi = x̂±i , x±αi = x± i, x̂±αi = x̂±i. There exists a nondegenerate supersymmetric invariant bilinear form (·, ·) on the Lie superalgebra A(n − 1, n − 1) such that (g0, g0) = (g1, g1) = 0 and g0 and g1 nondegenerately paired. We use also root generators xα, x̂α (α ∈ ∆) and elements xα, x̂α ∈ g1 dual (relatively form (·, ·)) to them. Let us extend the automorphism σ to automorphism σ̃ : g((u−1)) → g((u−1)), on Laurent series with values in g by formula: σ̃(x · uj) = σ(x)(−u)j . Consider the following Manin triple (P,P1,P2): (P = g((u−1))σ̃, P1 = g[u]σ̃, P2 = (u−1g[[u−1]])σ̃. Define the bilinear form 〈·, ·〉 on P by the formula: 〈f, g〉 = res (f(u), g(u))du, (1) where res ( n∑ k=−∞ ak · uk ) := a−1, (·, ·) is an invariant bilinear form on g. It is clear that P1, P2 are isotropic subsuperalgebras in relation to the form 〈·, ·〉. It can be shown in the usual way that there are the following decompositions: g[u]σ̃ = ∞⊕ k=0 ( g0 · u2k ⊕ g1 · u2k+1 ) , g((u−1))σ̃ = ⊕ k∈Z ( g0 · u2k ⊕ g1 · u2k+1 ) . (2) 4 V. Stukopin Describe the bisuperalgebra structures on g[u]σ̃. Let {ei} be a basis in g0 and {ei} be a dual basis in g1 in relation to the form (·, ·). Let t0 = ∑ ei ⊗ ei, t1 = ∑ ei ⊗ ei, t = t0 + t1. Consider also the basis {ei,k} in P1 and dual basis {ei,k} (⊂ P2) in relation to the form 〈·, ·〉, which define by the formulas: ei,2k = ei · u2k, ei,2k+1 = ei · u2k+1, k ∈ Z+, ei,2k = ei · u−2k−1, ei,2k+1 = ei · u−2k−2, k ∈ Z+. Calculate a canonical element r, defining the cocommutator in P r = ∑ ei,k ⊕ ei,k = ∑ k∈Z ∑ i ( ei · v2k ⊗ ei · u−2k−1 + ei · v2k+1 ⊗ ei · u−2k−2 ) = ∞∑ k=0 ((∑ ei ⊗ ei ) · u−1 (v u )2k ) + ∞∑ k=0 ((∑ ei ⊗ ei ) · u−1 (v u )2k+1 ) = t0 u−1 (1− (v/u)2) + t1 u−1(v/u) 1− (v/u)2 = t0 · u (u2 − v2) + t1 · v u2 − v2 = 1 2 ( 1 u− v + 1 u + v )t0 + 1 2 ( 1 u− v − 1 u + v ) t1 = 1 2 t0 + t1 u− v + 1 2 t0 − t1 u + v = 1 2 ∑ k∈Z+ (σk ⊗ id) · t u− εk · v . Denote rσ(u, v) := r. Then we have the following expression for cocommutator: δ : a(u) → [a(u)⊗ 1 + 1⊗ a(v), rσ(u, v)]. Proposition 1. The element rσ(u, v) has the following properties: 1) rσ(u, v) = −r21 σ (v, u); 2) [ r12 σ (u, v), r13 σ (u, w) ] + [ r12 σ (u, v), r23 σ (v, w) ] + [ r13 σ (u, w), r23 σ (v, w) ] = 0. Proof. Let us note, that t21 0 = t1, t211 = t0. Then r21 σ (v, u) = 1 2 t1 + t0 v − u + 1 2 t1 − t0 v + u = −rσ(u, v). The 1) is proved. Property 2) follows from the fact that the element r defined above satisfies the classical Yang–Baxter equation. Actually, the function r(u, v) = t0+t1 u−v = t u−v satisfies the classical Yang–Baxter equation (CYBE) (see [18, 1]):[ r12(u, v), r13(u, w) ] + [ r12(u, v), r23(v, w) ] + [ r13(u, w), r23(v, w) ] = 0. (3) Let s = −id. Let us apply to the left-hand side of (3) the operator id⊗ sk ⊗ sl (k, l ∈ Z2) and substitute (−1)k ·v, (−1)l ·w for v, w, respectively. Taking then the sum over k, l ∈ Z2 and using (s⊗ s)(t) = −t we will obtain the left-hand side of expression from item 2 of proposition. � 3 Quantization The definition of quantization of Lie bialgebras from [1] can be naturally extended on Lie bisuperalgebras. Quantization of Lie bisuperalgebras D is such Hopf superalgebra A~ over ring of formal power series C[[~]] that satisfies the following conditions: Yangian of the Strange Lie Superalgebra of Qn−1 Type, Drinfel’d Approach 5 1) A~/~A~ ∼= U(D), as a Hopf algebra (where U(D) is an universal enveloping algebra of the Lie superalgebra D); 2) the superalgebra A~ isomorphic to U(D)[[~]], as a vector space; 3) it is fulfilled the following correspondence principle: for any x0 ∈ D and any x ∈ A~ equal to x0: x0 ≡ x mod ~ one has ~−1(∆(x)−∆op(x)) mod ~ ≡ ϕ(x) mod ~, where ∆ is a comultiplication, ∆op is an opposite comultiplication (i.e., if ∆(x) = ∑ x′i⊗x′′i , then ∆op(x) = ∑ (−1)p(x′ i)p(x′′ i )x′′i ⊗ x′i). Let us describe the quantization of Lie bisuperalgebra (g[u]σ̃, δ). I recall (see (2)) that g[u]σ̃ = ∞⊕ k=0 ( g0 · u2k ⊕ g1 · u2k+1 ) is graded by degrees of u Lie superalgebra, δ : a(u) → a(u)⊗ 1 + 1⊗ a(v), 1 2 ∑ k∈Z+ (σk ⊗ id) · t u− εk · v  , (4) where t is a Casimir operator and δ is a homogeneous map of degree −1. Let us apply the additional conditions upon quantization. 1) Let A be a graded superalgebra over graded ring C[[~]], deg(~) = 1. 2) The grading of A and the grading of g[u]σ̃ induce the same gradings of U(g[u]σ̃), i.e. A/~A = U(g[u]σ̃) as graded superalgebra over C. I recall (see also [1]) that Hopf superalgebra A over C[[~]] such that A/~A ∼= B, where B is a Hopf superalgebra over C, is called a formal deformation of B. Let p : A → A/~A ∼= B be a canonical projection. If p(a) = x, then an element a is called a deformation of element x. There exist theorems that prove existence and uniqueness of quantization (or formal deforma- tion) in many special cases as well as in our one. But, we will not use these theorems. Let mi ∈ {hi, ki, x ± i , x̂±i } be generators of the Lie superalgebra Qn. We will denote the deforma- tions of the generators mi · uk of the Lie superalgebra A(n, n)[u]σ̃ by mi,k. As generators of associative superalgebra mi, mi · uk generate the superalgebra U(A(n, n)[u]σ̃), its deformations mi,0, mi,1 generate the Hopf superalgebra A. We are going to describe the system of defining relations between these generators. This system of defining relations is received from conditions of compatibility of superalgebra and cosuperalgebra structures of A (or from condition that co- multiplication is a homomorphism of superalgebras). First, we describe the comultiplication on generators mi,1. It follows from condition of homogeneity of quantization 2) comultiplication is defined only by of values of ∆ on generators mi,1. Describe values of ∆ on generators hi,1. Note that condition of homogeneity of quantization implies the fact that U(g0) embeds in A as a Hopf superalgebra. It means that we can identify generators mi,0 with generators of Lie superalgebra g0 = Qn−1. Calculate the value of cocycle δ on the generators hi · u, i = 1, . . . , n− 1. Proposition 2. Let A be a Lie superalgebra with invariant scalar product (·, ·); {ei}, {ei} be a dual relatively this scalar product bases. Then for every element g ∈ A we have equality:[ g ⊗ 1, ∑ ei ⊗ ei ] = − [ 1⊗ g, ∑ ei ⊗ ei ] . (5) 6 V. Stukopin Proof. Note that following the definition of bilinear invariant form, we have the equality: ([g, a], b) = −(−1)deg(g) deg(a)([a, g], b) = −(−1)deg(g) deg(a)(a, [g, b]) for ∀ a, b ∈ A. Therefore ([g, ei], ei) = −(−1)deg(g) deg(a)([ei, g], ei) = −(−1)deg(g) deg(a)(ei, [g, ei]). (6) The scalar product given on vector space V defines isomorphism between V and V ∗, and, therefore, between V ⊗ V and V ⊗ V ∗. Summing over i equality (6) we get∑ i ([g, ei], ei) = ∑ i −(−1)deg(g) deg(a)(ei, [g, ei]). Note the equality of functionals follows from the equality of values of functionals on elements of base and thus we have an equality:∑ i [g, ei]⊗ ei = ∑ i −(−1)deg(g) deg(a)ei ⊗ [g, ei] or [ g ⊗ 1, ∑ ei ⊗ ei ] = − [ 1⊗ g, ∑ ei ⊗ ei ] or equality (5). � Proposition 3. Let A = A0 ⊕ A1 be a Lie superalgebra with such nondegenerate invariant scalar product that A0, A1 are isotropic subspaces, A0, A1 are nondegenerately paired, A0 is a subsuperalgebra, A1 is a module over A0. (For example, the scalar product (1) satisfies these conditions.) Let also {ei}, {ei} be the dual bases in A0, A1, respectively, and t0 = ∑ i ei ⊗ ei, t1 = ∑ i e i ⊗ ei. Then for all a ∈ A0, b ∈ A1 we have the following equalities: [a⊗ 1, t0] = −[1⊗ a, t0], [a⊗ 1, t1] = −[1⊗ a, t1], [b⊗ 1, t0] = −[1⊗ b, t1], [b⊗ 1, t1] = −[1⊗ b, t0]. Now we can calculate the value δ (see (4)) on hi · u δ(hi · u) = [ hi · v ⊗ 1 + 1⊗ hi · u, 1 2 t0 + t1 u− v + 1 2 t0 − t1 u + v ] = [ hi · v ⊗ 1− hi · u⊗ 1, 1 2 t0 + t1 u− v ] + [ hi · v ⊗ 1 + hi · u⊗ 1, 1 2 t0 − t1 u + v ] = [ hi ⊗ 1, 1 2 (t0 + t1) ] + [ hi ⊗ 1, 1 2 (t0 − t1) ] = [hi ⊗ 1, t0] = −[1⊗ hi, t1]. Similarly, it is possible to calculate the values of cocycle on other generators δ(ki · u) = −[ki ⊗ 1, t0] = [1⊗ ki, t1], δ(x±i · u) = −[x±i ⊗ 1, t0] = [1⊗ x±i, t1], δ(x̂±i · u) = −[x̂±i ⊗ 1, t0] = [1⊗ x̂±i, t1]. It follows from homogeneity condition that ∆(hi,1) = ∆0(hi,1) + ~F (xα ⊗ x−α, x̂α ⊗ x̂−α + hi ⊗ hj + ki ⊗ kj). It follows from correspondence principle (item 3) of definition of quantization) that ~−1(∆(hi,1)−∆op(hi,1) = F − τF = [1⊗ hi, t0]. Let t̄0 = ∑ α∈∆+ xα ⊗ x−α − x̂α ⊗ x̂−α + 1 2 n−1∑ i=1 ki ⊗ ki, ∆+ is a set of positive roots of Lie algebra An−1 = sl(n). Yangian of the Strange Lie Superalgebra of Qn−1 Type, Drinfel’d Approach 7 Define ∆(hi,1), by formula ∆(hi,1) = ∆0(hi,1) + ~[1⊗ hi, t̄0]. Let us check that correspondence principle is fulfilled in these cases too: ~−1(∆(hi,1)−∆op(hi,1)) = 1⊗ hi, ∑ α∈∆+ xα ⊗ x−α − x̂α ⊗ x̂−α + 1 2 n−1∑ i=1 ki ⊗ ki  − hi ⊗ 1, ∑ α∈∆+ x−α ⊗ xα − x̂−α ⊗ x̂α + 1 2 n−1∑ i=1 ki ⊗ ki  = 1⊗ hi, ∑ α∈∆+ xα ⊗ x−α − x̂α ⊗ x̂−α − hi ⊗ 1, ∑ α∈∆+ x−α ⊗ xα − x̂−α ⊗ x̂α  . Show that[ hi ⊗ 1, ∑ x−α ⊗ xα + x̂−α ⊗ x̂α ] = [ 1⊗ hi, ∑ x−α ⊗ xα + x̂−α ⊗ x̂α ] . Actually,[ hi ⊗ 1, ∑ x−α ⊗ xα + x̂−α ⊗ x̂α ] = ∑ [hi, x−α]⊗ xα + [hi, x̂−α]⊗ x̂α. On the other hand[ 1⊗ hi, ∑ x−α ⊗ xα + x̂−α ⊗ x̂α ] = ∑ x−α ⊗ [hi, xα] + x̂−α ⊗ [hi, x̂α]. It follows in the standard way, that [hi, xαi−αj ] = −(δik + δjk − δi,k+1 − δj,k+1)xαi−αj , [ki, x̂αi−αj ] = (δik − δjk − δi,k+1 + δj,k+1)x̂αi−αj . Therefore [hi, x−α]⊗ xα = −x−α ⊗ [hi, xα], [hi, x̂−α]⊗ x̂α = x̂−α ⊗ [hi, x̂α]. Hence,[ hi ⊗ 1, ∑ x−α ⊗ xα + x̂−α ⊗ x̂α ] = [ 1⊗ hi, ∑ x−α ⊗ xα + x̂−α ⊗ x̂α ] and equality ~−1(∆(hi,1)−∆op(hi,1)) = 1⊗ hi, ∑ α∈∆+ xα ⊗ x−α − x̂α ⊗ x̂−α  − hi ⊗ 1, ∑ α∈∆+ x−α ⊗ xα − x̂−α ⊗ x̂α  = [1⊗ hi, t0] = δ(hi · u) is proved. Similarly we can define comultiplication on other generators. We get ∆(x+ i,1) = ∆0(x+ i,1) + ~[1⊗ x+ i , t̄0], ∆(x−i,1) = ∆0(x−i,1) + ~[x−i ⊗ 1, t̄0]. 8 V. Stukopin The following relations hold and comultiplication preserves them [hi,1, x ± j,0] = ±(α,αj)x±j,1, [ki,1, x ± j,0] = ±(α,αj)x̂±j,1, [hi,1, x̂ ± j,0] = ±(̃α,αj)x̂±j,1, [ki,1, x̂ ± j,0] = ±(α,αj)x±j,1. Let us prove these relations. It is sufficient to check one of them. Let us prove the first relation [∆(hi,1),∆(x±j,0)] = ±(αi, αj)∆(x±j,1). Actually, [∆(hi,1),∆(x±j,0)] = [∆0(hi,1) + ~[1⊗ hi, t̄0], x±j,0 ⊗ 1 + 1⊗ x±j,0] = [hi,1, x ± j,0]⊗ 1 + 1⊗ [hi,1, x ± j,0] + ~[[1⊗ hi, t̄0], x±j,0 ⊗ 1] + ~[[1⊗ hi, t̄0], 1⊗ x±j,0] = [∆(hi,0),∆(x±j,1)] = ±(αi, αj)∆(x±j,1). Now we can describe the Hopf superalgebra A = Ah, which is a deformation (quantization) of the Lie bisuperalgebra (gσ̃, δ). Let us introduce new notations. Let {a, b} be an anticommutator of elements a, b. Let m ∈ {0, 1} and k̄i,m = 1 n ( − i−1∑ r=0 rkr,m + n−1∑ r=i (n− r)kr,m ) , h̄i,m = 1 n ( − i−1∑ r=0 rhr,m + n−1∑ r=i (n− r)hr,m ) . Let also, {α1, · · · , αn−1} be a set of simple roots of sl(n), ˜(αi, αj) := (δi,j+1 − δi+1,j). Theorem 1. Hopf superalgebra A = Ah over C[[~]] is generated by generators hi,0, x±i,0, ki,0, x̂±i,0, hi,1, x±i,1, ki,1, x̂±i,1, 1 ≤ i ≤ n−1 (h, x are even, k, x̂ are odd generators). These generators satisfy the following defining relations: [hi,0, hj,0] = [hi,0, hj,1] = [hi,1, hj,1] = 0, [hi,0, kj,0] = [ki,1, kj,0] = 0, [hi,0, x ± j,0] = ±(αi, αj)x±j,0, [ki,0, x ± j,0] = ± ˜(αi, αj)x̂±j,0, [ki,0, kj,0] = 2(δi,j − δi,j+1)h̄i,0 + 2(δi,j − δi,j−1)h̄i+1,0, ki,1 = 1 2 [hi+1,1 − hi−1,1, ki,0], [x+ i,0, x − j,0] = δijhi,0, [x+ i,1, x − j,0] = [x+ i,0, x − j,1] = δij h̃i,1 = δij ( hi,1 + ~ 2 h2 i,0 ) , [x̂+ i,0, x − j,0] = [x+ i,0, x̂ − j,0] = δijki,0, [x+ i,1, x − j,0] = δij ( hi,1 + ~ 2 h2 i,0 ) , [x̂+ i,1, x − j,0] = [x+ i,0, x̂ − j,1] = δijki,1, [x+ i,1, x̂ − j,0] = −[x̂+ i,0, x − j,1] = δij(k̄i,1 + k̄i+1,1), [x̂+ i,1, x̂ − j,0] = δij ( hi,1 + ~ 2 h2 i,0 ) , [hi,1, x ± j,0] = ±(αi, αj)(x±j,1), [hi,1, x̂ ± j,0] = ± ˜(αi, αj)(x̂±j,1), ki,1 = 1 2 [hi+1,1 − hi−1,1, ki,0], [ki,1, x ± j,0] = ±(αi, αj)x̂±j,1, [ki,1, x̂ ± j,0] = ±(αi, αj)x±j,1, [hi,1, kj,0] = 2(δi,j − δi,j+1)k̄i,1 + 2(δi,j − δi,j−1)k̄i+1,1, Yangian of the Strange Lie Superalgebra of Qn−1 Type, Drinfel’d Approach 9 [x±i,1, x ± j,0]− [x±i,0, x ± j,1] = ±~ 2 ((αi, αj){x±i,0, x ± j,0}+ ˜(αi, αj){x̂±i,0, x̂ ± j,0}), [x̂±i,1, x ± j,0]− [x̂±i,0, x ± j,1] = ±~ 2 (− ˜(αi, αj){x̂±i,0, x ± j,0}+ ˜(αi, αj){x±i,0, x̂ ± j,0}), [x̂±i,1, x̂ ± j,0]− [x̂±i,0, x̂ ± j,1] = ±~ 2 ( ˜(αi, αj){x±i,0, x ± j,0}+ (αi, αj){x̂±i,0, x̂ ± j,0}), (adx±i,0) 2(x±j,0) = [x±i,0, [x ± i,0, x ± j,0]] = 0, i 6= j, (ad x̂±i,0) 2(x±j,0) = [x̂±i,0, [x̂ ± i,0, x ± j,0]] = 0 = [x̂±i,0, [x ± i,0, x ± j,0]], i 6= j, (adx±i,0) 2(x̂±j,0) = [x±i,0, [x ± i,0, x̂ ± j,0]] = 0, i 6= j, [x̂±i,0, x̂ ± j,0] = [x±i,0, x ± j,0], [x̂±i,0, x ± j,0] = [x̂±i,0, x ± j,0],∑ σ∈S3 [x±i,σ(s1), [x ± i,σ(s2), x ± i,σ(s3)]] = 0, ∑ σ∈S3 [x̂±i,σ(s1), [x ± i,σ(s2), x ± i,σ(s3)]] = 0, s1, s2, s3 ∈ {0, 1}. Here Sn is a permutation group of n elements. The comultiplication ∆ is defined by the formulas: ∆(hi,0) = hi,0 ⊗ 1 + 1⊗ hi,0, ∆(x±i,0) = x±i,0 ⊗ 1 + 1⊗ x±i,0, ∆(ki,0) = ki,0 ⊗ 1− 1⊗ ki,0, ∆(x̂±i,0) = x̂±i,0 ⊗ 1 + 1⊗ x̂±i,0, ∆(hi,1) = hi,1 ⊗ 1 + 1⊗ hi,1 + [1⊗ hi,0, t̄0] = hi,1 ⊗ 1 + 1⊗ hi,1 + ~ ki,0 ⊗ (k̄i,0 + k̄i+1,0)− ∑ α∈∆+ ( (αi, α)xα,0 ⊗ x−α,0 + (̃αi, α)x̂α,0 ⊗ x̂−α,0 ) , ∆(x+ i,1) = x+ i,1 ⊗ 1 + 1⊗ x+ i,1 + [1⊗ x+ i,0, t̄0] = x+ i,1 ⊗ 1 + 1⊗ x+ i,1 + ~ ( x̂+ i,0 ⊗ (k̄i,0 + k̄i+1,0) + x+ i,0 ⊗ hi,0 − ∑ α∈∆+ ( [x+ i,0, xα,0]⊗ x−α,0 + [x+ i,0, x̂−α,0]⊗ x̂−α,0 )) , ∆(x−i,1) = x−i,1 ⊗ 1 + 1⊗ x−i,1 + [x−i,0 ⊗ 1, t̄0] = x−i,1 ⊗ 1 + 1⊗ x−i,1 + ~ (( k̄i,0 + k̄i+1,0)⊗ x̂−i,0 + hi,0 ⊗ x−i,0 − ∑ α∈∆+ ( xα,0 ⊗ [x−i,0, x−α,0] + x̂α,0 ⊗ [x−i,0, x̂−α,0] )) , ∆(x̂+ i,1) = x̂+ i,1 ⊗ 1− 1⊗ x̂+ i,1 + ~ ( x+ i,0 ⊗ (k̄i,0 + k̄i+1,0) + x̂+ i,0 ⊗ hi,0 − ∑ α∈∆+ ( [x̂+ i,0, xα,0]⊗ x−α,0 − [x+ i,0, x−α,0]⊗ x̂−α,0 )) , ∆(x̂−i,1) = x̂−i,1 ⊗ 1− 1⊗ x̂−i,1 + [x̂−i,0 ⊗ 1, t̄0] = x̂−i,1 ⊗ 1 + 1⊗ x̂−i,1 + ~ ( (k̄i,0 + k̄i+1,0)⊗ x−i,0 + hi,0 ⊗ x̂−i,0 10 V. Stukopin − ∑ α∈∆+ ( xα,0 ⊗ [x̂−i,0, x−α,0] + x̂α,0 ⊗ [x−i,0, x−α,0] )) , ∆(ki,1) = ki,1 ⊗ 1− 1⊗ ki,1 + [ki,0 ⊗ 1, t̄0] = ki,1 ⊗ 1 + 1⊗ ki,1 + ~ ( (h̄i,0 + h̄i+1,0)⊗ (k̄i,0 + k̄i+1,0) − ∑ α∈∆+ ( (αi, α)x̂α,0 ⊗ x−α,0 + (̃αi, α)xα,0 ⊗ x̂−α,0 )) . Let us note that the Hopf superalgebras A~1 and A~2 for fixed ~1, ~2 6= 0 (as superalgebras over C) are isomorphic. Setting ~ = 1 in these formulas we receive the system of defining relations of Yangian Y (Qn−1). 4 Current system of generators Let G = Qn. Let us introduce a new system of generators and defining relations. This system in the quasiclassical limit transforms to the current system of generators for twisted current Lie superalgebra ℘1 = G[u]σ̃ of polynomial currents. We introduce the generators h̃i,m, ki,m, x±i,m, x̃±i,m, i ∈ I = {1, 2, . . . , n− 1}, m ∈ Z+, by the following formulas: x±i,m+1 = ±1 2 [hi,1, x ± i,m], (7) x̂±i,2m+1 = 1 2 [hi+1,1 − hi−1,1, x̂ ± i,2m], (8) x̂±i,2m+2 = −1 2 [hi+1,1,−hi−1,1, x̂ ± i,2m+1], (9) ki,m+1 = 1 2 [hi+1,1,−hi−1,1, ki,m], (10) h̃i,m = [x+ i,m, x−i,0], (11) k̄i,m = 1 n ( − i−1∑ r=0 rkr,m + n−1∑ r=i (n− r)kr,m ) , h̄i,m = 1 n ( − i−1∑ r=0 rh̃r,m + n−1∑ r=i (n− r)h̃r,m ) . (12) This section results in to the following theorem describing the Y (Qn−1) in a convenient form. Theorem 2. The Yangian Y (Qn−1) isomorphic to the unital associative superalgebra over C, generated by generators h̃i,m, ki,m, x±i,m, x̂±i,m, i ∈ I = {1, 2, . . . , n − 1}, m ∈ Z+ (isomorphism is given by the formulas (7)–(12)), satisfying the following system of defining relations: [h̃i,m, h̃j,n] = 0, h̃i,m+n = δij [x+ i,m, x−i,n], [x̂+ i,m, x−j,2k] = [x+ i,2k, x̃ − j,m] = δijki,m+2k ( n− 2 n )k , [x̂+ i,m, x−j,2k+1] = [x+ i,2k+1, x̂ − j,m] = δij(k̄i,m+2k+1 + k̄i+1,m+2k+1) ( n− 2 n )k , [hi,0, x ± j,l] = ±(αi, αj)x±j,l, [hi,0, x̃ ± j,l] = ±(αi, αj)x̂±j,l, [ki,0, x ± j,l] = ±(αi, αj)x̂±j,l, [ki,0, x̂ ± j,l] = ± ˜(αi, αj)x±j,l, Yangian of the Strange Lie Superalgebra of Qn−1 Type, Drinfel’d Approach 11 ki,m+1 = 1 2 [hi+1,1,−hi−1,1, ki,m], h̃i,1 = hi,1 + 1 2 h2 i,0, x̂±i,2m+1 = 1 2 [hi+1,1,−hi−1,1, x̂ ± i,2m], x̂±i,2m+2 = 1 2 [hi+1,1,−hi−1,1, x̂ ± i,2m+1], [h̃i,m+1, x ± j,r]− [h̃i,m, x±j,r+1] = ±(αi,αj) 2 {h̃i,m, x±j,r}+ (±δi,j+1 − δi+1,j){ki,m, x̂±j,r}, we use before δ sign “+” in the case m + r ∈ 2Z+, and sign “−” for m + r ∈ 2Z+ + 1; [x±i,m+1, x ± j,r]− [x±i,m, x±j,r+1] = ±(αi,αj) 2 {x±i,m, x±j,r}+ (±δi,j+1 − δi+1,j){x̂±i,m, x̃±j,r}, here signs before δ are defined also as in the previous formula; [x̂±i,m+1, x ± j,r]− [x̂±i,m, x±j,r+1] = ± ˜(αi, αj) 2 {x̂±i,m, x±j,r} ∓ ˜(αi, αj) 2 {x±i,m, x̂±j,r}, [x̂±i,m+1, x̂ ± j,r]− [x̂±i,m, x̂±j,r+1] = ±(αi, αj) 2 {x̂±i,m, x̂±j,r} ∓ (̃αi,αj) 2 {x±i,m, x±j,r}, [ki,m+1, x ± j,r]− [ki,m, x±j,r+1] = ±(αi,αj) 2 {ki,m, x±j,r} + (±δi,j+1 − δi+1,j){(h̄i,m + h̄i+1,m), x̂±j,r}, [h̃i,2m+1, kj,r] = 2((δi,j − δi,j+1)k̄i,2m+r+1 + (δi,j − δi,j−1)k̄i+1,2m+r+1), [h̃i,2m, kj,2r+1] = 0, [ki,2k, kj,2l] = 2(δi,j − δi,j+1)h̄i,2(k+l) + 2(δi,j − δi,j−1)h̄i+1,2(k+l), [ki,2m+1, kj,2r] = 0, ∑ σ∈S3 [x±i,σ(s1), [x ± i,σ(s2), x ± j,σ(s3)]] = 0, ∑ σ∈S3 [x̂±i,σ(s1), [x ± i,σ(s2), x ± j,σ(s3)]] = 0, s1, s2, s3 ∈ Z+. Note that proof of this theorem is quite complicated and technical. We note only two issues of the proof: 1) the formulas for even generators are proved similarly to the case of Y (A(m,n)) (see [10]); 2) the defining relations given in the Theorem 1 easily follows from those given in Theorem 2. In conclusion let us note that the problems of explicit description of quantum double of Yangian of strange Lie superalgebra and computation of the universal R-matrix are not discussed in paper and will be considered in further work. This paper makes basis for such research. References [1] Drinfel’d V.G., Quantum groups, in Proceedings of the International Congress of Mathematicians, Vol. 1, Berkley, 1988, 789–820. [2] Drinfel’d V.G., Hopf algebras and the quantum Yang–Baxter equation, Soviet Math. Dokl. 32 (1985), 254– 258. [3] Drinfel’d V.G., A new realization of Yangians and of quantum affine algebras, Soviet Math. Dokl. 36 (1988), 212–216. [4] Molev A., Yangians and their applications, in Handbook of Algebra, Vol. 3, North-Holland, Amsterdam, 2003, 907–959, math.QA/0211288. [5] Chari V., Pressley A., A guide to quantum groups, Camb. Univ. Press, Cambridge, 1995. [6] Zhang R.B., Representations of super Yangian, J. Math. Phys. 36 (1995), 3854–3865, hep-th/9411243. http://arxiv.org/abs/math.QA/0211288 http://arxiv.org/abs/hep-th/9411243 12 V. Stukopin [7] Zhang R.B., The gl(M, N) super Yangian and its finite-dimensional representations, Lett. Math. Phys. 37 (1996), 419–434, q-alg/9507029. [8] Zhang Y.-Z., Super-Yangian double and its central extension, Phys. Lett. A 234 (1997), 20–26, q-alg/9703027. [9] Crampe N., Hopf structure of the Yangian Y (sln) in the Drinfel’d realization, J. Math. Phys. 45 (2004), 434–447, math.QA/0304254. [10] Stukopin V., Yangians of Lie superalgebras of type A(m, n), Funct. Anal. Appl. 28 (1994), 217–219. 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Phys. 208 (1999), 195–223, math.QA/9902146. [16] Kac V., A sketch of Lie superalgebra theory, Comm. Math. Phys. 53 (1977), 31–64. [17] Frappat L., Sciarrino A., Sorba P., Dictionary on Lie superalgebras, Academic Press, Inc., San Diego, CA, 2000. [18] Leites D., Serganova V., Solutions of the classical Yang–Baxter equations for simple Lie superalgebras, Theoret. and Math. Phys. 58 (1984), 16–24. http://arxiv.org/abs/q-alg/9507029 http://arxiv.org/abs/q-alg/9703027 http://arxiv.org/abs/math.QA/0304254 http://arxiv.org/abs/math.QA/0504302 http://arxiv.org/abs/math.QA/9902146 1 Introduction 2 Twisted current bisuperalgebras 3 Quantization 4 Current system of generators References

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