SQU Journal for Science, 2020, 25(2), 107-111 DOI:10.24200/squjs.vol25iss2pp107-111 Sultan Qaboos University 107 Dicyclic Groups and Frobenius Manifolds Yassir Dinar and Zainab Al-Maamari Department of Mathematics, College of Science, Sultan Qaboos University, P.O. Box 36, Al-Khod, PC 123, Muscat, Sultanate of Oman. *Email: dinar@squ.edu.om ABSTRACT: The orbits space of an irreducible representation of a finite group is a variety whose coordinate ring is finitely generated by homogeneous invariant polynomials. Boris Dubrovin showed that the orbits spaces of the reflection groups acquire the structure of polynomial Frobenius manifolds. Dubrovin’s method to construct examples of Frobenius manifolds on orbits spaces was carried for other linear representations of discrete groups which have in common that the coordinate rings of the orbits spaces are polynomial rings. In this article, we show that the orbits space of an irreducible representation of a dicyclic group acquires two structures of Frobenius manifolds. The coordinate ring of this orbits space is not a polynomial ring. Keywords: Differential geometry; Frobenius manifolds; Invariant theory; Dicyclic group; Orbifolds. ةالهندسيفروبينيس وفضاءات زمر مزدوجة الدورة زينب المعمري و ياسر دينار حدود من كثيرات تتشكل ةحداثية محدودالقة ح يمتلك متنوعفضاء محدودة هو لزمرةقابل لالختزال الغير لتمثيلل مداراتالفضاء إن :صلخمال .حدودالكثيرات ل الهندسية فضاءات فروبينيس تحتفظ ببنية لمتعاكسةا لزمرل يةالمدار اتفضاءال. أثبت بوريس دوبروفين أن وغير متبدلة متجانسة عامة في لها خاصية ،أخرى متقطعة لزمر اخطي تتمثل يةمدارفضاءات أمثلة لفضاءات فروبينيس على يمكن ايجاد ،طريقة دوبروفين باستخدام ثنائية زمرل لالختزال ةغير قابل تتمثيالل تمدارالأن فضاء ،في هذه المقالةنبين . حدودال كثيرةحلقات تكون ،الحلقات اإلحداثية للفضاءات المدارية .الحدودلكثيرات ةليست حلق ات المذكورفضاء المدارلاإلحداثية ةحلقإن ال .ات فروبينيستكتسب هيكلين من فضاء انالدور ، المدارات.راندوثنائية ال ة، مجموعفضاءات فروبينيس، النظرية الثابتةالهندسة التفاضلية، :مفتاحيةالكلمات ال 1. Introduction he notion of a Frobenius manifold was introduced by Boris Dubrovin as a geometric realization of a potential F satisfying a system of partial differential equations known in topological fields theory as WDVV equations [1]. Besides topological fields theory, Frobenius manifolds appear in many fields such as invariant theory, integrable systems, quantum cohomology and singularity theory. This article contributes to the relation between Frobenius manifolds and invariant theory. Let W be a finite group of linear transformations acting on a complex vector space V of dimention r. Then the orbits space M = V/W of this group is a variety whose coordinate ring is the ring of invariant polynomials C[V ] W . The ring C[V ] W is finitely generated by homogeneous polynomials. If f1,f2,...,fm is a set of such generators then m ≥ r and the relation between them is called syzygies. The set of generators are not unique, nor are their degrees [2,3]. An element w ∈ W is called a reflection if it fixes a subspace of V of codimention one pointwise. The group W is called a complex reflection group if it is generated by reflections. Then Shephard-Todd-Chevalley theorem states that W is a reflection group if and only if the invariant ring C[V ] W is a polynomial ring [11], i.e. it is generated by r algebraically independent homogeneous polynomials (so there are no syzygies). Furthermore, when W is a reflection group, the degrees of such a set generators of C[V ] W are uniquely specified by the group and we refer to them as the degrees of W. T YASIR DINAR and ZAINAB AL-MAAMARI 108 Let us assume W is a Shephard group, i.e. a symmetry group of a regular complex polytope. Then W is a reflection group. Let f1,f2,...,fr be a set of algebraically independent homogeneous generators of C[V ] W . We assume that degree fi is less than or equal to the degree fj when i < j. Then the inverse of the Hessian of f1 defines a flat metric (·,·)2 on * T M [4]. There is another flat metric (·,·)1 on T∗M, which was studied initially by Saito [5, 6], defined as the Lie derivative of (·,·)2 along the vector field rf e   . The two metrics form what is called ‘a flat pencil of metrics’ (more details are given below). Dubrovin used the properties of this flat pencil of metrics to construct polynomial Frobenius manifolds [7] (see [8] and [9] for the case of Coxeter groups). This article is about applying Dubrovin’s method for other finite linear groups than Shephard groups. Dubrovin’s method to construct Frobenius manifolds, through finding flat pencils of metrics on orbits spaces, was carried out for infinite linear groups like extended affine Weyl groups [10, 11], Jacobi groups [12] and recently a new extension of affine Weyl groups [13]. They all have in common that the invariant rings are polynomial rings. Moreover, even when considering a generalization of Frobenius manifold structure on orbits spaces, many results were obtained under the assumption that the invariant ring is a polynomial ring [14]. It is then a natural question to ask about applying Dubrovin’s method on orbits spaces of finite non-reflection groups. In this article we apply Dubrovin’s method and construct Frobenius manifolds on orbits spaces of Dicyclic groups. The resulting Frobenius manifolds can be obtained by using an ad-hoc procedure, but it is fascinating to find them on orbits spaces of some group. Precisely, we will show that the orbits space of the Dicyclic group of order 4n is endowed with two structures of Frobenius manifolds which up to scaling has the following potential (1.1) where or . To make the article as self-contained as possible, we review in the next section the definition of the Frobenius manifold and its relation with the theory of flat pencils of metrics. In the last section we obtain the promised Frobenius manifolds by direct calculations. 2. Preliminaries 2.1 Frobenius manifolds A Frobenius algebra is a commutative associative algebra with unity e and an invariant nondegenerate bilinear form < ·,· >. A Frobenius manifold is a manifold M with a smooth structure of a Frobenius algebra on the tangent space TtM at any point t ∈ M with certain compatibility conditions [6]. Globally, we require the metric < ·,· > to be flat and the unity vector field e to be covariantly constant with respect to it. In the flat coordinates (t 1 ,...,t r ) where r e t    the compatibility conditions imply that there exists a function F(t 1 ,...,t r ) such that ηij =< ∂ti,∂tj >= ∂tr∂ti∂tjF(t) and the structure constants of the Frobenius algebra are given by 1 ( )p i j k kp ij t t t p C t     where 1 ij  denotes the inverse of the matrix ηij. In this work, we consider Frobenius manifolds where the quasihomogeneity condition takes the form 1 ( ) (3 ) ( ); 1.i r i i rt i d t t d t d      (2.1) This condition defines the degrees di and the charge d of the Frobenius structure. The associativity of the Frobenius algebra implies that the potential F(t) satisfies a system of partial differential equations which appears in topological field theory and is called Witten-Dijkgraaf-Verlinde-Verlinde (WDVV) equations: 1 1 , , ( ) ( ) ( ) ( ), , , , .i j k p q n n j k p q i kp kp t t t t t t t t t t t t k p k p t t t t i j q n                 (2.2) Detailed information about Frobenius manifolds and related topics can be found in [1]. 2.2 Flat pencil of metrics and Frobenius manifolds In this section we review the relation between the geometry of flat pencil of metrics and Frobenius manifolds. See [15] for details. DICYCLIC GROUPS AND FROBENIUS MANIFOLDS 109 Let M be a smooth manifold of dimension r. A symmetric bilinear form (·,·) on * T M is called a contravariant metric if it is invertible on an open dense subset M0 ⊂ M. In local coordinates, if we set Ω ij (u) = (du i ,du j ); i,j = 1,...,r (2.3) then the inverse matrix Ωij(u) of Ω ij (u) determines a metric < ·,· > on TM0. We define the contravariant Christoffel symbols of (·,·) by Γ where Γ j sk are the Christoffel symbols of < ·,· >. We say the metric (·,·) is flat if < ·,· > is flat. Let 1 ( , )  and 2 ( , )  be two contravariant flat metrics on M and denote their Christoffel symbols by 1; ( ) ij k u and 2; ( ) ij k u respectively. We say 1 ( , )  and 2 ( , )  form a flat pencil of metrics if 1 2 ( , ) : ( , ) ( , )          defines a flat metric on * T M for a generic  and its Christoffel symbols are given by ; 2; 1;( ) ( ) ( ). ij ij ij k k k u u u       Let 1 ( , )  and 2 ( , )  be two contravariant metrics on M and denote their matrices by 1 ( ) ij u and 2 ( ) ij u , respectively, in some coordinates 1 ( ,..., ) r u u . Suppose that they form a flat pencil of metrics. This flat pencil of metrics is called quasihomogeneous of degree d if there exists a function on M such that the vector fields (2.4) satisfy the following relations [e,E] = e, LieE( , )2 = (d − 1)( , )2, Liee( , )2 = ( , )1, Liee( , )1 = 0. Here LieX denote the Lie derivative along a given vector field X. In addition, the quasihomogeneous flat pencil of metrics is called regular if the (1,1)-tensor is nondegenerate on M. The following theorem due to Dubrovin gives a connection between the geometry of Frobenius manifolds and flat pencils of metrics. Theorem 2.1. [15] A quasihomogeneous regular flat pencil of metrics of degree d on a manifold M defines a Frobenius structure on M of charge d. Let us assume the flat pencil of metrics on M is regular quasihomogeneous of degree d. Let 1 ( ,..., ) r t t be flat coordinates of 1 ( , )  where 1 , r t t e    and i i i t i E d t  . Let ij denote the inverse of 1 ( ) ij t . Then it turns out that the potential 1 ( ,..., ) r t t is obtained from the equations (2.5) It is well known that from a Frobenius manifold we always have a flat pencil of metrics but it does not necessarily satisfy the regularity condition [15]. 3. Dicyclic groups Let n be a natural number greater than 1 and W be the matrix group generated by (3.1) where ξ is a primitive 2n-th root of unity. Then σ and α satisfy the relations 2 2 1 1. 1, , n n            . (3.2) Thus W is isomorphic to the dicyclic group of order 4n. The invariant ring of W is generated by the following homogeneous polynomials [2] (3.3) subject to the relation . (3.4) The orbits space M of W is a variety isomorphic to the hypersurface T defined as the zero set of equation (3.4) in C 3 . Consider equation (3.4) as a quadratic equation in u3. Then any point p out of the discriminant locus has a small YASIR DINAR and ZAINAB AL-MAAMARI 110 neighbourhood Up where u1 and u2 act as coordinates. In what follows we assume that we fix such the open set U ⊂ V with coordinates (u1,u2) and we omit the subscript p. Let h be the Hessian matrix of u1, i.e. and let h −1 denotes its inverse. Then, by direct calculations, h −1 defines a flat contravariant metric (·,·)2 on U. This metric, in the coordinates u1 and u2, is given as follows . (3.5) Let e be a vector field of the form f(u1)∂u2, where f(u1) is any smooth function. Then, by direct calculations, the Lie derivative (·,·)1 of (·,·)2 along e forms with (·,·)2 a flat pencil of metrics. This metric takes the value . (3.6) The guess for the vector field to take this from was inspired by [1]. In order to get a quasihomogeneous flat pencil of metrics, we need the Lie derivative of (·,·)1 with respect to e to equal zero. This condition leads to the following differential equation for f(u) (3.7) which has two independent solutions and . (3.8) Let us assume . Then . (3.9) It turns out that the two metrics (·,·)2 and (·,·)1 form a quasihomogeneous flat pencil of metrics with degree . (3.10) In the notations of equations (2.4), we have and . (3.11) This flat pencil of metrics is also regular since the (1,1)-tensor Ri j equals the nondegenerate matrix . (3.12) Flat coordinates for (·,·)1 are obtained by setting . (3.13) In these coordinates we get . (3.14) The potential  of the corresponding Frobenius manifold is . (3.15) Let us take . Then similar to the method above, we get a regular quasihomogenous flat pencil of metrics of degree (3.16) with . The resulting potential will be . (3.17) We repeat the calculation by taking (u1,u3) as coordinates instead of (u1,u2). It turns out that even though the middle steps may differ in values, the resulting Frobenius manifolds are exactly the same as those given by the potentials (3.15),(3.17). DICYCLIC GROUPS AND FROBENIUS MANIFOLDS 111 We observe that Dubrovin computed by an ad hoc procedure all possible potentials of 2-dimensional Frobenius manifolds [6]. The potentials found in this article, after scaling, are listed by Dubrovin in the form (3.18) where or . However, finding this by using the method of a flat pencil of metrics on an orbits space of a finite group that is not a reflection group is a surprising result. 4. Conclusion In this paper we prove that for a linear representation of Dicyclic groups we can still use Dubrovin's method to construct Frobenius manifolds on its orbits spaces. In addition, the method leads to two structures of Frobenius manifolds. The result reported in this article is a part of work in progress to apply Dubrovin’s method on orbits spaces of finite groups to find interesting new examples of Frobenius manifolds. In future, we will consider irreducible representations of Coxeter groups which are not reflection representations [16]. Conflict of interest The authors declare no conflict of interest. Acknowledgment This work is funded by the internal grant of Sultan Qaboos University (IG/SCI/DOMS/19/08). The authors thank Hans-Christian Herbig for stimulating discussions and the anonymous reviewers for their comments and suggestions. References 1. Dubrovin, B. Geometry of 2D topological field theories. 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Letters in Mathematical Physics, 2020, 110 (7), 1903-1940. 14. Arsie, A. and Lorenzoni, P. Complex reflection groups, logarithmic connections and bi-flat F-manifolds. Letters in Mathematical Physics, 2017, 107(10), 1919-1961. 15. Dubrovin, B. Flat pencils of metrics and Frobenius manifolds. Integrable systems and algebraic geometry Kobe/Kyoto, 1997, 47-72. 16. Al-Maamari, Z. and Dinar, Y. Frobenius manifolds from a few linear representations, in preparation. Received 15 November 2019 Accepted 16 July 2020