Journal of Nonlinear Mathematical Physics

Volume 25, Issue 3, July 2018, Pages 485 - 496

The number of independent Traces and Supertraces on the Symplectic Reflection Algebra H1,η(Γ ≀ SN)

Authors
S.E. Konstein
I.E. Tamm Department of Theoretical Physics, P.N. Lebedev Physical Institute, 53, Leninsky Prospect Moscow, 117924, Russia,konstein@lpi.ru
I.V. Tyutin
I.E. Tamm Department of Theoretical Physics, P.N. Lebedev Physical Institute, 53, Leninsky Prospect, Moscow, 117924, Russia Tomsk State Pedagogical University, Kievskaya St. 60, 634061 Tomsk, Russia,tyutin@lpi.ru
Received 28 November 2017, Accepted 27 March 2018, Available Online 6 January 2021.
DOI
10.1080/14029251.2018.1494768How to use a DOI?
Abstract

Symplectic reflection algebra H1,η(G) has a T(G)-dimensional space of traces whereas, when considered as a superalgebra with a natural parity, it has an S(G)-dimensional space of supertraces. The values of T(G) and S(G) depend on the symplectic reflection group G and do not depend on the parameter η.

In this paper, the values T(G) and S(G) are explicitly calculated for the groups G = Γ ≀ SN, where Γ is a finite subgroup of Sp(2, ℂ).

Copyright
© 2018 The Authors. Published by Atlantis and Taylor & Francis
Open Access
This is an open access article distributed under the CC BY-NC 4.0 license (http://creativecommons.org/licenses/by-nc/4.0/).

1. Introduction

Let V := ℂ2N, let GSp(2N, ℂ) be a finite group generated by symplectic reflections. In [11], it was shown that Symplectic Reflection Algebra H1,η(G) has T(G) independent traces, where T(G) is the number of conjugacy classes of elements without eigenvalue 1 belonging to the group GSp(2N) ⊂ End(V), and that the algebra H1,η(G), considered as a superalgebra with a natural parity, has S(G) independent supertraces, where S(G) is the number of conjugacy classes of elements without eigenvalue −1 belonging to GSp(2N) ⊂ End(V). Hereafter, speaking about spectrum, eigenvalues and eigenvectors, the rank of an element of the group algebra ℂ[G] of the group G, etc., we have in mind the representation of the group algebra ℂ[G] in the space V. Besides, we denote all the units in groups, algebras, etc., by 1, and c · 1 by c for any number c.

Apart from a few cases, there are two families of groups generated by symplectic reflections, see [7] and also [9], [2], [5]:

  • Family 1): G is a complex reflection group acting on 𝔥 ⊕ 𝔥*, where 𝔥 is the space of reflection representation. In this case, G is a direct product of several groups from the following set of Coxeter groups

    An(n1),Bn=Cn(n2),Dn(n3),E6,E7,E8,F4,G2,H3,H4,I2(n)(n5,n6).(1.1)

  • Family 2): G = Γ ≀ SN, which means here G = ΓNSN acting on (ℂ2)N, where Γ is a finite subgroup of Sp(2, ℂ).

For groups G from the set (1.1), the list of values T(G) and S(G) is given in [10].

In this work, we give the values of T(G) and S(G) for the 2nd family. Namely, we found the generating functions

t(Γ,x):=N=0T(ΓSN)xN,(1.2)
s(Γ,x):=N=0S(ΓSN)xN(1.3)
for each finite subgroup Γ ⊂ Sp(2, ℂ), see Theorem 5.1.

All needed definitions are given in the Section 2; the structure, conjugacy classes and characteristic polynomials of the groups Γ ≀ SN are described in Section 3.

To include the case N = 0 in consideration in formulas (1.2)(1.3), it is natural to set Γ ≀ S0 := {E} and, since dimV = 0, to set H1,η(Γ ≀ S0) := ℂ[{E}], where {E} is the group containing only one element E.

Applying the definitions given in Section 2 to the algebra H1,η(Γ ≀ S0) we deduce that

  1. a)

    if the algebra H1,η(Γ ≀ S0) = ℂ[{E}] is considered as superalgebra, it has only a trivial parity π ≡ 0;

  2. b)

    the algebra H1,η(Γ ≀ S0) = ℂ[{E}] has 1-dimensional space of traces and 1-dimensional space of supertraces; these spaces coincide;

  3. c)

    it is natural to set T(Γ ≀ S0) = S(Γ ≀ S0) = 1;

  4. d)

    the algebra H1,η(Γ ≀ S0) = ℂ[{E}] contains two Klein operators (i.e., elements satisfying conditions (2.1)(2.3)), namely, 1 and −1.

2. Preliminaries

2.1. Traces

Let 𝒜 be an associative superalgebra with parity π. All expressions of linear algebra are given for homogenous elements only and are supposed to be extended to inhomogeneous elements via linearity.

A linear complex-valued function str on 𝒜 is called a supertrace, if

str(fg)=(1)π(f)π(g)str(gf)forallf,g𝒜.

A linear complex-valued function tr on 𝒜 is called a trace, if

tr(fg)=tr(gf)forallf,g𝒜.

The element K𝒜 is called a Klein operator, if

π(K)=0,(2.1)
K2=1,(2.2)
Kf=(1)π(f)fK,forallf𝒜.(2.3)

Any Klein operator, if exists, establishes an isomorphism between the space of traces on 𝒜 and the space of supertraces on 𝒜.

Namely, if f ↦ tr(f) is a trace, then f ↦tr(fK1+π(f)) is a supertrace, and if f ↦str(f) is a supertrace, then f ↦str(fK1+π(f)) is a trace.

2.2. Symplectic reflection group

Let V = ℂ2N be endowed with a non-degenerate anti-symmetric Sp(2N)-invariant bilinear form ω(·,·), let the vectors eiV, where i = 1 ... , 2N, constitute a basis in V.

The matrix (ωij) := ω(ei, ej) is anti-symmetric and non-degenerate.

Let xi be the coordinates of xV, i.e., x = ei xi. Then ω(x, y) = ωijxiyj for any x, yV. The indices i are lowered and raised by means of the forms (ωij) and (ωij), where ωijωkj=δik.

Definition 2.1.

The element R ∈ Sp(2N)⊂EndV is called a symplectic reflection, if rank(R−1)=2.

Definition 2.2.

Any finite subgroup G of Sp(2N) generated by a set of symplectic reflections is called a symplectic reflection group.

In what follows, G stands for a symplectic reflection group, and stands for the set of all symplectic reflections in G.

Let R. Set

VR:=Im(R1),(2.4)
ZR:=Ker(R1).(2.5)

Clearly, VR and ZR are symplectically perpendicular, i.e., ω(VR, ZR) = 0, and V = VRZR.

So, let x = xVR + xZR for any xV, where xVRVR and xZRZR. Set

ωR(x,y):=ω(xVR,yVR).(2.6)

2.3. Symplectic reflection algebra (following [3])

Let ℂ[G] be the group algebra of G, i.e., the set of all linear combinations gGαgg¯, where αg ∈ ℂ.

If we were rigorists, we would write g¯ to distinguish g considered as an element of G ⊂ End(V) from the same element g¯[G] considered as an element of the group algebra. The addition in ℂ[G] is defined as follows:

gGαgg¯+gGβgg¯=gG(αg+βg)g¯
and the multiplication is defined by setting g1¯g2¯=g1g2¯. In what follows, however, we abuse notation and omit the bar sign over elements of the group algebra.

Let η be a function on , i.e., a set of constants ηR with R such that ηR1 = ηR2, if R1 and R2 belong to one conjugacy class of G.

Definition 2.3.

The algebra Ht,η(G), where t ∈ ℂ, is an associative algebra with unit 1; it is the algebra ℂ[V] of (noncommutative) polynomials in the elements of V with coefficients in the group algebra ℂ[G] subject to the relations

gx=g(x)gforanygGandxV,whereg(x)=eigijxiforx=eixi,(2.7)
[x,y]=tω(x,y)+RηRωR(x,y)Rforanyx,yV.(2.8)

The algebra Ht,η(G) is called a symplectic reflection algebra, see [3].

The commutation relations (2.8) suggest to define the parity π by setting:

π(x)=1,π(g)=0foranyxV,andgG,(2.9)
enabling one to consider Ht,η(G) as an associative superalgebra.

We consider the case t ≠ 0 only, for any such t it is equivalent to the case t = 1.

Let 𝒜 and be superalgebras such that 𝒜 is a -module. We say that the superalgebra 𝒜 * is a crossed product of 𝒜 and , if 𝒜 * = 𝒜 as a superspace and

(a1b1)*(a2b2)=a1b1(a2)b1b2,
see [14]. The element b1(a2) may include a sign factor imposed by the Sign Rule, see [1], p. 45.

The (super)algebra H1,η(G) is a deform of the crossed product of the Weyl algebra WN and the group algebra of a finite subgroup G ⊂ Sp(2N) generated by symplectic reflections.

2.4. The number of independent traces and supertraces on the symplectic reflection algebras

Theorem 2.1 ([11]).

Let the symplectic reflection group G ⊂ End(V) have TG conjugacy classes without eigenvalue 1 and SG conjugacy classes without eigenvalue −1.

Then the algebra H1,η(G) has T(G) = TG independent traces whereas H1,η(G) considered as a superalgebra, see (2.9), has S(G) = SG independent supertraces.

Proposition 2.1.

Let G1 ⊂ End(V1), G2 ⊂ End(V2) and G = G1 × G2 ⊂ End(V1V2) be symplectic reflection groups. Then T(G) = T(G1)T(G2) and S(G) = S(G1)S(G2).

Proof follows from evident relations TG = TG1TG2, SG = SG1SG2 and Theorem 2.1.

Proposition 2.2.

If there exists a KG such that K|V = −1, then K is a Klein operator.

3. The group Γ ≀ SN

3.1. Finite subgroups of Sp(2,ℂ)

The complete list of the finite subgroups Γ ⊂ Sp(2, ℂ) is as follows, see, e.g., [15]:

Γ Order Presence of −1 The number of conjugacy classes C(Γ)
Cyclic group Zn := 𝕑/n𝕑 n yes, if n is even;
no, if n is odd
n
Binary dihedral group 𝒟n 4n yes n + 3
Binary tetrahedral group 𝒯 24 yes 7
Binary octahedral group 𝒪 48 yes 8
Binary icosahedral group 120 yes 9

It is easy to see that each of these groups, except Z2k+1, has C(Γ) − 1 conjugacy classes without +1 in the spectrum and has C(Γ) − 1 conjugacy classes without −1 in the spectrum. The group Z2k+1 has C(Z2k+1) − 1 conjugacy classes without +1 in the spectrum and it has C(Z2k+1) conjugacy classes without −1 in the spectrum.

3.2. Symplectic reflections in Γ ≀ SN (following [4])

Let V = ℂ2N and let the symplectic form ω have the shape

ω:=(ϖϖϖ),whereϖ=(0110).(3.1)

The elements of the group Γ≀SN have the form of N × N block matrix with 2×2 blocks. Consider the following elements of Γ ≀ SN

(Dg,i)kl:={g,ifk=l=i,1,ifk=li,0,otherwise,(3.2)
(Kij)kl:={δkl,ifk,li,k,lj,δkiδlj+δkjδli,otherwise,(3.3)
Sg,ij:=Dg,iDg1,jKij,(3.4)
where i, j = 1,...,N, ij, 1 ≠ g ∈ Γ. It is clear that Kij = Kji and Sg,ij = Sg−1,ji.

The complete set of symplectic reflections in Γ ≀ SN consists of Dg,i, Kij and Sg,ij, where 1 ⩽ i < jN and 1 ≠ g ∈ Γ. This set generates the group Γ ≀ SN.

The symplectic reflections Kij and Sg,ij lie in one conjugacy class for all ij and g ≠ 1; the elements Dg,i (g ≠ 1) and Dh,j (h ≠ 1) lie in one conjugacy class, if g and h are conjugate in Γ. So, the algebra H1,η(Γ ≀ SN) depends on C(Γ) parameters η, if N ⩾ 2, and on C(Γ) − 1 parameters, if N = 1. Here C(Γ) is the number of conjugacy classes in Γ including the class {1}.

3.3. Conjugacy classes (following [13])

Further, the elements of the group Γ ≀ SN can be represented in the form where D ∈ ΓN is a diagonal N × N block matrix, each block being a 2 × 2-matrix, and σ is N × N block matrix of permutation each block being a 2 × 2-matrix.

The product has the form:

(D1σ1)(D2σ3)=D3σ3
where σ3 = σ1σ2 and D3=D1σ1D2σ11.

Fix an element g0 = D0σ0. Since the permutation σ0 is a product of cycles, there exists a permutation σ′ such that

σσ0(σ)1=(c1c2cs),whereckarethecyclesoflengthLk,kLk=N,(3.5)
ck=(0100000100000100000110000).(3.6)

The element σ′D0σ0(σ′)−1 has the form

σD0σ0(σ)1=(D1c1D2c2Dscs),
where Dk is an Lk × Lk diagonal block matrix, each block being a 2 × 2-matrix:
Dk=(g1kg2kgLkk),gikΓ.

Next, consider diagonal block matrices Hk=diag(h1k,h2k,,hLkk) and the elements

HkDkckHk1=(h1kg1k(h2k)1h2kg2k(h3k)1h3kg3k(h4k)1hLkkgLkk(h1k)1)ck.

For any element h1kΓ, one can choose

h2k=h1kg1k,h3k=h2kg2k,,hLkk=hLk1kgLk1k
such that
HkDkckHk1=(111h1kg1kg2kgLkk(h1k)1)ck.

So, each conjugacy class of Γ ≀ SN is described by the set of cycles in the decomposition (3.5), (3.6) of σ0, where each cycle is marked by some conjugacy class of Γ.

The cycle of length r marked by the conjugacy class α of Γ with representative gα ∈ Γ has the shape:

Aα,r:=(111gα)cr=(01000001000001000001gα0000),(3.7)
where α = 1,...,C(Γ) and r = 1, 2,...; the matrix Aα,r and the cycle cr are the r × r block matrices, each block being a 2 × 2 matrix.

So, each element g ∈ Γ ≀ SN is conjugate to the element of the shape

(Aα1,r1Aα2,r2Aαs,rs)(3.8)

It is convenient to describe the conjugacy class of Γ ≀ SN with representative (3.8) by the set of nonnegative integers prα, where r = 1, 2, 3,..., and α = 1, ... , C(Γ), such that

α,rrprα=N.(3.9)

The value prα for some conjugacy class is the number of cycles Aα,r of length r in the decomposition (3.8) marked by the conjugacy class α of the group Γ.

Note that in [13] the notation mr(α) is used instead of prα we use in this paper.

The restriction (3.9) can be omitted and can serve as definition of N for each set of the numbers prα.

The number of conjugacy classes in Γ ≀ SN is equal to

C(ΓSN)=prα:α,rrprα=N1.

The generating function c(Γ, x) of the number of conjugacy classes is defined as

c(Γ,x):=N=0C(ΓSN)xN
and is equal to
c(Γ,x)=prαxα,rrprα=prα=0r=1α=1C(Γ)(xr)prα=r=1α=1C(Γ)11xr=(Ψ(x))C(Γ),
where Ψ(x) is the Euler function
Ψ(x):=r=111xr

3.4. Characteristic polynomials of conjugacy classes

Before seeking the generating functions t(Γ, x) and s(Γ, x), let us find the characteristic polynomial of the conjugacy class g of Γ ≀ SN identified by the set prα.

Let PM(λ) := det(Mλ) be the characteristic polynomial of the matrix M. Then it is easy to see that

PAα,r(λ)=det(Aα,rλ)=det(gαλr)=Pgα(λr),
where the marked cycle Aα,r is defined by (3.7).

Let g ∈ Γ ≀ SN be defined by Eq. (3.8).

Now, it is easy to show that

Pg(λ)=det(gλ)=i=1sdet(Aαi,riλ)=α,r:prα1det(Aα,rλ)prα=α,r:prα1(det(gαλr))prα,(3.10)
if g is a representative of the congugacy class in Γ ≀ SN corresponding to the set prα.

Definition 3.1.

We call a conjugacy class t-admissible, if its representative g ∈ Γ ≀ SN is such that Pg(1) ≠ 0.

Definition 3.2.

We call a conjugacy class s-admissible, if its representative g ∈ Γ ≀ SN is such that Pg(−1) ≠ 0.

Definition 3.3.

We call a marked cycle Aα,r, see Eq. (3.7), t-admissible, if PAα,r(1) ≠ 0.

Definition 3.4.

We call a marked cycle Aα,r, see Eq. (3.7), s-admissible, if PAα,r(−1) ≠ 0.

Equation (3.10) implies the following statements:

Proposition 3.1.

The conjugacy class of Γ ≀ SN identified by the set prα is t-admissible, if and only if the marked cycle Aα,r is t-admissible for any pair α, r such that prα0,

Proposition 3.2.

The conjugacy class of Γ ≀ SN identified by the set prα is s-admissible, if and only if the marked cycle Aα,r is s-admissible for any pair α, r such that prα0,

Recall that gα ∈ Γ ⊂ Sp(2, ℂ), where Γ is a finite group. So detgα = 1 and the Jordan normal form of gα is diagonal. This implies that if gα has +1 in its spectrum, then gα = 1 and if gα has −1 in its spectrum, then gα = −1. These facts together with Eq. (3.10) imply, in their turn, the following two propositions:

Proposition 3.3.

The conjugacy class of Γ ≀ SN identified by the set prα is t-admissible if and only if gα ≠ 1 for all α, r with prα0.

Proposition 3.4.

The conjugacy class of Γ ≀ SN identified by the set prα is s-admissible if and only if for any pair α, r such that prα0 , at least one of the next three conditions holds:

  1. a)

    gα ≠ −1 and gα ≠ 1,

  2. b)

    r is even and gα = −1,

  3. c)

    r is odd and gα = 1.

Note that the three sets of pairs (r, α) defined by the cases a), b), c) in Proposition 3.4 have empty pair-wise intersections.

Definition 3.5.

Let tr(Γ) for r = 1, 2 ... be equal to the number of different α such that Aα,r is t-admissible.

Evidently,

tr(Γ)=C(Γ)1.(3.11)

Definition 3.6.

Let sr(Γ) for r = 1, 2 ... be equal to the number of different α such that Aα,r is s-admissible.

Evidently, if Γ ∋ −1, then

sr(Γ)=C(Γ)1.(3.12)
and if Γ ∌ −1, then
sr(Γ)={C(Γ)1,ifriseven,C(Γ),ifrisodd.(3.13)

4. Combinatorial problem

Consider the following combinatorial problem (analogous problems are considered in [8]).

Suppose we have an unlimited supply of 1-gram colored weights for each of n1 different colors, an unlimited supply of 2-gram colored weights for each of n2 different colors, an unlimited supply of 3-gram colored weights for each of n3 different colors, and so on. Let an1,,nk,N be the number of opportunities to choose weights from our set of total mass N grams.

The problem is to find generating function

Fn1,,nk,(x):=N=0an1,,nk,NxN.

This problem is exactly the problem we discussed earlier. Namely, now we say “r-gram weight” instead of cycle of length r, and “the number of different colors nr” instead of the number tr (3.11) or sr (3.12)(3.13) of different α.

Proposition 4.1.

Fn1+m1,n2+m2,,nk+mk,(x)=Fn1,n2,,nk,(x)Fm1,m2,,mk,(x).

Proof.

To prove this proposition, it suffices to note that

an1+m1,n2+m2,,nk+mk,N=M=0Nan1,n2,,nk,Mam1,m2,,mk,NM.

Introduce the functions

fi:=Fn1i,n2i,,nki,,wherenki=δki.

Then

fi(x)=1+xi+x2i+x3i+=11xi.

The next theorem follows from Proposition 4.1

Theorem 4.1.

Fn1,n2,,nk,=i=1(fi)ni.

The function F1, 1, 1,... = Ψ(x) is the well-known Euler function, the generating function of the number of partitions of N into the sum of positive integers.

5. Generating functions t(Γ) and s(Γ)

Theorem 5.1.

Set

Ψ(x)=i=111xi(Eulerfunction),(5.1)
Φ(x)=k=011x2k+1.(5.2)

Let T (Γ ≀ SN) be the dimension of the space of traces on H1,η(Γ ≀ SN) and let S(Γ ≀ SN) be the dimension of the space of supertraces on H1,η(Γ ≀ SN) considered as a superalgebra.

Let

t(Γ,x):=N=0T(ΓSN)xNands(Γ,x):=N=0S(ΓSN)xN.

Then

t(Γ,x)=(Ψ(x))C(Γ)1,s(Γ,x)=(Ψ(x))C(Γ)1,ifΓZ2k+1,s(Γ,x)=(Ψ(x))C(Γ)1Φ(x),ifΓ=Z2k+1.

Proof.

To prove Theorem 5.1. we apply Theorem 4.1 to the numbers (3.11)(3.13) of admissible conjugacy classes. It is clear that

t(Γ)=Ft1(Γ),t2(Γ),t3(Γ),=ΨC(Γ)1,s(Γ)=Fs1(Γ),s2(Γ),s3(Γ),={ΨC(Γ)1,ifΓ1,ΨC(Γ)1Φ,ifΓ1.

Observe that Φ(x)=i=0ONxN, where ON is the number of partitions of N into the sum of odd positive integers, and ON coinsides with the number of independent supertraces on H1η(SN), see [12].

5.1. Inequality theorem

Theorem 5.2.

Let G = Γ ≀ SN. For each positive integer N, the following statements hold:

S(G)>0,S(G)T(G),S(G)=T(G)ifandonlyifH1,η(G)containsaKleinoperator.

Literally the same statements were proved for the groups G from Family 1) in [10], and hence these statements hold for the direct product of any finite number of groups from Family 1) and Family 2) defined on page 1.

Proof.

Let Γ ≠ Z2k+1. Since each finite group Γ ∈ Sp(2N, ℂ), except Γ = Z2k+1, contains −1, the group Γ ≀ SN contains Klein operator K=i=1ND1,i.

There is no Klein operator in H1,η(Z2k+1SN) since for this algebra, S(Z2k+1SN) > T (Z2k+1SN), as it follows from Theorem 5.1.

Acknowledgments

The authors (S.K. and I.T.) are grateful to Russian Fund for Basic Research (grant No. 17-02-00317) for partial support of this work.

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Journal
Journal of Nonlinear Mathematical Physics
Volume-Issue
25 - 3
Pages
485 - 496
Publication Date
2021/01/06
ISSN (Online)
1776-0852
ISSN (Print)
1402-9251
DOI
10.1080/14029251.2018.1494768How to use a DOI?
Copyright
© 2018 The Authors. Published by Atlantis and Taylor & Francis
Open Access
This is an open access article distributed under the CC BY-NC 4.0 license (http://creativecommons.org/licenses/by-nc/4.0/).

Cite this article

TY  - JOUR
AU  - S.E. Konstein
AU  - I.V. Tyutin
PY  - 2021
DA  - 2021/01/06
TI  - The number of independent Traces and Supertraces on the Symplectic Reflection Algebra H₁,η(Γ ≀ SN)
JO  - Journal of Nonlinear Mathematical Physics
SP  - 485
EP  - 496
VL  - 25
IS  - 3
SN  - 1776-0852
UR  - https://doi.org/10.1080/14029251.2018.1494768
DO  - 10.1080/14029251.2018.1494768
ID  - Konstein2021
ER  -