Volume 2011, Issue 1 252186
Research Article
Open Access

Integer Solutions of Integral Inequalities and H-Invariant Jacobian Poisson Structures

G. Ortenzi

G. Ortenzi

Dipartimento di Matematica Pura e Applicazioni, Università degli Milano Bicocca, Via R.Cozzi 53, 20125 Milano, Italy unimib.it

Search for more papers by this author
V. Rubtsov

V. Rubtsov

Département de Mathématiques 2, Laboratoire Angevin de Recherche en Mathématiques Université D′Angers, boulevard Lavoisier, 49045 Angers, France univ-angers.fr

Search for more papers by this author
S. R. Tagne Pelap

Corresponding Author

S. R. Tagne Pelap

Mathematics Research Unit at Luxembourg, University of Luxembourg, 6 rue Richard Coudenhove-Kalergi, 1359 Luxembourg City, Luxembourg uni.lu

Search for more papers by this author
First published: 03 October 2011
Citations: 2
Academic Editor: Yao-Zhong Zhang

Abstract

We study the Jacobian Poisson structures in any dimension invariant with respect to the discrete Heisenberg group. The classification problem is related to the discrete volume of suitable solids. Particular attention is given to dimension 3 whose simplest example is the Artin-Schelter-Tate Poisson tensors.

1. Introduction

This paper continues the authors′ program of studies of the Heisenberg invariance properties of polynomial Poisson algebras which were started in [1] and extended in [2, 3]. Formally speaking, we consider the polynomials in n variables [x0, x1, …, xn−1] over and the action of some subgroup Hn of GLn() generated by the shifts operators xixi+1(mod n) and by the operators xɛixi, where ɛn = 1. We are interested in the polynomial Poisson brackets on [x0, x1, …, xn−1] which are “stable” under this actions (we will give more precise definition below).

The most famous examples of the Heisenberg invariant polynomial Poisson structures are the Sklyanin-Odesskii-Feigin-Artin-Tate quadratic Poisson brackets known also as the elliptic Poisson structures. One can also think about these algebras like the “quasiclassical limits” of elliptic Sklyanin associative algebras. These is a class of Noetherian graded associative algebras which are Koszul, Cohen-Macaulay, and have the same Hilbert function as a polynomial ring with n variables. The above-mentioned Heisenberg group action provides the automorphisms of Sklyanin algebras which are compatible with the grading and defines an Hn-action on the elliptic quadratic Poisson structures on n. The latter are identified with Poisson structures on some moduli spaces of the degree n and rank k + 1 vector bundles with parabolic structure (= the flag 0 ⊂ Fk+1 on the elliptic curve ). We will denote this elliptic Poisson algebras by qn;k(). The algebras qn;k(E) arise in the Feigin-Odesskii “deformational” approach and form a subclass of polynomial Poisson structures. A comprehensive review of elliptic algebras can be found in [4] to which we refer for all additional information. We will mention only that as we have proved in [3] all elliptic Poisson algebras (being in particular Heisenberg-invariant) are unimodular.

Another interesting class of polynomial Poisson structures consists of so-called Jacobian Poisson structures (JPS). These structures are a special case of Nambu-Poisson structures. Their rank is two, and the Jacobian Poisson bracket {P, Q} of two polynomials P and Q is given by the determinant of Jacobi matrix of functions (P, Q, P1, …, Pn−2). The polynomials Pi, 1 ≤ in − 2 are Casimirs of the bracket and under some mild condition of independence are generators of the centrum for the Jacobian Poisson algebra structure on [x0, …, xn−1]. This type of Poisson algebras was intensively studied (due to their natural origin and relative simplicity) in a huge number of publications among which we should mention [1, 59].

There are some beautiful intersections between two described types of polynomial Poisson structures: when we are restricting ourselves to the class of quadratic Poisson brackets then there are only Artin-Schelter-Tate (n = 3) and Sklyanin (n = 4) algebras which are both elliptic and Jacobian. It is no longer true for n > 4. The relations between the Sklyanin Poisson algebras qn,k() whose centrum has dimension 1 (for n odd) and 2 (for n even) in the case k = 1 and is generated by l = 𝔤cd(n, k + 1) Casimirs for qn,k() for k > 1 are in general quite obscure. We can easily found that sometimes the JPS structures correspond to some degenerations of the Sklyanin elliptic algebras. One example of such JPS for n = 5 was remarked in [8] and was attributed to so-called Briesckorn-Pham polynomials for n = 5
()
It is easy to check that the homogeneous quintic P = P1P2P3 (see Section 4.2) defines a Casimir for some rational degeneration of (one of) elliptic algebras q5,1() and q5,2() if it satisfies the H-invariance condition.
In this paper, we will study the Jacobian Poisson structures in any number of variables which are Heisenberg-invariant and we relate all such structures to some graded subvector space of polynomial algebra. This vector space is completely determined by some enumerative problem of a number-theoretic type. More precisely, the homogeneous subspace i of of degree i is in bijection with integer solutions of a system of Diophant inequalities. Geometric interpretation of the dimension of i is described in terms of integer points in a convex polytope given by this Diophant system. In the special case of dimension 3, is a subalgebra of polynomial algebra with 3 variables and all JPS are given by this space. We solve explicitly the enumerative problem in this case and obtain a complete classification of the H-invariant not necessarily quadratic Jacobian Poisson algebras with three generators. As a byproduct, we explicitly compute the Poincaré series of . In this dimension, we observe that the H-invariant JPS of degree 5 is given by the Casimir sextic
()
a, b, c, d. This structure is a “projectively dual” to the Artin-Schelter-Tate elliptic Poisson structure which is the H-invariant JPS given by the cubic
()
where γ. In fact, the algebraic variety : {P = 0} ∈ 2 is the (generically) projectively dual to the elliptic curve : {P = 0} ⊂ 2.

The paper is organized as follows: in Section 2, we remind a definition of the Heisenberg group in the Schroedinger representation and describe its action on Poisson polynomial tensors and also the definition of JPS. In Section 3, we treat the above mentioned enumerative problem in dimension 3. The last section concerns the case of any dimension. Here, we discuss some possible approaches to the general enumerative question.

2. Preliminary Facts

Throughout of this paper, K is a field of characteristic zero. Let us start by remembering some elementary notions of the Poisson geometry.

2.1. Poisson Algebras and Poisson Manifold

Let be a commutative K-algebra. One says that is a Poisson algebra if is endowed with a Lie bracket, indicated with {·, ·}, which is also a biderivation. One can also say that is endowed with a Poisson structure, and therefore, the bracket {·, ·} is called the Poisson bracket. Elements of the center are called Casimirs: a is a Casimir if {a, b} = 0 for all b.

A Poisson manifold M (smooth, algebraic, etc.) is a manifold whose function algebra 𝒜 (C(M), regular, etc.) is endowed with a Poisson bracket.

As examples of Poisson structures let us consider a particular subclass of Poisson structures which are uniquely characterized by their Casimirs. In the dimension 4, let
()
be two elements of [x0, x1, x2, x3], where k.
On [x0, x1, x2, x3], a Poisson structure π is defined by
()
or more explicitly (mod 4)
()
Sklyanin had introduced this Poisson algebra which carries today his name in a Hamiltonian approach to the continuous and discrete integrable Landau-Lifshitz models [10, 11]. He showed that the Hamiltonian structure of the classical model is completely determined by two quadratic “Casimirs”. The Sklyanin Poisson algebra is also called elliptic due to its relations with an elliptic curve. The elliptic curve enters in the game from the geometric side. The symplectic foliation of Sklyanin′s structure is too complicated. This is because the structure is degenerated and looks quite different from a symplectic one. But the intersection locus of two Casimirs in the affine space of dimension four (one can consider also the projective situation) is an elliptic curve given by two quadrics q1,2. We can think about this curve as a complete intersection of the couple q1 = 0, q2 = 0 embedded in 𝒞P3 (as it was observed in Sklyanin′s initial paper).
A possible generalization one can be obtained considering n − 2 polynomials Qi in Kn with coordinates xi, i = 0, …, n − 1. We can define a bilinear differential operation
()
by
()
This operation, which gives a Poisson algebra structure on K[x1, …, xn], is called a Jacobian Poisson structure (JPS), and it is a partial case of more general nm-ary Nambu operation given by an antisymmetric nm-polyvector field introduced by Nambu [6] and was extensively studied by Takhtajan [5].

The polynomials Qi,  i = 1, …, n − 2 are Casimir functions for the brackets (2.5).

There exists a second generalization of the Sklyanin algebra that we will describe briefly in the next subsection (see, for details, [4]).

2.2. Elliptic Poisson Algebras qn(, η) and qn,k(, η)

(We report here this subsection from [2] for sake of self-consistency).

These algebras, defined by Feĭgin and Odesskiĭ, arise as quasiclassical limits of elliptic associative algebras Qn(, η) and Qn,k(, η) [12, 13].

Let Γ = + τ be an integral lattice generated by 1 and τ, with Imτ > 0. Consider the elliptic curve = /Γ and a point η on this curve.

In their article [13], given k < n, mutually prime, Odesskiĭ and Feĭgin construct an algebra, called elliptic, Qn,k(, η), as an algebra defined by n generators {xi, i/n} and the following relations:
()
where θα are theta functions [13].
These family of algebras has the following properties:
  • (1)

    the center of the algebra Qn,k(, η), for generic and η, is the algebra of polynomial of m = pgcd(n, k + 1) variables of degree n/m,

  • (2)

    Qn,k(, 0) = [x1, …, xn] is commutative,

  • (3)

    Qn,n−1(, η) = [x1, …, xn] is commutative for all η,

  • (4)

    , if kk ≡ 1 (mod n),

  • (5)

    the maps xixi+1 et xiɛixi, where ɛn = 1, define automorphisms of the algebra Qn,k(, η),

  • (6)

    the algebras Qn,k(, η) are deformations of polynomial algebras. The associated Poisson structure is denoted by qn,k(, η),

  • (7)

    among the algebras qn,k(, η), only q3(, η) (the Artin-Schelter-Tate algebra) and the Sklyanin algebra q4(, η) are Jacobian Poisson structures.

2.3. The Heisenberg Invariant Poisson Structures

2.3.1. The G-Invariant Poisson Structures

Let G be a group acting on a Poisson algebra .

Definition 2.1. A Poisson bracket {·, ·} on is said to be a G-invariant if G acts on by Poisson automorphisms.

In other words, for every gG, the morphism φg : , ag · a is an automorphism and the following diagram is a commutative:

image

()

2.3.2. The H-Invariant Poisson Structures

In their paper [2], the authors introduced the notion of H-invariant Poisson structures. That is, a special case of a G-invariant structure when G in the finite Heisenberg group and is the polynomial algebra. Let us remember this notion.

Let V be a complex vector space of dimension n and e0, …, en−1 a basis of V. Take the nth primitive root of unity ɛ = e2πi/n.

Consider σ, τ of GL(V) defined by
()
The Heisenberg of dimension n is nothing else that the subspace HnGL(V) generated by σ and τ.

From now on, we assume that V = n, with x0, x1, …, xn−1 as a basis and consider the coordinate ring [x0, x1, …, xn−1].

Naturally, σ and τ act by automorphisms on the algebra [x0, x1, …, xn−1] as follows:
()
We introduced in [2] the notion of τ-degree on the polynomial algebra [x0, x1, …, xn−1]. The τ-degree of a monomial is the positive integer α1 + 2α2 + ⋯+(n − 1)αn−1/n if α ≠ 0 and − if not. The τ-degree of M is denoted τϖ(M). A τ-degree of a polynomial is the highest τ-degree of its monomials.
For simplicity, the Hn-invariance condition will be referred from now on just as H-invariance. An H-invariant Poisson bracket on 𝒜 = [x0, x1, …, xn−1] is nothing but a bracket on 𝒜 which satisfy the following:
()
for all i, j/n.

The τ invariance is, in some sense, a “discrete” homogeneity.

Proposition 2.2 (see [2].)The Sklyanin-Odesskii-Feigin Poisson algebras qn,k() are H-invariant Poisson algebras.

Therefore, an H-invariant Poisson structures on the polynomial algebra includes as the Sklyanin Poisson algebra or more generally of the Odesskii-Feigin Poisson algebras.

In this paper, we are interested in the intersection of the two classes of generalizations of Artin-Shelter-Tate-Sklyanin Poisson algebras: JPS and H-invariant Poisson structures.

Proposition 2.3 (see [2].)If {·, ·} is an H-invariant polynomial Poisson bracket, the usual polynomial degree of the monomial of {xi, xj} equals to 2 + sn,  s.

Proposition 2.4 (see [2].)Let P = [x0, …, xn−1].

For all i ∈ {0, …, n − 1},

()

3. H-Invariant JPS in Dimension 3

We consider first a generalization of Artin-Schelter-Tate quadratic Poisson algebras. Let = [x0, x1, x2] be the polynomial algebra with 3 generators. For every P𝒜, we have a JPS π(P) on given by
()
where (i, j, k) ∈ /3 is a cyclic permutation of (0,1, 2). Let be the set of all P𝒜 such that π(P) is an H-invariant Poisson structure.

Proposition 3.1. If P is a homogeneous polynomial, then σ · P = P and τϖ(P) = 0.

Proof. Let (i, j, k)∈(/3) 3 be a cyclic permutation of (0,1, 2). One has

()
()
Using Proposition 2.4, we conclude that for all m/3,  σP/xm = P/xm.

It gives that σ · P = P.

On the other hand, from (3.2), one has τϖ(P) ≡ i + j + kmod 3. And we get the second half of the proposition.

Proposition 3.2. is a subalgebra of .

Proof. Let P, Q. It is clear that for all α, β,  αP + βQ belongs to .

Let us denote by {·, ·} F the JPS associated with the polynomial F. It is easy to verify that {xi, xj} PQ = P{xi, xj} Q + Q{xi, xj} P. Therefore, it is clear that the H-invariance condition is verified for the JPS associated to the polynomial PQ.

We endow with the usual grading of the polynomial algebra . For F, an element of , we denote by ϖ(F) its usual weight degree. We denote by i the homogeneous subspace of of degree i.

Proposition 3.3. If 3 does not divide i (in other words i ≠ 3k), then i = 0.

Proof. First of all 0 = . We suppose now that i ≠ 0. Let Pi,   P ≠ 0. Then, ϖ(P) = i. It follows from Proposition 2.3 and the definition of the Poisson brackets that there exists s such that ϖ(xi, xj) = 2 + 3s. The result follows from the fact that ϖ(xi, xj) = ϖ(P) − 1.

Set , where . We suppose that ϖ(P) = 3(1 + s). We want to find all α0, α1, α2 such that P and, therefore, the dimension 3(1+s) as -vector space.

Proposition 3.4. There exist s, s′′, and s′′′ such that

()

Proof. This is a direct consequence of Proposition 3.3.

Proposition 3.5. The system equation (3.4) has as solutions the following set:

()
where r = 1 + s,  s and s′′ live in the polygon given by the following inequalities in 2:
()

Remark 3.6. For r = 1, one obtains the Artin-Schelter-Tate Poisson algebra which is the JPS given by the Casimir ,  α, β. Suppose that α ≠ 0, then it can take the form

()
where γ. The interesting feature of this Poisson algebra is that their polynomial character is preserved even after the following nonalgebraic changes of variables. Let
()
The polynomial P in the coordinates (y0; y1; y2) has the form
()
The Poisson bracket is also polynomial (which is not evident at all!) and has the same form
()
where (i, j, k) is the cyclic permutation of (0,1, 2). This JPS structure is no longer satisfying the Heisenberg invariance condition. But it is invariant with respect the following toric action: (*) 3 × 2 given by
()

Put deg y0 = 2;   deg y2 = 1;   deg y2 = 3. Then, the polynomial is also homogeneous in (y0; y1; y2) and defines an elliptic curve in the weighted projective space 𝕎P2;1;3.

The similar change of variables

()
defines the JPS structure invariant with respect to the torus action (*) 3 × 2 given by
()
and related to the elliptic curve in the weighted projective space 𝕎P1;1;2.

These structures had appeared in [1], their Poisson cohomology was studied by Pichereau [14], and their relation to the noncommutative del Pezzo surfaces and Calabi-Yau algebras were discussed in [15].

Proposition 3.7. The subset of 2 given by the system (3.6) is a triangle 𝒯r with (0, r),  (r, 2r), and (2r, 0) as vertices. Then,   dim 3r = Card(𝒯r2).

Remark 3.8. For r = 2, the case of Figure 1, the generic Heisenberg-invariant JPS is given by the sextic polynomial

()
The corresponding Poisson bracket takes the form
()
where i, j, k are the cyclic permutations of 0,1, 2.

This new JPS should be considered as the “projectively dual” to the Artin-Schelter-Tate JPS, since the algebraic variety : P = 0 is generically the projective dual curve in 2 to the elliptic curve

()

To establish the exact duality and the explicit values of the coefficients, we should use (see [16, chapter 1]) Schläfli′s formula for the dual of a smooth plane cubic = 0 ⊂ 2. The coordinates of a point satisfies to the sextic relation = 0 if and only if the line x0p0 + x1p1 + x2p2 = 0 is tangent to the conic locus 𝒞(x, p) = 0, where

()

Set 𝒮r = 𝒯r2.  , and .  .

Details are in the caption following the image
An example of the triangle 𝒯2 in the case r = 2.

Proposition 3.9.

()

Proof. Let α ∈ {0, …, r}, and set . Therefore,

()
Let
()
.

It is easy to prove that

()
The result follows from the summation of all .

Proposition 3.10.

()

Proof. Let α ∈ {r + 1, …, 2r}, and set . Therefore,

()
Let
()
.

It is easy to prove that

()
The result follows from the summation of all ,  α ∈ {r + 1, …, 2r}.

Theorem 3.11.

()

Proof. This result is a direct consequence of Propositions 3.9 and 3.10.

Corollary 3.12. The Poincaré series of the algebras is

()

Remark 3.13. For r = 2, the case of Figure 1, our formula gives the same answer like the classical Pick′s formula for integer points in a convex polygon Π with integer vertices on the plane ([17, chapter 10])

()
Here, s = 1 and dim 3(1+1) = 10. In other hand the Pick′s formula ingredients are
()
hence 6 + 3 + 1 = 10.

This remark gives a good hint how one can use the developed machinery of integer points computations in rational polytopes to our problems.

4. H-Invariant JPS in Any Dimension

In order to formulate the problem in any dimension, let us remember some number theoretic notions concerning the enumeration of nonnegative integer points in a polytope or more generally discrete volume of a polytope.

4.1. Enumeration of Integer Solutions to Linear Inequalities

In their papers [18, 19], the authors study the problem of nonnegative integer solutions to linear inequalities as well as their relation with the enumeration of integer partitions and compositions.

Define the weight of a sequence λ = (λ0, λ2, …, λn−1) of integers to be |λ | = λ0 + ⋯+λn−1. If sequence λ of weight N has all parts nonnegative, it is called a composition of N; if, in addition, λ is a nonincreasing sequence, we call it a partition of N.

Given an r × n integer matrix C = [ci,j],  (i, j)∈({−1} ∪ /r) × /n, consider the set SC of nonnegative integer sequences λ = (λ1, λ2, …, λn) satisfying the constraints
()
The associated full generating function is defined as follows:
()
This function “encapsulates” the solution set SC: the coefficient of qN in FC(qx0, qx1, …, qxn−1) is a “listing” (as the terms of a polynomial) of all nonnegative integer solutions to (4.1) of weight N, and the number of such solutions is the coefficient of qN in FC(q, q, …, q).

4.2. Formulation of the Problem in Any Dimension

Let = [x0, x1, …, xn−1] be the polynomial algebra with n generators. For given n − 2 polynomials P1, P2, …, Pn−2, one can associate the JPS π(P1, …, Pn−2) on given by
()
for f, g.

We will denote by P the particular Casimir of the Poisson structure π(P1, …, Pn−2). We suppose that each Pi is homogeneous in the sense of τ-degree.

Proposition 4.1. Consider a JPS π(P1, …, Pn−2) given by homogeneous (in the sense of τ-degree) polynomials P1, …, Pn−2. If π(P1, …, Pn−2) is H-invariant, then

()
where P = P1P2Pn−2.

Proof. Let i < j/n, and consider the set Ii,j, formed by the integers i1 < i2 < ⋯<in−2/n∖{i, j}. We denote by Si,j the set of all permutation of elements of Ii,j. We have

()
From the τ-degree condition,
()

We can deduce, therefore, that

()
And we obtain the first part of the result. The second part is the direct consequence of facts that
()
α(i1) + 1 ≠ ⋯≠α(in−2) + 1 ∈ Z/n∖{i + 1, j + 1} and the τ-degree condition.

Set
()
Let be the set of all Q such that τϖ(σ · Q) = τϖ(Q) = l. One can easily check the following result.

Proposition 4.2. is a subvector space of . It is subalgebra of if l = 0.

We endow with the usual grading of the polynomial algebra . For Q, an element of , we denote by ϖ(Q) its usual weight degree. We denote by i the homogeneous subspace of of degree i.

Proposition 4.3. If n is not a divisor of i (in other words, inm) then i = 0.

Proof. It is clear the 0 = . We suppose now that i ≠ 0. Let Qi,  Q ≠ 0. Then,

()
Hence,
()
Since τϖ(σ · Q) = τϖ(Q) = l,  i ≡ 0  modulo  n.

Set . We suppose that ϖ(Q) = n(1 + s). We want to find all α0, α1, …, αn−1 such that Q and, therefore, the dimension 3(1+s) as -vector space.

Proposition 4.4. There exist s0, s1, …, sn−1 such that

()

Proof. That is, the direct consequence of the fact that τϖ(σ · Q) = τϖ(Q) = l.

One can easily obtain the following result.

Proposition 4.5. The system equation (4.12) has as a solution

()
where r = s + 1 and the s0, …, sn−1 satisfy the condition
()

Therefore α0, α1, …, αn−1 are completely determined by the set of nonnegative integer sequences (s0, s1, …, sn−1) satisfying the constraints
()
and such that
()
There are two approaches to determine the dimension of nr.

The first one is exactly as in the case of dimension 3. The constraint (4.16) is equivalent to say that

()
Therefore, by replacing sn−1 by this value, α0, …, αn−1 are completely determined by the set of nonnegative integer sequences (s0, s1, …, sn−2) satisfying the constraints
()
Hence, the dimension nr is just the number of nonnegative integer points contained in the polytope given by the system (4.18), where r = s + 1.

In dimension 3, one obtains the triangle in 2 given by the vertices A(0,2r), B(r, 2r),   and C(2r, 0) (see Section 3).

In dimension 4, we get the following polytope (see Figure 2).

Details are in the caption following the image
An example of the polytope T4 in the case r = 4. The vertices are in (−1/2, r − 1/2, 2r − 1/2), (r − 2/3, 2r − 2/3, 3r − 2/3), (r, 2r − 1,3r − 1), (r, 2r, 3r − 2), (2r − 1/2, 3r − 1/2, −1/2), and (3r − 1/2, −1/2, r − 1/2).
For the second method, one can observe that the dimension of nr is nothing else that the cardinality of the set SC of all compositions (s0, …, sn−1) of N = ((n − 1)n/2)rl subjected to the constraints (4.15). Therefore, if SC is the set of all nonnegative integers (s0, …, sn−1) satisfying the constraints (4.15) and FC is the associated generating function, then the dimension of nr is the coefficient of qN in FC(q, q, …, q).The set SC consists of all nonnegative integers points contained in the polytope of n
()

(See Figure 3).

Details are in the caption following the image
An example of the polytope 𝒫3 in the case r = 2.

Acknowledgments

The authors are grateful to M. Beck and T. Schedler for useful and illuminative discussions. This work has begun when G. Ortenzi was visiting Mathematics Research Unit at Luxembourg. G. Ortenzi thanks this institute for the invitation and for the kind hospitality. A Part of this work has been done when S. R. T. Pelap: was visiting Max Planck Institute at Bonn. S. R. T. Pelap thanks this institute for the invitation and for good working conditions. S. R. T. Pelap have been partially financed by “Fond National de Recherche (Luxembourg)”. He is thankful to LAREMA for a kind invitation and a support during his stay in Angers. V. Rubtsov was partially supported by the French National Research Agency (ANR) Grant no. 2011 DIADEMS and by franco-ukrainian PICS (CNRS-NAS) in Mathematical Physics. He is grateful to MATPYL project for a support of T. Schedler visit in Angers and to the University of Luxembourg for a support of his visit to Luxembourg.

      The full text of this article hosted at iucr.org is unavailable due to technical difficulties.