Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems
We consider trigonometric solutions of WDVV equations and derive geometric conditions when a collection of vectors with multiplicities determines such a solution. We incorporate these conditions into the notion of trigonometric Veselov system (∨-system) and we determine all trigonometric ∨-systems w...
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| Cite this: | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems / M.V. Feigin // Symmetry, Integrability and Geometry: Methods and Applications. — 2009. — Т. 5. — Бібліогр.: 16 назв. — англ. |
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| citation_txt | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems / M.V. Feigin // Symmetry, Integrability and Geometry: Methods and Applications. — 2009. — Т. 5. — Бібліогр.: 16 назв. — англ. |
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| description | We consider trigonometric solutions of WDVV equations and derive geometric conditions when a collection of vectors with multiplicities determines such a solution. We incorporate these conditions into the notion of trigonometric Veselov system (∨-system) and we determine all trigonometric ∨-systems with up to five vectors. We show that generalized Calogero-Moser-Sutherland operator admits a factorized eigenfunction if and only if it corresponds to the trigonometric ∨-system; this inverts a one-way implication observed by Veselov for the rational solutions.
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Symmetry, Integrability and Geometry: Methods and Applications SIGMA 5 (2009), 088, 10 pages
Trigonometric Solutions of WDVV Equations
and Generalized Calogero–Moser–Sutherland Systems
Misha V. FEIGIN
Department of Mathematics, University of Glasgow, G12 8QW, UK
E-mail: M.Feigin@maths.gla.ac.uk
URL: http://www.maths.gla.ac.uk/∼mf/
Received May 18, 2009, in final form September 07, 2009; Published online September 17, 2009
doi:10.3842/SIGMA.2009.088
Abstract. We consider trigonometric solutions of WDVV equations and derive geometric
conditions when a collection of vectors with multiplicities determines such a solution. We
incorporate these conditions into the notion of trigonometric Veselov system (∨-system) and
we determine all trigonometric ∨-systems with up to five vectors. We show that generali-
zed Calogero–Moser–Sutherland operator admits a factorized eigenfunction if and only if it
corresponds to the trigonometric ∨-system; this inverts a one-way implication observed by
Veselov for the rational solutions.
Key words: Witten–Dijkgraaf–Verlinde–Verlinde equations, ∨-systems, Calogero–Moser–
Sutherland systems
2000 Mathematics Subject Classification: 35Q40; 52C99
1 Introduction
In this note we are interested in the special trilogarithmic solutions of the generalized Witten–
Dijkgraaf–Verlinde–Verlinde (WDVV) equations [1]. Such solutions are determined by a finite
collection A of covectors α with multiplicities cα. More specifically, the prepotential satisfying
the WDVV equations has the form
F =
∑
α∈A
cαLi3
(
e2iα(x)
)
+ cubic terms, (1)
where Li3 is the trilogarithm function. Solution of this type for the An root system appeared
in [2] in relation with Seiberg–Witten theory. More systematically such solutions were studied
by Hoevenaars and Martini in [3, 4] who determined solutions for all irreducible reduced root
systems [4]. More recently solutions of the form (1) were derived from reductions of Egorov
hydrodynamic chains in [5].
The rational versions of solutions (1) play an important role in the theory of Frobenius
manifolds, a geometric framework for the WDVV equations [6]. Thus solutions corresponding
to the Coxeter root systems are almost dual to the Frobenius structures on the orbit spaces of
finite Coxeter groups [7]. In the trigonometric case such a duality is verified for the affine An
case in [8, 9]. The study of general rational solutions of the form
F =
∑
α∈A
α(x)2 logα(x) (2)
was initiated by Veselov in [10] where a geometric notion of the ∨-system equivalent to the
WDVV equations for (2) was introduced. It was shown in [11] that any generalized Calogero–
Moser–Sutherland (CMS) operator admitting a factorized eigenfunction determines a ∨-system.
mailto:M.Feigin@maths.gla.ac.uk
http://www.maths.gla.ac.uk/~mf/
http://dx.doi.org/10.3842/SIGMA.2009.088
2 M.V. Feigin
In this note we are interested in the solutions (1) where the cubic terms involve extra variable
like in the works [3, 4] on the solutions for the root systems. We derive geometric and algebraic
conditions for a system of vectors with multiplicities so that the corresponding function (1)
satisfies the WDVV equations. These conditions should be thought of as trigonometric analogue
of the notion of the ∨-system. The conditions carry rather strong geometrical restrictions on
the collection of vectors formulated in terms of series of vectors parallel to a chosen one. We
illustrate this by determining all trigonometric ∨-systems with up to five vectors in the plane.
Trigonometric ansatz, in contrast to the rational one, allows to define the generalized CMS
operator corresponding to the solution (1). We show that this operator has a factorized eigen-
function. This statement inverts the one for the rational ∨-systems obtained in [11]. In fact
our arguments follow [11] very closely. We also discuss additional condition needed to have
trigonometric solution to the WDVV equations starting from a CMS operator with factorized
eigenfunction.
2 Trigonometric ∨-systems
Consider a function F of the form
F =
1
3
y3 +
∑
α∈A
cαα(x)2y + λ
∑
α∈A
cαf(α(x)), (3)
where A is a finite collection of covectors on V ∼= Cn, x = (x1, . . . , xn), cα, λ are non-zero
constants and function f(x) satisfies f ′′′(x) = cotx. The last equation fixes function f(x) up
to 2nd order terms which will not be important for the WDVV equations below. We may fix
a choice of f(x) by
f(x) =
1
6
ix3 +
1
4
Li3
(
e−2ix
)
.
The ansatz (3) introducing extra variable y was proposed in [4] in the case of root systems
A = R. The form (3) guarantees that the matrix of third derivatives involving y is constant, as
we will explore below.
We will assume throughout the paper that collection A of covectors α belongs to an n-dimen-
sional lattice, and that the bilinear form
(u, v) :=
∑
α∈A
cαα(u)α(v) (4)
is non-degenerate on V . The form (·, ·) identifies V and V ∗ and following [10] we will denote
by γ∨ the vector dual to the covector γ. We will also denote through (·, ·) the corresponding
inner product on V ∗. We are interested in the conditions on {α, cα, λ} when function F satisfies
the WDVV equations
FiF
−1
k Fj = FjF
−1
k Fi, (5)
i, j, k = 0, 1, . . . , n. Here Fi are (n+ 1)× (n+ 1) matrices of third derivatives in the coordinates
(x0 = y, x1, . . . , xn), (Fi)ab = ∂3F
∂xi∂xa∂xb
. It is sufficient to fix k = 0, then F0 = Fy is the
following non-degenerate matrix
Fy = 2
(
1 0
0
∑
α∈A
cαα⊗ α
)
.
Trigonometric Solutions of WDVV Equations and Generalized CMS Systems 3
Similarly
Fi =
0 2
∑
α∈A
cααiα
2
∑
α∈A
cααiα λ
∑
α∈A
cααi cotα(x)α⊗ α
,
where we denoted by α both column and row vectors α = (α1, . . . , αn).
The WDVV conditions for a function F can be reformulated partly using geometry of the
system A. For any α ∈ A let us collect all the covectors from A non-parallel to α into the
disjoint union of ααα-series Γ1
α, . . . ,Γ
k
α. These series are determined by the property that for any
s = 1, . . . , k and for any two covectors γ1, γ2 ∈ Γs
α one has either γ1 − γ2 = nα or γ1 + γ2 = nα
for some integer n. We also assume that the series are maximal, that is if β ∈ Γi
α then Γi
α must
contain all the vectors of the form ±β + nα ∈ A with n ∈ Z.
We note that solution (3) is not affected if some of the covectors α ∈ A are replaced with −α.
By appropriate choice of signs the vectors can be made to belong to a half-space, we will denote
such systems as A+. Moreover, for any α ∈ A one can choose a positive system A+ 3 α in such
a way that α-series Γs
α will consist of vectors of the form βs + niα ∈ A+ for appropriate integer
parameters ni with βs ∈ A+.
Definition 1. Let A ⊂ V ∗ ∼= Cn be a finite collection of covectors α with multiplicities cα
such that the corresponding form (4) is non-degenerate and the covectors α belong to an n-
dimensional lattice. We say that A is a trigonometric ∨-system if for any α ∈ A and for any
α-series Γs
α one has∑
β∈Γs
α
cβ(α, β)α ∧ β = 0. (6)
Notice that α∧β1 = ±α∧β2 if β1, β2 belong to the same α-series Γs
α so identities (6) may be
simplified accordingly. Also replacement of some of the covectors by their opposite preserves the
class of trigonometric ∨-systems. Note also that the non-degenerate linear transformations act
naturally on the trigonometric ∨-systems, and that the direct sum A1⊕A2 of the trigonometric
∨-systems A1 ⊂ V ∗
1 , A2 ⊂ V ∗
2 considered as a set of covectors in V1⊕V2 is again a trigonometric
∨-system. The systems obtained in this way will be called reducible. If such a decomposition is
not possible then the (trigonometric ∨-)system is called irreducible.
Theorem 1. The WDVV equations
FiF
−1
y Fj = FjF
−1
y Fi,
i, j = 0, 1, . . . , n, for the function (3) are equivalent to the following two conditions:
1) A is a trigonometric ∨-system;
2) for a positive system A+ and for any vectors a, b, c, d ∈ V∑
α,β∈A+
(
1
4
λ2(α, β)− 1
)
cαcβBα,β(a, b)Bα,β(c, d) = 0, (7)
where Bα,β(a, b) = α ∧ β(a, b) = α(a)β(b)− α(b)β(a).
Proof. For a vector a ∈ V we define F∨a = F−1
y Fa where Fa =
n∑
i=1
aiFi. The WDVV equations
are equivalent to the commutativity [F∨a , F
∨
b ] = 0 for any a, b ∈ V . We have
F∨i =
0
∑
α∈A
cααiα∑
α∈A
cααiα
∨ λ
2
∑
α∈A
cααi cotα(x)α⊗ α∨
,
4 M.V. Feigin
where α∨ is the (column) vector dual to the (row) covector α under the bilinear form G =∑
α∈A
cαα⊗ α. Therefore
F∨a =
0
∑
α∈A
cαα(a)α∑
α∈A
cαα(a)α∨ λ
2
∑
α∈A
cαα(a) cotα(x)α⊗ α∨
for any a ∈ Cn. Now the product F∨a F
∨
b equals
∑
α,β∈A
cαcβα(a)β(b)α(β∨) λ
2
∑
α,β∈A
cαcβα(a)β(b)α(β∨) cotβ(x)β
λ
2
∑
α,β∈A
cβcαα(a)β(b)α(β∨) cotα(x)α∨
∑
α,β∈A
cαcβα(a)β(b)α∨⊗β
+λ2
4
∑
α,β∈A
cαcβα(a)β(b)α(β∨) cot α(x) cot β(x)β⊗α∨
.
Therefore [F∨a , F
∨
b ] = 0 is equivalent to the identities∑
α,β∈A
cαcβBα,β(a, b)(α, β) cotα(x)α∨ = 0, (8)
∑
α,β∈A
(
λ2
4
cαcβ(α, β) cotα(x) cotβ(x) + cαcβ
)
Bα,β(a, b)α ∧ β = 0. (9)
To cancel singularities in (9) one should have∑
β∈A
β�α
cβ(α, β) cotβ(x)Bα,β(a, b)α ∧ β = 0
when cotα(x) = 0. A linear combination of functions cotβ(x)|cot α(x)=0 can vanish only if it
vanishes for each α-series:∑
β∈Γs
α
cβ(α, β) cotβ(x)Bα,β(a, b)α ∧ β = 0
for all α-series Γs
α (see e.g. [14] for more detailed explanation). The last relation can be sim-
plified as∑
β∈Γs
α
cβ(α, β)α ∧ β = 0, (10)
which means that A is a trigonometric ∨-system. Identities (10) guarantee that the left-hand side
of (9) is non-singular. Since all the vectors from A belong to an n-dimensional lattice with basis
e1, . . . , en, the left-hand side of (9) is a rational function in the exponential coordinates ee
i(x).
This rational function has degree zero and therefore it is a constant. We can assume that all
covectors from A belong to a half-space hence form a positive system A+, so in appropriate limit
cot(α, x) → i for all α ∈ A+. Thus property (9) is equivalent to (10) together with the condition∑
α,β∈A+
(
λ2
4
cαcβ(α, β)− cαcβ
)
Bα,β(a, b)α ∧ β = 0.
The remaining condition (8) is equivalent to the set of properties∑
β∈A
cβ(α, β)Bα,β(a, b) = 0, (11)
for any α ∈ A. Identities (11) follow from the ∨-conditions (10), this completes the proof of the
theorem. �
Trigonometric Solutions of WDVV Equations and Generalized CMS Systems 5
Remark 1. Let trigonometric ∨-systems A1 ⊂ V ∗
1 , A2 ⊂ V ∗
2 define the solutions (3) of the
WDVV equations for some λ1, λ2. Then the trigonometric ∨-system A1 ⊕ A2 does not define
a solution. Indeed, let us take vectors a, c ∈ V1 and b, d ∈ V2. Then property (7) implies that
(a, c)1(b, d)2 = 0, (12)
where (·, ·)1,2 are ∨-forms (4) in the corresponding spaces V1,2. Clearly, the relation (12) does
not hold for general vectors a, b, c, d.
Remark 2. Not all the trigonometric solutions of the WDVV equations have the form (3).
It is shown in [15] that trilogarithmic functions have to arise when ansatz for F is given by
summation of g((α, x)) over the roots of a root system, x ∈ V .
Remark 3. A slightly more general ansatz for the solutions F can be considered when cubic
terms in x are added to F . Similarly to the proof of Theorem 1 it follows that A still has to
be a trigonometric ∨-system. The almost dual potentials corresponding to the An affine Weyl
group orbit spaces have such a form [9]. The corresponding trigonometric ∨-system A is the An
root system in this case.
Proposition 1. Let A = {α, cα} be a trigonometric ∨-system. Then the set of vectors {√cαα}
is a (rational) ∨-system, that is F rat =
∑
α∈A
cαα(x)2 logα(x) is a solution of the WDVV equations
in the space V .
Proof. By definition of the trigonometric ∨-system for any α ∈ A relations (6) hold. Consider
two-dimensional plane π ⊂ V and sum up relations (6) over s so that the α-series Γs
α belong to
the plane π 3 α. We arrive at the relations∑
β∈A∩π
cβ(α, β)α ∧ β = 0,
or, equivalently,∑
β∈A∩π
cβ(α, β)β is proportional to α. (13)
Relations (13) is a definition of the (rational) ∨-system for the set of covectors {√cαα} (see [10]
and [13] for the complex space). It is equivalent to the property that F rat satisfies WDVV
equations in the space V [10, 13]. Proposition is proven. �
Due to existence of extra variable y in the ansatz (3) the WDVV equations are nontrivial al-
ready when n = 2. Thus it is natural to study at first two-dimensional configurations A defining
solutions of WDVV equations. When A consists of one vector the corresponding form (4) is de-
generate. If A consists of two non-collinear vectors α, β then it follows that (α, β) = 0 therefore
relation (6) holds and A is a trigonometric ∨-system. However relation (7) cannot hold then for
any λ and therefore a pair of vectors does not define a solution to WDVV equations (see also
Remark 1 above). The following propositions deal with the next simplest cases when A consists
of 3, 4 and 5 vectors respectively. In fact all irreducible trigonometric ∨-systems with up to 5
covectors have to be two-dimensional.
Proposition 2. Let system A consist of three vectors α, β, γ with nonzero multiplicities cα,
cβ, cγ. Then A is an irreducible trigonometric ∨-system iff α ± β ± γ = 0 for some choice of
signs. The non-degeneracy condition for the form (4) is then given by cαcβ + cαcγ + cβcγ 6= 0.
Any such system A defines the solution (3) of the WDVV equations with λ = 2(cαcβ + cαcγ +
cβcγ)(cαcβcγ)−1/2.
6 M.V. Feigin
Proof. It follows from relations (6) that γ = α+ β up to multiplication of some of the vectors
by −1. We take a basis e1 = α, e2 = β in C2. The bilinear form (4) takes the form G =
cαx
2
1 + cβx
2
2 + cγ(x1 + x2)2. This form is non-degenerate iff cαcβ + cαcγ + cβcγ 6= 0. One can
check that
e1
∨ =
(cβ + cγ)e1 − cγe2
cαcβ + cαcγ + cβcγ
, e2
∨ =
−cγe1 + (cα + cγ)e2
cαcβ + cαcγ + cβcγ
,
where e1, e2 is dual basis to e1, e2, that is ei(ej) = δi
j . Relations (6) look as follows(
e1
∨
, e2
∨)(cβ + cγ) +
(
e1
∨
, e1
∨)
cγ = 0,(
e1
∨
, e2
∨)(cα + cγ) +
(
e2
∨
, e2
∨)
cγ = 0,(
e1
∨
, e2
∨)(cα − cβ) +
(
e1
∨
, e1
∨)
cα −
(
e2
∨
, e2
∨)
cβ = 0,
and they are automatically satisfied. Relation (7) results to one scalar equation
λ2
4
(
cαcβ(α∨, β∨) + cαcγ(α∨, γ∨) + cβcγ(β∨, γ∨)
)
= cαcβ + cαcγ + cβcγ ,
which has solution as stated in the formulation. �
In the following proposition we study configurations consisting of four covectors.
Proposition 3. Let system A consist of four vectors α, β, γ, δ with nonzero multiplicities cα,
cβ, cγ, cδ. Then A is an irreducible trigonometric ∨-system iff the vectors in A+ take the form e1,
e2, e1±e2 in a suitable basis, and the corresponding multiplicities c1, c2, c± satisfy c1 = c2. This
property is equivalent to the orthogonality (e1+e2, e1−e2) = 0 under the corresponding ∨-product.
The non-degeneracy condition for the form (4) is then given by ∆ = (c1 + 2c+)(c1 + 2c−) 6= 0.
These systems A define the solutions (3) of the WDVV equations with λ = 2∆c−1/2
1 (4c+c−+
c1(c+ + c−))−1/2 once λ is finite.
Proof. It follows from the series relations (6) that there is a a vector α ∈ A such that all the
remaining vectors β, γ, δ ∈ A belong to single α-series Γ1
α.
Indeed, otherwise, up to renaming the covectors and taking opposite, we have δ = γ + nα,
n ∈ N, (α, β) = (γ, δ) = 0. Then consideration of β-series gives 2γ + nα = mβ for some m ∈ Z.
And consideration of γ-series gives α+pγ = ±β for some p ∈ Z. Therefore 2γ+nα = ±m(α+pγ),
hence n = ±m and 2 = ±mp, thus m = ±1 or p = ±1. In the case m = ±1 we have n = 1
hence γ-series contains δ together with α and β. And in the case p = ±1 the α-series contains β
together with γ and δ.
So we can assume that there is only one α-series so that the remaining vectors take the form
γ = β + n1α, δ = β + n2α with integer n2 > n1 > 0. By considering β-series we conclude that
n1 = 1. Consider now the δ-series. It is easy to see that covector β has to form a single series,
therefore (β, δ) = 0 and the covectors β + α and α belong to a δ-series. This is possible only
if n2 = 2. Taking now the basis vectors as e1 = α, e2 = β + α we conclude that the system A
consists of covectors e1, e2, e1 ± e2.
The bilinear form (4) takes now the form
G = c1x
2
1 + c2x
2
2 + c+(x1 + x2)2 + c−(x1 − x2)2
= (c1 + c+ + c−)x2
1 + (c2 + c+ + c−)x2
2 + 2(c+ − c−)x1x2,
which has determinant ∆ = c1c2 + (c1 + c2)(c+ + c−) + 4c+c−. Therefore(
e1, e1
)
= ∆−1(c2 + c+ + c−),
(
e2, e2
)
= ∆−1(c1 + c+ + c−),(
e1, e2
)
= ∆−1(c− − c+). (14)
Trigonometric Solutions of WDVV Equations and Generalized CMS Systems 7
Now we analyze the series relations (6). The orthogonality (e1 − e2, e1 + e2) = 0 is clearly
equivalent to the condition c1 = c2. Then the remaining conditions (6) on (e1 ± e2)-series are
automatically satisfied. The condition (6) for the e1-series has the form
c−
(
− e1 + e2, e1
)
+ c2
(
e2, e1
)
+ c+
(
e1 + e2, e1
)
= 0,
and it follows from the scalar products (14). The condition on the e2-series is also satisfied.
It is easy to check that relation (7) holds iff λ is as stated, hence proposition is proven. �
Proposition 4. Let irreducible trigonometric ∨-system A consist of five vectors with non-zero
multiplicities. Then in the appropriate basis A+ takes the form e1, 2e1, e2, e1 ± e2 and the
corresponding multiplicities c1, c̃1, c2, c± satisfy c+ = c− (equivalently, (e1, e2) = 0) and 2c̃1c2 =
c+(c1 − c2).
The form (4) is then non-degenerate when ∆ = (c1 + 4c̃1 + 2c+)(c2 + 2c+) 6= 0. The corre-
sponding solution of the WDVV equations has the form (3) with λ =
√
2∆(c2 + 2c+)−1/2(c1 +
4c̃1)−1/2c
−1/2
+ .
Proof is obtained by simple analysis of the series conditions (6). One can firstly establish
that A is two-dimensional. Then it is easy to see that A has to contain collinear vectors, and
the required form follows.
To conclude this section we present a few examples of trigonometric ∨-systems on the plane
with higher number of vectors. Recall firstly that the positive roots of the root system G2 can
be written as α, β, β +α, β + nα, β + (n+ 1)α, 2β + (n+ 1)α where n = 2. One can show that
for integer n > 2 the above vectors never form a trigonometric ∨-system, and that for n = 2 the
multiplicities have to satisfy cα = cβ+α = cβ+nα and cβ = c2β+(n+1)α = cβ+(n+1)α which is the
case of the G2 system.
There are though some possibilities to extend the G2 system. Firstly, one can show that
G2 ∪A2 where the system A2 consists of doubled short roots of G2, is a trigonometric ∨-system
for appropriate multiplicities. Secondly the following proposition takes place.
Proposition 5. Let A consist of the vectors e1, e2, 2e2, 1
2(e1 ± e2), 1
2(e1 ± 3e2) with the
corresponding nonzero multiplicities c1, c2, c̃2, a, b. Then A is a trigonometric ∨-system iff the
multiplicities satisfy the relations a = 3b, c2 = a+ 2c̃2, (2c1 + b)c2 = (c1 + 2b)a.
Note that in the limiting case c̃2 = 0 we recover the system G2 with special multiplicities.
An example of trigonometric ∨-system with yet higher number of vectors is given by vectors
e1, 2e1, e2, 2e2, e1 ± e2, e1 ± 2e2, 2e1 ± e2 where the multiplicities can be chosen appropriately.
3 Relations with generalized Calogero–Moser–Sutherland
systems
Relation between ∨-systems and the property of a Schrödinger operator of CMS type to have
a factorized eigenfunction was observed by Veselov in [11]. Namely, it was shown in [11] that if
an operator
L = −∆ +
∑
α∈A+
mα(mα + 1)(α, α)
sin2(α, x)
has a formal eigenfunction
ψ =
∏
α∈A+
sin−mα(α, x), Lψ = µψ,
8 M.V. Feigin
then F =
∑
α∈A+
mα(α, x)2 log(α, x) satisfies the WDVV equations. The following theorem es-
tablishes the converse statement in the case of trigonometric ∨-systems.
Theorem 2. Let A be a trigonometric ∨-system consisting of pairwise non-collinear covectors
α with multiplicities cα. Then Schrödinger operator
L = −∆ +
∑
α∈A
cα(cα + 1)(α, α)
sin2 α(x)
(15)
constructed by the metric (4) has the formal eigenfunction
ψ =
∏
α∈A
sin−cα α(x), Lψ = µψ. (16)
Proof. The property Lψ = µψ is equivalent to the identity∑
α 6=β
cαcβ(α, β) cotα(x) cotβ(x) = const. (17)
To establish the last identity it is sufficient to show that the left-hand side of (17) is non-singular.
In other words, we need to show that∑
β,β 6=α
cβ(α, β) cotβ(x) = 0 (18)
if cotα(x) = 0. The last properties are sufficient to check when summation is taken along
arbitrary α-series, then it is guaranteed by relation (6). This proves the theorem. �
Corollary 1. Assume that function (3) constructed by a set of pairwise non-collinear covec-
tors α with multiplicities cα satisfies the WDVV equations (5). Then relation (16) holds for the
Schrödinger operator (15).
Conversely, the property of a Schrödinger operator to have a factorized eigenfunction implies
that the corresponding vectors
√
cαα form a rational ∨-system [11]. This property is also
sufficient to obtain the trigonometric ∨-system, and the arguments are close to [11].
Theorem 3. Assume that the Schrödinger operator (15) has an eigenfunction (16). Then the
set A of vectors α with the multiplicities cα forms the trigonometric ∨-system.
Proof. From equation (16), (15) it follows identity (18) at cotα(x) = 0. Therefore for each
α-series Γs
α we have∑
β∈Γs
α
cβ(α, β)α ∧ β = 0. (19)
Let βw denote a vector dual to β with respect to the inner product (·, ·) involved in the
Schrödinger equation. By summing identities (19) along all the α-series we conclude that∑
β∈A
cββ(αw)βw is proportional to αw. (20)
Now we can decompose the space V = V1 ⊕ · · · ⊕ Vk so that the operator
∑
β∈A cββ ⊗ βw is
equal to constant µi on Vi. We can also assume that (Vi, Vj) = 0 if i 6= j. It follows from (20)
that G(·, ·)|Vi = µi(·, ·)|Vi . Therefore identities (19) imply∑
β∈Γs
α
cβα(β∨)α ∧ β = 0
which are identities (6) from the definition of the trigonometric ∨-systems. �
Trigonometric Solutions of WDVV Equations and Generalized CMS Systems 9
Corollary 2. Assume that the Schrödinger operator (15) has an eigenfunction (16). Assume
also that the system A is irreducible and that for some Λ and any a, b, c, d ∈ V the property∑
α,β∈A+
(Λ(α, β)− 1)cαcβBα,β(a, b)Bα,β(c, d) = 0 (21)
holds. Then the corresponding function (3) with appropriate λ satisfies the WDVV equations (5).
Remark 4. The previous corollary also holds for the reducible systems A if we replace the
Schrödinger equation metric (α, β) in (21) by the ∨-product α(β∨). In this case λ = 2
√
Λ.
4 Concluding remarks
Trigonometric ∨-systems require further investigations. It would be interesting to obtain almost
dual prepotentials for the Frobenius manifolds of the affine Weyl groups as well as for their dis-
criminants (cf. rational case [7, 12]). Comparison with a recent work on the elliptic solutions [16]
might also be interesting. We also hope that the series conditions would allow understanding
and eventually classification of the trigonometric ∨-systems. We hope to return to some of these
questions soon.
Acknowledgements
I am very grateful to L. Hoevenaars, A. Kirpichnikova, M. Pavlov, I. Strachan and A.P. Veselov
for useful and stimulating discussions. The work was partially supported by the EPSRC grant
EP/F032889/1, by European research network ENIGMA (contract MRTN-CT-2004-5652), by
PMI2 Project funded by the UK Department for Innovation, Universities and Skills for the
benefit of the Japanese Higher Education Sector and the UK Higher Education Sector.
References
[1] Marshakov A., Mironov A., Morozov A., WDVV-like equations in N = 2 SUSY Yang–Mills theory, Phys.
Lett. B 389 (1996), 43–52, hep-th/9607109.
[2] Marshakov A., Mironov A., Morozov A., More evidence for the WDVV equations in N = 2 SUSY Yang–Mills
theories, Internat. J. Modern Phys. A 15 (2000), 1157–1206, hep-th/9701123.
[3] Hoevenaars L.K., Martini R., On the WDVV equations in five-dimensional gauge theories, Phys. Lett. B
557 (2003), 94–104, math-ph/0212016.
[4] Martini R., Hoevenaars L.K., Trigonometric solutions of the WDVV equations from root systems, Lett.
Math. Phys. 65 (2003), 15–18, math-ph/0302059.
[5] Pavlov M., Explicit solutions of the WDVV equation determined by the “flat” hydrodynamic reductions of
the Egorov hydrodynamic chains, nlin.SI/0606008.
[6] Dubrovin B., Geometry of 2D topological field theories, in Integrable Systems and Quantum Groups (Mon-
tecatini Terme, 1993), Lecture Notes in Math., Vol. 1620, Springer, Berlin, 1996, 120–348, hep-th/9407018.
[7] Dubrovin B., On almost duality for Frobenius manifolds, in Geometry, Topology, and Mathematical
Physics, Amer. Math. Soc. Transl. Ser. 2, Vol. 212, Amer. Math. Soc., Providence, RI, 2004, 75–132,
math.DG/0307374.
[8] Riley A., Frobenius manifolds: caustic submanifolds and discriminant almost duality, Ph.D. Thesis, Hull
University, 2007.
[9] Riley A., Strachan I.A.B., A note on the relationship between rational and trigonometric solutions of the
WDVV equations, J. Nonlinear Math. Phys. 14 (2007), 82–94, nlin.SI/0605005.
[10] Veselov A.P., Deformations of the root systems and new solutions to generalised WDVV equations, Phys.
Lett. A 261 (1999), 297–302, hep-th/9902142.
http://arxiv.org/abs/hep-th/9607109
http://arxiv.org/abs/hep-th/9701123
http://arxiv.org/abs/math-ph/0212016
http://arxiv.org/abs/math-ph/0302059
http://arxiv.org/abs/nlin.SI/0606008
http://arxiv.org/abs/hep-th/9407018
http://arxiv.org/abs/math.DG/0307374
http://arxiv.org/abs/nlin.SI/0605005
http://arxiv.org/abs/hep-th/9902142
10 M.V. Feigin
[11] Veselov A.P., On generalizations of the Calogero–Moser–Sutherland quantum problem and WDVV equa-
tions, J. Math. Phys. 43 (2002), 5675–5682, math-ph/0204050.
[12] Feigin M.V., Veselov A.P., Logarithmic Frobenius structures and Coxeter discriminants, Adv. Math. 212
(2007), 143–162, math-ph/0512095.
[13] Feigin M.V., Veselov A.P., On the geometry of ∨-systems, in Geometry, Topology, and Mathematical
Physics, Amer. Math. Soc. Transl. Ser. 2, Vol. 224, Amer. Math. Soc., Providence, RI, 2008, 111–123,
arXiv:0710.5729.
[14] Feigin M.V., Bispectrality for deformed Calogero–Moser–Sutherland systems, J. Nonlinear Math. Phys. 12
(2005), suppl. 2, 95–136, math-ph/0503020.
[15] Braden H., Marshakov A., Mironov A., Morozov A., Seiberg–Witten theory for a non-trivial compactification
from five to four dimensions, Phys. Lett. B 448 (1999), 195–202, hep-th/9812078.
[16] Strachan I.A.B., Weyl groups and elliptic solutions of the WDVV equations, arXiv:0802.0388.
http://arxiv.org/abs/math-ph/0204050
http://arxiv.org/abs/math-ph/0512095
http://arxiv.org/abs/0710.5729
http://arxiv.org/abs/math-ph/0503020
http://arxiv.org/abs/hep-th/9812078
http://arxiv.org/abs/0802.0388
1 Introduction
2 Trigonometric -systems
3 Relations with generalized Calogero-Moser-Sutherland systems
4 Concluding remarks
References
|
| id | nasplib_isofts_kiev_ua-123456789-149132 |
| institution | Digital Library of Periodicals of National Academy of Sciences of Ukraine |
| issn | 1815-0659 |
| language | English |
| last_indexed | 2025-12-07T18:57:15Z |
| publishDate | 2009 |
| publisher | Інститут математики НАН України |
| record_format | dspace |
| spelling | Feigin, M.V. 2019-02-19T17:35:38Z 2019-02-19T17:35:38Z 2009 Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems / M.V. Feigin // Symmetry, Integrability and Geometry: Methods and Applications. — 2009. — Т. 5. — Бібліогр.: 16 назв. — англ. 1815-0659 2000 Mathematics Subject Classification: 35Q40; 52C99 https://nasplib.isofts.kiev.ua/handle/123456789/149132 We consider trigonometric solutions of WDVV equations and derive geometric conditions when a collection of vectors with multiplicities determines such a solution. We incorporate these conditions into the notion of trigonometric Veselov system (∨-system) and we determine all trigonometric ∨-systems with up to five vectors. We show that generalized Calogero-Moser-Sutherland operator admits a factorized eigenfunction if and only if it corresponds to the trigonometric ∨-system; this inverts a one-way implication observed by Veselov for the rational solutions. I am very grateful to L. Hoevenaars, A. Kirpichnikova, M. Pavlov, I. Strachan and A.P. Veselov for useful and stimulating discussions. The work was partially supported by the EPSRC grant EP/F032889/1, by European research network ENIGMA (contract MRTN-CT-2004-5652), by PMI2 Project funded by the UK Department for Innovation, Universities and Skills for the benefit of the Japanese Higher Education Sector and the UK Higher Education Sector. en Інститут математики НАН України Symmetry, Integrability and Geometry: Methods and Applications Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems Article published earlier |
| spellingShingle | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems Feigin, M.V. |
| title | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems |
| title_full | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems |
| title_fullStr | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems |
| title_full_unstemmed | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems |
| title_short | Trigonometric Solutions of WDVV Equations and Generalized Calogero-Moser-Sutherland Systems |
| title_sort | trigonometric solutions of wdvv equations and generalized calogero-moser-sutherland systems |
| url | https://nasplib.isofts.kiev.ua/handle/123456789/149132 |
| work_keys_str_mv | AT feiginmv trigonometricsolutionsofwdvvequationsandgeneralizedcalogeromosersutherlandsystems |