This paper introduces a new algebra related to the universal enveloping algebra of rak{gl}_n, constructed via invariants under alternating groups, and explores its structure, representations, and connections to classical conjectures.
Contribution
It defines the algebra alA(rak{gl}_n) as an invariant ring under alternating groups, shows it is a Galois ring, and analyzes its structure and modules, extending previous work on symmetric groups.
Findings
01
alA(rak{gl}_n) is a Galois ring.
02
For n=2, alA(rak{gl}_n) is a generalized Weyl algebra.
03
Connections to Gelfand-Kirillov Conjecture and Noether's problem.
Abstract
In 2010, V. Futorny and S. Ovsienko gave a realization of U(gln) as a subalgebra of the ring of invariants of a certain noncommutative ring with respect to the action of S1×S2×⋯×Sn, where Sj is the symmetric group on j variables. An interesting question is what a similar algebra would be in the invariant ring with respect to a product of alternating groups. In this paper we define such an algebra, denoted A(gln), and show that it is a Galois ring. For n=2, we show that it is a generalized Weyl algebra, and for n=3 provide generators and a list of verified relations. We also discuss some techniques to construct Galois orders from Galois rings. Additionally, we study categories of finite-dimensional modules and generic Gelfand-Tsetlin modules over A(gln). Finally, we discuss connections…
Equations187
φHC:Z(A(gln))≅C[x1,…,xn]An.
φHC:Z(A(gln))≅C[x1,…,xn]An.
(A1)
(A1)
(A2)
(A3)
\operatorname{supp}u=\bigg{\{}\mu\in\mathscr{M}~{}\Big{|}~{}a_{\mu}\neq 0\text{ for }u=\sum_{\mu\in\mathscr{M}}a_{\mu}\mu\bigg{\}}
\operatorname{supp}u=\bigg{\{}\mu\in\mathscr{M}~{}\Big{|}~{}a_{\mu}\neq 0\text{ for }u=\sum_{\mu\in\mathscr{M}}a_{\mu}\mu\bigg{\}}
\begin{array}[]{ll}X_{k}^{\pm}=\sum_{i=1}^{k}(\delta^{ki})^{\pm 1}a_{ki}^{\pm}&\text{ for }k=1,\ldots,n-1,\\
X_{kk}=\sum_{j=1}^{k}(x_{kj}+j-1)-\sum_{i=1}^{k-1}(x_{k-1,i}+i-1)&\text{ for }k=1,\ldots,n,\\
\mathcal{V}_{k}=\mathcal{V}_{k}(x_{k1},\ldots,x_{kk})=\prod_{i<j}(x_{ki}-x_{kj})&\text{ for }k=1,\ldots,n-1,\end{array}
\begin{array}[]{ll}X_{k}^{\pm}=\sum_{i=1}^{k}(\delta^{ki})^{\pm 1}a_{ki}^{\pm}&\text{ for }k=1,\ldots,n-1,\\
X_{kk}=\sum_{j=1}^{k}(x_{kj}+j-1)-\sum_{i=1}^{k-1}(x_{k-1,i}+i-1)&\text{ for }k=1,\ldots,n,\\
\mathcal{V}_{k}=\mathcal{V}_{k}(x_{k1},\ldots,x_{kk})=\prod_{i<j}(x_{ki}-x_{kj})&\text{ for }k=1,\ldots,n-1,\end{array}
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Full text
An Extension of U(gln) Related to the Alternating Group and Galois Orders
Erich C. Jauch
Department of Mathematics, Iowa State University, Ames, IA-50011, USA
In 2010, V. Futorny and S. Ovsienko gave a realization of U(gln) as a subalgebra
of the ring of invariants of a certain noncommutative ring with respect to the action
of S1×S2×⋯×Sn, where Sj is the symmetric group on j
variables. An interesting question is what a similar algebra would be in the invariant
ring with respect to a product of alternating groups. In this paper we define such an
algebra, denoted A(gln), and show that it is a Galois ring. For n=2, we show that it is a generalized Weyl algebra, and for n=3 provide generators and a list of verified relations. We also discuss some
techniques to construct Galois orders from Galois rings. Additionally, we study categories of
finite-dimensional modules and generic Gelfand-Tsetlin modules over A(gln).
Finally, we discuss connections between the Gelfand-Kirillov Conjecture, A(gln), and the positive solution to Noether’s problem for the alternating group.
The study of algebra-subalgebra pairs is an important technique used in the representation theory
of Lie algebras [16],[2]. In 2010, Futorny and Ovsienko focused on so called semicommutative
pairs Γ⊂U, where U is an associative (noncommutative)
C-algebra and Γ is an integral domain [7].
This situation generalizes the pair (Γ,U(gln)) where Γ
is the Gelfand-Tsetlin subalgebra Γ=C⟨∪k=1nZ(U(glk))⟩
[12], [2]. Galois rings and Galois orders were originally
defined and studied by Futorny and Ovsienko in [7] and [8]. They form a
collection of algebras that contains many important examples including:
generalized Weyl algebras defined by independently by Bavula [1]
and Rosenberg [19] in the early nineties, the universal enveloping algebra
of gln, shifted Yangians and finite W-algebras [6], Coulomb branches
[21], and Uq(gln) [5]. Their structures and representations
have been studied in [4], [9],
[14], and [18].
In [7], Futorny and Ovsienko described U(gln) as the subalgebra of
the ring of invariants of a certain noncommutative ring with respect to the action
of S1×S2×⋯×Sn, where Sj is the symmetric group on j
variables such that U(gln) was a Galois order with respect to its
Gelfand-Tsetlin subalgebra Γ.
We recall in Galois theory, given a Galois extension L/K with Gal(L/K)=G the
subgroups G of G correspond to intermediate fields K
with Gal(L/K)=G with normal subgroups of particular
interest. Since Sn has only one normal subgroup for n≥5, one might wonder
what the object similar to U(gln) would be if we considered the invariants with
respect to the normal subgroup A1×A2×⋯×An, where Aj
is the alternating group on j variables. This paper describes such an algebra,
denoted by A(gln) (see Definition 2.1). This provides the
first natural example of a Galois ring whose ring Γ is not a semi-Laurent
polynomial ring, that is, a tensor product of polynomial rings and Laurent
polynomial rings. Additionally, our symmetry group A1×A2×⋯×An is not
a complex reflection group. Our algebra A(gln) is an extension of U(gln)
by n−1 elements V2,…,Vn.
In Proposition 2.2, we prove some
properties of A(gln) that are quite similar to U(gln).
For example, it is shown that the “Weyl Group” of A(gln) is the
alternating group An, in the sense that there is a natural extension
φHC of the Harish-Chandra homomorphism
φHC:Z(U(gln))→S(h)≅C[x1,…,xn],
such that
[TABLE]
Moreover, there is a chain of subalgebras
A(gl1)⊂A(gl2)⊂⋯⊂A(gln).
In Section 3, we give multiple descriptions of A(gl2) and
prove it is realizable as a Galois order. Example 4.2
shows that A(gln) is not a Galois order for n≥3. The rest
of Section 4 lists a set of generators and some verified relations for
A(gl3), but this list may be incomplete. In Section 5,
we show that the category of finite-dimensional modules in not semi-simple and
classify simple finite-dimensional weight modules. In Section
6, we provide a technique to turn a general Galois ring
into a Galois order that is related to localization (see Theorem
6.2).
We use this to prove that a family of simple examples are Galois orders (see Corollary
6.8) and that a localization of A(gln) is a
(co-)principal Galois order over the localized Γ (see Definition
1.13 and Corollary
6.11). We use this localization
to construct canonical Gelfand-Tsetlin modules over A(gln) in
Section 7. Finally, in Section
8, we compute the division ring of fractions and
prove, that for n≤5, A(gln) satisfies the Gelfand-Kirillov conjecture
(see [13]). For the latter, we use Maeda’s positive
solution to Noether’s problem for the alternating group A5 [17],
and Futorny-Schwarz’s Theorem 1.1 in [10].
1.1. Galois orders
Galois orders were introduced in [7]. We will be following
the set up from [14]. Let Λ be an integrally closed
domain, G a finite subgroup of Aut(Λ), and M a
submonoid of Aut(Λ). We will adhere to the following
assumptions for the entire paper:
[TABLE]
Let L=Frac(Λ) and L=L#M, the skew monoid ring, which is defined as the
free left L-module on M with multiplication given by
a1μ1⋅a2μ2=(a1μ1(a2))(μ1μ2) for ai∈L and μi∈M.
As G acts on Λ by automorphisms, we can easily extend this action to L, and by (A2),
G acts on L. So we consider the following G-invariant subrings
Γ=ΛG, K=LG, and K=LG.
A benefit of these assumptions is the following lemma.
A Galois Γ-ring U in K is a left (respectively right)
Galois Γ-order in K if for any finite-dimensional left (respectively right)
K-subspace W⊆K, W∩U is a finitely generated left (respectively
right) Γ-module. A Galois Γ-ring U in K is a Galois
Γ-order in K if U is a left and right Galois Γ-order in
K.
Let Γ⊂U be a commutative subalgebra. Γ is called a
Harish-Chandra subalgebra in U if for any u∈U, ΓuΓ
is finitely generated as both a left and as a right Γ-module.
Let U be a Galois ring and e∈M the unit element. We denote
Ue=U∩Le.
Assume that U is a Galois ring, Γ is finitely generated and M
is a group.
(1)
Let m∈M. Assume m−1(Γ)⊆Λ (respectively m(Γ)⊆Λ).
Then U is right (respectively left) Galois order if and only if Ue is an
integral extension of Γ.
2. (2)
Assume that Γ is a Harish-Chandra subalgebra in U. Then U is
a Galois order if and only if Ue is an integral extension of Γ.
Let U1 and U2 be two Galois Γ-rings in
K such that U1⊆U2. If
U2 is a Galois Γ-order, then so too is U1.
It is common to write elements of L on the right side of elements of M.
Definition 1.11**.**
For X=∑μ∈Mμαμ∈L and a∈L
defines the evaluation of X at a to be
[TABLE]
Similarly defined is co-evaluation by
[TABLE]
The following was independently defined by [20] called the universal ring.
Definition 1.12**.**
The standard Galois Γ-order is as follows:
[TABLE]
Similarly we define the co-standard Galois Γ-order by
[TABLE]
Definition 1.13**.**
Let U be a Galois Γ-ring in K. If U⊆KΓ (resp.
U⊆ΓK), then U is called a principal (resp.
co-principal) Galois Γ-order.
In [14] it was shown that any (co-)principal Galois Γ-order is a
Galois order in the sense of Definition 1.6.
2. Defining the Extension
2.1. Galois order realization of U(gln)
We first recall the realization of U(gln) as a Galois Γ-order from [7].
Let Λ=C[xki∣1≤i≤k≤n] the polynomial algebra
in indeterminates xki,
Sn=S1×S2×⋯×Sn, and
Γ=ΛSn=C[eki∣1≤i≤k≤n].
Here
[TABLE]
are the elementary symmetric polynomials. Also, let L=Frac(Λ)
and K=Frac(Γ). Now, we construct a skew monoid ring. Let
M be the subgroup of Aut(Λ) generated by {δki}1≤i≤k≤n−1,
where δki is defined by
[TABLE]
We observe that M≅Zn(n−1)/2. Let L=L#M and
K=(L#M)Sn. In [7], the authors describe
an embedding φ:U(gln)→K defined by
[TABLE]
where
[TABLE]
and Ek+=Ek,k+1, Ek−=Ek+1,k where
Eij denotes the matrix units.
Let Un=φ(U(gln)). The algebra Un is a Galois Γ-order.
2.2. Defining A(gln)
Let An=A1×A2×⋯×An and
[TABLE]
Here
[TABLE]
denotes the Vandermonde polynomial in the ℓ variables
xℓ1,…,xℓℓ. Abstractly, Γ is isomorphic to the following quotient
[TABLE]
where Tki,Vℓ are indeterminates and Dℓ(Tℓ1,…,Tℓℓ)
is the Vandermonde discriminant. Also, let
K=Frac(Γ) and
K=(L#M)An.
Definition 2.1**.**
Consider the following extension of U(gln), denoted A(gln), defined as
the subalgebra of K generated
by Un∪{V2,V3,⋯,Vn}. Explicitly, A(gln)
is the subalgebra of L generated by
Since Xi±∈X, it is clear that ⋃u∈Xsuppu generates
M. Thus, A(gln) is a Galois Γ-ring for every n≥1 by
Proposition 1.4.
(3) As δki fixes xℓj iff ℓ=k
and k=n, it follows that Vn is central in A(gln).
(4) We first show that
Z(A(gln)=C⟨Z(Un),Vn⟩.
C⟨Z(Un),Vn)⟩⊆Z(A(gln)) is clear. Next, we observe that
A(gln)⊂(L′#M)An,
where L′=C(xki∣1≤i≤k≤n−1)[xn1,…,xnn].
By Theorem 1.5, we have
[TABLE]
Consider the
Harish-Chandra homomorphism
φHC:Z(U(gln))→C[x1,…,xn]Sn.
We can define an extension of this map
φHC:Z(A(gln))→C[x1,…,xn]
as follows:
[TABLE]
In conjuction with Chevalley’s Theorem (see [15]),
φHC provides an isomorphism with C[x1,…,xn]Sn. The
claim follows by recalling that C[x1,…,xn]An is generated
by the symmetric polynomials and the Vandermonde polynomial.
(6) We prove this
result by induction on n. Since A(gl1)=U(gl1), the base step is clear.
Assuming the claim holds for A(gln−1), now consider an extension A
of U(gln) satisfying (4) and
(5). By (5),
A contains Vℓ for ℓ=1,…,n−1, and it contains U(gln)
by definition. From (4) we get an element V that
is central in A that maps to ∏i<j(xi−xj)∈C[x1,…,xn]An.
This allows us to define an isomorphism τ:A→A(gln)
by sending {U(gln),Vℓ∣ℓ=1,…,n−1} to themselves
and V↦Vn.
∎
Remark 1*.*
In [11] another Galois algebra is described in the invariants of
a Weyl algebra with respect to a single alternating group in Corollary 24 in [11].
3. The Structure of A(gl2)
In this section, we find a presentation for A(gl2) as an extension of
U(gl2) and as a generalized Weyl algebra as well as prove that it is a Galois Γ-order.
Let p(T2)=T22−(−c212+2c22−1)∈U(gl2)[T2]. Since p(T2) is degree two, U(gl2)[T2]/(p(T2))
is free of rank 2 as a left U(gl2)-module with basis {1,T2} where T2=T2+(p(T2)). It follows Lemma
3.1(2) that A(gl2) is also free of rank 2 with basis
{1,V2} via the isomorphism φ in (3).
Therefore there is an isomorphism φ:U(gl2)[T2]/(p(T2))→A(gl2)
as U(gl2)-modules sending 1 to 1 and T2 to V2. Thus, it suffices to show that
φ(T22)=V22.
To show this, we calculate the images of c2i under φ:
[TABLE]
As such,
[TABLE]
Therefore, φ is an
algebra isomorphism.
∎
Theorem 3.4**.**
A(gl2)* is a Galois Γ-order.*
Proof.
We first observe that A(gl2) is a Galois Γ-ring by
Proposition 2.2(2).
To prove that A(gl2) is a Galois Γ-order,
we will use Theorem 1.8. Since Γ is a
Harish-Chandra subalgebra of U(gl2), Γ
is a Harish-Chandra subalgebra of A(gl2). Since A2 is a group,
all we need to show is that Γ is maximal commutative
in A(gl2). This is clear because Γ is maximal commutative in U2,
and Γ is just an extension by a central
element by Proposition 3.3. Γ
is maximal commutative in A(gl2); therefore, A(gl2) is a
Galois Γ-order.
∎
The following shows that A(gl2) is a generalized Weyl algebra [1],
which gives another way to show it is a Galois order [7]. First we recall
the definition of a generalized Weyl algebra.
Let D be a ring, σ a ring automorphism of D, and t a central element of
D. The generalized Weyl algebra of rank 1, D(σ,t)
is a ring generated by the ring D and two elements x and y subject to the
following relations:
[TABLE]
[TABLE]
Proposition 3.6**.**
A(gl2)* is isomorphic to the generalized Weyl algebra
Γ(σ,t), where σ=δ11,
Recall that A(gl2) is the subalgebra generated by Γ,X1± (see Definition 2.1).
We define ψ:Γ(σ,t)→A(gl2) by
[TABLE]
One can verify that the defining relations (10)
and (11) are preserved by ψ, making it well-defined.
Clearly ψ is surjective. For injectivity, we note ψ is graded, when
Γ(σ,t) and A(gl2) are equipped with the Z-gradations determined
by
[TABLE]
As such, kerψ is a graded ideal. But Γ∩(kerψ)=0. Since the only
graded ideal I in a generalized Weyl algebra D(σ,t), where D is a domain, with
D∩I=0 is I=0, we get kerψ=0.
∎
We observe the following interesting property of A(gl2) that we prove
does not hold for general n (see Proposition 4.3).
Proposition 3.7**.**
A(gl2)* has the property that (A(gl2))S2=U2.*
Proof.
This becomes clear when we consider the direct sum decomposition shown in
Lemma 3.1(2).
Consider a+bV2∈A(gl2):
[TABLE]
Therefore, (A(gl2))S2=U2.
∎
4. The Structure of A(gl3)
Based on the result of the previous section, the next logical step is to see if similar
results hold for gln with n≥3. We will continue using the notation of
the images of the generators of the U(gln) as before. As such:
[TABLE]
4.1. Non-polynomial rational functions in A(gl3)
Unlike in U(gl3) and A(gl2), we can construct non-polynomial rational
functions in A(gl3). It follows that for n≥3, A(gln) is not a Galois
Γ-order, and the invariant property of A(gl2) does not hold.
Let us denote the element described in (13)
by X2±. We define the following:
[TABLE]
By their definition, it is clear that they are in A(gl3).
The following example shows that if n≥3, then Γ
is not maximal commutative; hence, A(gln) is not a Galois Γ-order
by Proposition 1.9.
Example 4.2**.**
The following element belongs to A(gln) for n≥3:
[TABLE]
This is a rational function; hence, it lies in CentA(gl3)(Γ).
The following rather surprising fact shows that
the property in Proposition 3.7 does not hold for
larger n.
Proposition 4.3**.**
For n≥3, A(gln)Sn⊋Un.
Proof.
The fact that Un⊂A(gln)Sn is obvious by definition. To
show the containment is strict, we recall that because Un is a Galois Γ-order,
it is known that Un∩K=Γ. Therefore, we consider
A(gln)Sn∩K. Since U3⊆Un for every
n≥3, it suffices to show that A(gl3)S3∩K⊋Γ.
The object to prove this claim is constructed in the same way as in Example
4.2. It is quickly observed that
[TABLE]
is invariant under the action of S3. This element is clearly
not in Γ, so this element is in A(gl3)S3∩K∖Γ,
thereby proving the claim.
∎
4.2. Generators and relations for n=3
Based on the previous subsection, we determine a set of generators and some verified relations
for A(gl3). However, we do not know if this constitutes a presentation, that is, this
may be an incomplete list.
Proposition 4.4**.**
The algebra A(gl3) is generated by {X11,X22,X33,A11±,A21±,A22±,V2,V3}, where Aij±:=(δij)±1aij±, V2=x21−x22, and
V3=∏i<j(x3i−x3j).
What follows is a list of known relations:
(1)
[V3,X]=0* for all X∈A(gl3) (i.e V3 is central
in A(gl3)),*
2. (2)
[X,Y]=0* for all X,Y∈h=SpanC{X11,X22,X33,V2,V3},*
3. (3)
[h,Aij±]=±αij(h)Aij±* for all h∈h and 1≤j≤i≤2,
where αij(h) are given by the following matrix:*
[TABLE]
4. (4)
[A21±,A22∓]=0,
5. (5)
[A11±,A2i∓]=0* for i=1,2,*
6. (6)
[A11+,A11−]=X11−X22,
7. (7)
[A21+,A21−]+[A22+,A22−]=X22−X33,
8. (8)
[A11±,[A11±,A2i±]]=0* for i=1,2,*
9. (9)
A22±V2A21±=A21±V2A22±.
Proof.
Any of the relations involving only elements from U(gl3) (such as
(6)) follow from U(gl3) relations by
recalling that {X11,X22,X33,A11+,A11−}∈A(gl3)
correspond to {E11,E22,E33,E12,E21}∈U(gl3). All that
remains is to prove the relations involving new elements.
(2) This follows by observing that each is an element of
Γ which is a commutative ring.
(3) By the statement at the beginning
of this proof and (1), we only need to check
the second two rows and the second to last column. Each is proved in an
identical manner, we provide one below:
Determine whether the relations in Proposition 4.4
constitute a presentation for the algebra A(gl3).
5. Finite-Dimensional Modules over A(gln)
Since, as was shown in Section 4, A(gln) is not a Galois
Γ-order, techniques different from [8] are required
to study representations of A(gln).
If we consider the case of n=2, we recall that
A(gl2)≅U(gl2)[T2]/(T22−(−c212+2c22+1)). As such, it makes
sense to consider the induction and restriction functors between the categories of
A(gl2)-modules and U(gl2)-modules.
By applying the restriction functor to a given finite-dimensional simple module,
we see that it decomposes to a direct sum of finite-dimensional simple
U(gl2)-modules, so the induction functor should help us to construct
all of the possible finite-dimensional simple A(gl2)-modules.
Proposition 5.1**.**
The finite-dimensional simple A(gl2)-modules are characterized by ordered pairs
(λ2,ε2), where λ2:=(λ21,λ22)∈C2
is a dominant integral weight for U(gl2) (i.e. λ21−λ22∈Z≥0) and ε2∈{1,−1}.
Proof.
Recall that every finite-dimensional simple U(gl2)-module is characterized by a weight denoted by a pair
of complex numbers λ2=(λ21,λ22) with λ21−λ22∈Z≥0; we will denote this module by
V(λ2). We can induce such a module V(λ2)
to a A(gl2)-module as follows,
[TABLE]
So, it is important to describe A(gl2) as a right U(gl2)-module. By Proposition 3.3:
[TABLE]
as right U(gl2)-modules. Thus:
[TABLE]
As such, we can determine the action of T2 on this modules now. For
v∈V(λ2), we have that T2.(1⊗v)=T2⊗v, and
T2.(T2⊗v)=T22⊗v=1⊗T22.v=(λ21−λ22)2(1⊗v).
Thus, T2 can be characterized by the following matrix:
[TABLE]
so we can see that A(gl2)⊗U(gl2)V(λ2) decomposes into
the two eigenspaces of the action of T2: V(λ2,+1):=⟨(λ21−λ22)(1⊗v)+T2⊗v∣v∈V(λ2)⟩ and V(λ2,−1):=⟨−(λ21−λ22)(1⊗v)+T2⊗v∣v∈V(λ2)⟩ both of which are clearly simple. It is also
clear that as vector spaces V(λ2,±1)≅V(λ2).
Conversely, if we have a finite-dimensional simple A(gl2)-module V restricted
to a U(gl2)-module, it must remain simple, as T2 is a central element. As such,
V≅V(λ2) for some weight λ2. Thus,
V≅V(λ2,ε2) for some ε2∈{±1}.
∎
Next, we classify a collection of finite-dimensional simple weight modules over A(gln).
Definition 5.2**.**
Let V(λn) be a weight module of U(gln), we extend it to a module for A(gln), denoted
V(λn,εn,εn−1,…,ε2), by describing the actions of each Vk for
k=2,3,…,n as follows:
[TABLE]
with εn=±1. Recall that when we restrict V(λn) to a U(glk) module, the number of
simple U(glk) modules it decomposes into is the same as the number of ways to fill in the k-th row of a Gelfand-Tsetlin
pattern with top row λn. Denote this number by rλn,k. Then let Vk act diagonallizably
on a v=(v1,…,vrλn,k)∈V(λn,εn,εn−1,…,ε2) by the following rλn,k×rλn,k matrix,
[TABLE]
where λkiℓ denotes the ki entry from the ℓ-th pattern in the decomposition of v as a U(glk)-module,
and εk=(εk,1,εk,2,…,εk,rλn,k)∈{±1}rλn,k.
Theorem 5.3**.**
Every finite-dimensional simple module over A(gln), on which
V2,…,Vn−1 act diagonallizably, is of the form
V(λn,εn,εn−1,…,ε2) (see Definition 5.2), where
λn=(λn1,λn2,…,λnn) is a dominant integral weight of U(gln),
εj∈{±1}rλn,j, with rλn,j denoting the number
of ways to fill the j-th row of Gelfand-Tsetlin pattern with fixed top row λn,
and j=2,3,…,n.
Proof.
We prove this by induction on n. For the base case, n=3, we have the
following commutative diagram:
where each arrow is the restriction functor. If we consider a simple
V∈A(gl3)-Modf.d. and its image in the bottom right corner, we see that
V≅⨁λ3⨁λ2V(λ2)λ3∈U(gl2)-Modf.d., where λ3 and λ2 are weights for U(gl3) and
U(gl2), respectively, by the semi-simplicity of U(gl3) and U(gl2). Moreover,
V(λ2)λ3’s are the components of the restriction of V(λ3)
to U(gl2). We know that V2 must have a diagonal action by assumption.
As such, we have V≅⨁λ3⨁λ2V(λ2,ε2)λ3 in the upper right corner by Proposition
5.1, where ε2=ε2(λ2)
depends λ2. This is because otherwise the dimensions of the λ2 weight
spaces would not match. Since V2 acts diagonally, V3 is central, and
the diagram commutes, it follows that
V≅V(λ3,ε3,ε2)∈A(gl3)-Modf.d., where
ε3 is determined as in Proposition 5.1,
and ε2={ε2(λ2)}λ2 is indexed by the
number rλ3,2.
To finish the induction we look at a similar diagram:
Following the image of a simple V∈A(gln)-Modf.d. and using identical arguments,
we observe that:
[TABLE]
By the induction hypothesis,
[TABLE]
Finally by Vn central, Vj acting diagonally for j=2,…,n−1,
and the diagram commuting, it follows that
V≅V(λn,εn,εn−1,…,ε2).
∎
The following example demonstrates that A(gln)-Modf.d. is not semi-simple for every
n≥2.
Example 5.4**.**
We recall that V22 must act diagonally
on any A(gl2)-module V because ResU(gl2)A(gl2)V
can be viewed as a direct sum of irreducible U(gl2)-modules and
V22 is a quadratic polynomial of Gelfand invariants in
U(gl2). Let V=V(0)⊕V(0), where U(gl2) acts trivially. This means that
V22 must act as IdV. We define the following action of V2
[TABLE]
with 0=α∈C. It is clear then that V22
acts as the identity on V, but the subrepesentation W={(v1,0)∣v1∈V(0)}
is not a direct summand of V as a A(gl2)-module.
6. A Technique for Creating Galois Orders from Galois Rings Via
Localization
In this section, we describe a technique that allows us to turn a Galois ring
into a Galois order involving localization. We use this technique on a toy example
and a localized version of A(gln) denoted A(gln)
(see Definition 6.10).
6.1. The general result
We recall that Proposition 1.9
states that Γ is maximal commutative in a Galois Γ-order. We observe that
for a general Galois Γ-ring U, while Γ might not be maximal
commutative, its centralizer CU(Γ) in U will be [7].
This can be seen from the following remark:
Remark 2*.*
For Galois Γ-ring U, the centralizer of Γ in U,
denoted CU(Γ), is equal to U∩K.
First we define a subring of L that is needed in our result.
Definition 6.1**.**
Let U be a subalgebra of L. We define the
ring of coefficients of U:
[TABLE]
Similarly, we define the opposite ring of coefficients of U, denoted
DUop, using right coefficients.
Now for the result.
Theorem 6.2**.**
Let G be arbitrary and U be a Galois Γ-ring in (L#M)G.
If C=CU(Γ) is the G invariants of the localization of Λ
with respect to a set that is M-invariant, that is C=(S−1Λ)G,
where S is M-invariant, and DU is a finitely generated
module over C, then U is a Galois C-order in (L#M)G.
Moreover, if DU⊆S−1Λ (resp. DUop⊂S−1Λ),
then U is a (co-)principal Galois C-order.
Proof.
First, we find a Λ′ such that (Λ′,G,M)
satisfies the assumptions in Section 1.1. We define
Λ′=C, the integral closure of C in L. We observe that
C=(SG)−1Γ. As such, C is a localization, and it follows that:
[TABLE]
Since S is M-invariant and C is integral over C,
it follows that M and G are subgroups of Aut(Λ′).
The first two assumptions clearly hold, and the third follows by
Λ′=S−1Λ.
We have that U is a Galois C-ring since it is a Galois
Γ-ring and Frac(C)=Frac(Γ)=K. All that remains is to show
that U is a Galois C-order. We consider W⊂L
a finite-dimensional left L-subspace and aim to show that W∩U
is finitely generated as a left C-module. W has a finite basis
w1,…,wn such that:
[TABLE]
Note that for each i, wi=∑μ∈Mβi,μμ;
as such, since C is a localization of a Noetherian ring and therefore Noetherian,
WLOG we can assume wi=μi for some μi∈M.
Hence:
[TABLE]
So, W∩U⊂∑iDUμi, and is
therefore finitely generated. A similar argument justifies the claim if W
is instead a right L-module. Therefore, U is a Galois C-order.
If additionally we assume DU⊂S−1Λ, we need
to show that X(c)∈C for all X∈U and c∈C. So, we consider
an arbitrary c∈C and X∈U. By Lemma 2.19 in [14],
it follows that X(c)∈K. Since C=(SG)−1Γ, it follows that
X(c)∈S−1Λ. As such:
[TABLE]
Thus X(c)∈C. If instead DUop⊂S−1Λ,
a similar argument shows that X†(c)∈C, thereby proving the claim.
∎
The above theorem also gives an alternate proof to one direction of Corollary 2.15 in [14].
6.2. A toy example
In this subsection, we provide a family of simple examples of Galois rings
to which Theorem 6.2
can be applied.
Let Λ=C[x] the polynomial algebra in one indeterminate x, δ∈AutΛ such that δ(x)=x−1,
M=⟨δ⟩grp, and G the trivial group.
Then, let L=L#M be the skew-monoid ring and f(x)∈C[x]
such that f(0)=0. We define X,Y∈L such that:
[TABLE]
Let Uf=C⟨Λ,X,Y⟩alg and CUf(Λ)(=CUf)
the centralizer of Λ in Uf. We note, as G is trivial,
that Λ=Γ. First, we will show that Uf is Galois Γ-ring.
Proposition 6.3**.**
The algebra Uf is a Galois Γ-ring in L#M.
Proof.
This immediately follows from Proposition 1.4
letting X={X,Y}.
∎
In order to apply Theorem 6.2,
we need to describe CUf. The next three lemmas are used to do just that.
Lemma 6.4**.**
For any f(x) such that f(0)=0, we have x1,x−11∈CUf.
Proof.
First, we show that x1∈CUf. Now, f(x)=anxn+⋯+a1x+a0 with a0=0
by assumption. As such:
[TABLE]
This shows that x1∈CUf. To see that x−11∈CUf, we follow a similar
division algorithm argument with x−1f(x−1).
∎
Lemma 6.5**.**
For any f(x) such that f(0)=0 and k≥1, we have x+k1∈CUf.
Proof.
Let m be the order of (x+k) in j=0∏k−1f(x+j). Then consider the following:
[TABLE]
As such, there are m factors of (x+k) in the numerator and m+1 factors in the
denominator. Thus, multiplying by j=0∏k−1(x+j) and using
a division algorithm argument, it follows that x+k1∈CUf.
∎
Lemma 6.6**.**
For any f(x) such that f(0)=0 and k≥2, we have x−k1∈CUf.
Proof.
Let m be the order of (x−k) in j=1∏k−1f(x−j). Then consider
the following:
[TABLE]
As such, there are m factors of (x−k) in the numerator and m+1 factors in the
denominator. Thus, multiplying by j=1∏k−1(x−j) and using a
division algorithm argument, it follows that x−k1∈CUf.
∎
Proposition 6.7**.**
If f(x) is a polynomial such that f(0)=0, then
C_{U_{f}}=\mathbb{C}[x]\bigg{[}\frac{1}{x+k}~{}\bigg{|}~{}k\in\mathbb{Z}\bigg{]}.
Proof.
C_{U_{f}}\supseteq\mathbb{C}[x]\bigg{[}\frac{1}{x+k}~{}\bigg{|}~{}k\in\mathbb{Z}\bigg{]} by
Lemmas 6.4, 6.5, and 6.6.
To show the reverse inclusion, we observe that for Z∈CUf, Z must be
of ”degree 0” with regards to δ that is:
[TABLE]
where kℓ=0 for at most finitely many terms. Thus
C_{U_{f}}\subseteq\mathbb{C}[x]\bigg{[}\frac{1}{x+k}~{}\bigg{|}~{}k\in\mathbb{Z}\bigg{]}.
∎
We can now prove that Uf is a Galois CUf-order using
Theorem 6.2.
Corollary 6.8**.**
The algebra Uf is a principal and co-principal Galois CUf-order
in L#M.
Proof.
Proposition 6.7 gives us that
the main supposition of Theorem 6.2.
All that remains to show is DUf,DUfop⊂S−1Λ=CUf in this case.
However, this is clear since Uf is generated by X, Y, and Λ.
∎
6.3. Localizing A(gln)
In this subsection, we construct a localization of A(gln) denoted
A(gln), to which Theorem 6.2.
can be applied.
In order to construct this localization, we describe shifted Vandermonde
polynomials using the following notation:
Notation.
Let Vk be the Vandermonde in the xki variables. Let
l:=(l1,l2,…,lk−1)∈Zk−1. We denote the (l-)shifted Vk as follows:
[TABLE]
This notation makes sense because for i<j:
[TABLE]
Therefore, any shift of Vk is uniquely determined by the shifts of xki−xk,i+1 for
i=1,2,…,k−1.
Now to construct our localization.
Definition 6.9**.**
Let S:=⟨Vk,l∣l∈Zk−1;k=2,…,n−1⟩monoid.
We observe that S is a multiplicatively closed set in Λ, and
A(gln)⊂(S−1Λ#M)An. We also note
that S is the smallest M-invariant multiplicatively closed set
that contains V2,…,Vn−1.
As Example 4.2 demonstrates,
CA(gln)(Γ)⊂(S−1Λ)An.
It is not known if this containment is strict, so this motivates the construction
of the following localization of A(gln).
Definition 6.10**.**
Our new algebra of interest in K is
A(gln):=C⟨Un,(S−1Λ)An⟩alg.
Notice this coincides with the definitions of A(gl2) for n=2.
Remark 3*.*
It follows from Lemma 2.10 in [14] that A(gln)
is a Galois Γ-ring since it contains A(gln).
Moreover, CA(gln)(Γ)=(S−1Λ)An
as well.
Remark 4*.*
In A(gln), relation (9) from
Section 4.2 can be rewritten either as
The subalgebra A(gln)⊂K is both a principal and co-principal
Galois (S−1Λ)An-order.
Proof.
It is clear by construction that A(gln) satisfies the main supposition
of Theorem 6.2.
Also, it follows from the definition of the aki±’s in
(4) that
DA(gln),DA(gln)op⊆S−1Λ. We can therefore apply
Theorem 6.2.
∎
In [21], it was shown that every (co-)principal Galois order has a corresponding (co-)principal
flag order. This leads us to the following:
Open Problem 2**.**
What is the corresponding (co-)principal flag order of A(gln)?
7. (Generic) Gelfand-Tsetlin Modules over A(gln)
7.1. Some general results
Following the techniques in [3] and [14],
we construct canonical simple Gelfand-Tsetlin modules over A(gln). We need the
following additional assumptions for these next two results:
[TABLE]
Let Γ^ be the set of all Γ-characters (i.e., \mathbbmk-algebra homomorphisms
ξ:Γ→\mathbbmk).
Definition 7.1**.**
Let U be a Galois Γ-ring in K. A left
U-modules V is said to be a Gelfand-Tsetlin module (with
respect to Γ) if Γ acts locally finitely on V. Equivalently:
[TABLE]
Similarly, one can define a right Gelfand-Tsetlin modules.
The details for the following lemma can be found in [2].
Lemma 7.2**.**
Let U be a Galois Γ-ring in K.
(1)
Any submodule and any quotient of a Gelfand-Tsetlin module is a
Gelfand-Tsetlin module.
2. (2)
Any U-module generated by generalized weight vectors is a
Gelfand-Tsetlin module.
Let ξ∈Γ^ be any character. If U is a co-principal Galois
Γ-order in K, then the left cyclic U-module
Uξ has a unique simple quotient V′(ξ). Moreover,
V′(ξ) is a Gelfand-Tsetlin over U with V′(ξ)ξ=0
and is called the canonical simple left Gelfand-Tsetlin U-module
associated to ξ.
7.2. The case of A(gln)
We note that for n≥3 that Λ is not finitely generated as a
C-algebra. This prevents us from using all of the results as is, but all is not
lost. The main arguments of Theorem
7.3 rests on:
[TABLE]
If we want a similar result for S−1Γ we need to recall that
every maximal ideal m of S−1Γ is of the form
S−1p, where p is a prime (not necessarily maximal)
ideal of Γ∖S. Therefore we have the following result.
Theorem 7.4**.**
Let ξ be a character of S−1Γ such that
kerξ=S−1m, for some maximal ideal m of
Γ. Then the left cyclic module A(gln)ξ has a unique
simple quotient V′(ξ) which is a Gelfand-Tsetlin module over
A(gln) with V′(ξ)ξ=0.
Proof.
The key difference in this proof compared to Theorem
7.3 is observing that
[TABLE]
Otherwise, the proof follows the same structure.
∎
Since A(gln) is created by localizing Γ and Λ, we can view
any A(gln)-module V as a A(gln)-module by precomposing
with the embedding ι:A(gln)↪A(gln).
8. Gelfand-Kirillov Conjecture for A(gln)
In this section we will discuss for which n’s the algebras A(gln) and
A(gln) satisfy the Gelfand-Kirillov Conjecture. This is related to the
Noncommutative Noether Problem for the alternating group An, as discussed in
[10].
An algebra A is said to satisfy Gelfand-Kirillov Conjecture if it
is birationally equivalent to a Weyl algebra. That is its skew-field of fractions
is isomorphic to a skew Weyl field.
Lemma 8.1**.**
Frac(A(gln))=Frac(A(gln)).
Proof.
This follows because A(gln) is created by localizing Γ and
Λ.
∎
Hence, A(gln) and A(gln) either both will or will not satisfy
the Gelfand-Kirillov Conjecture for each n.
Proposition 8.2**.**
For every n,
[TABLE]
where Wk(C)
is the k-dimensional Weyl algebra over C.
Proof.
It is clear by construction that:
[TABLE]
Since L=Frac(Λ):
[TABLE]
We now recall that M is generated by δki’s and δki fixes
xℓj if ℓ=k. As such, we have:
[TABLE]
where Λk=C[xk1,…,xkk]⊂Λ and Mk=⟨δki∣1≤i≤k⟩grp≤M. Now, the k-th component
of An acts only on the k-th component of the tensor product. Therefore:
We finish the proof by observing that Frac(Λn)≅C(x1,…,xn)
and Λk#Mk≅Wk(C) by sending δkixki↦Xi and
(δki)−1↦Yi.
∎
We recall for readers both the classical Noether’s problem and the
noncommutative Noether’s problem as stated in [10].
The classical problem asks, given a finite group G and a rational function field
\mathbbmk(x1,…,xn) over a field \mathbbmk such that G acts linearly
on \mathbbmk(x1,…,xn), is \mathbbmk(x1,…,xn)G a purely transcendental
extension of \mathbbmk. The noncommutative problem exchanges the rational function field
with the skew field of fractions of a Weyl algebra and asks if the G invariants are the skew
field of some purely transcendental extension of \mathbbmk.
If G satisfies the Commutative Noether’s problem, then G satisfies the Noncommutative
Noether’s Problem.
Noether’s problem for An is still open for n≥5. However, we obtain the following
result:
Theorem 8.4**.**
If the alternating groups A1,A2,…,An provide a positive solution to Noether’s problem, then
A(gln) satisfies the Gelfand-Kirillov conjecture.
Proof.
If Ak satisfies Noether’s problem, then
Frac(Wk(C))Ak≅Frac(Wk(C)). The rest follows from
Proposition 8.2.
∎
Hence, as a corollary to Theorem 8.4
and Maeda’s results in [17], we have:
Corollary 8.5**.**
For n≤5, A(gln) satisfies the Gelfand-Kirillov Conjecture.
Acknowledgements
The author would like to thank his advisor Jonas Hartwig for guidance and helpful
discussion. The author would also like to thank João Schwarz for his comments and helpful discussion. Finally, the author would like to thank Iowa State University, where the author resided during the completion of this work.
Bibliography21
The reference list from the paper itself. Each links out to its DOI / PubMed record.
1[1] V. V. Bavula. Generalized Weyl algebras and their representations. St. Petersbg. Math. J. , 4(1):71–92, 1992.
2[2] Y.A. Drozd, V.M. Futorny, and S.A. Ovsienko. Harish-chandra subalgebras and Gelfand-Zetlin modules. Finite Dimensional Algebras and Related Topics , 424, 1994.
3[3] Nick Early, Volodymyr Mazorchuk, and Elizaveta Vishnyakova. Canonical Gelfand–Zeitlin modules over orthogonal Gelfand–Zeitlin algebras. International Mathematics Research Notices , Feb 2019. rnz 002.
4[4] Vyacheslav Futorny, Dimitar Grantcharov, Luis Enrique Ramírez, and Pablo Zadunaisky. Gelfand-Tsetlin Theory for Rational Galois Algebras. ar Xiv e-prints , page ar Xiv:1801.09316 , Jan 2018.
5[5] Vyacheslav Futorny and Jonas Hartwig. Solution of a q-difference Noether problem and the quantum Gelfand–Kirillov conjecture for 𝔤 𝔩 n subscript 𝔤 𝔩 𝑛 \operatorname{\mathfrak{gl}}_{n} . Mathematische Zeitschrift , 276, 02 2014.
6[6] Vyacheslav Futorny, Alexander Molev, and Serge Ovsienko. The Gelfand–Kirillov conjecture and Gelfand–Tsetlin modules for finite w-algebras. Advances in Mathematics , 223(3):773 – 796, 2010.
7[7] Vyacheslav Futorny and Serge Ovsienko. Galois orders in skew monoid rings. Journal of Algebra , 324(4):598 – 630, 2010.
8[8] Vyacheslav Futorny and Serge Ovsienko. Fibers of characters in Gelfand-Tsetlin categories. Transactions of the American Mathematical Society , 366, 08 2014.