A characterization of unitarity of some highest weight Harish-Chandra modules
Abstract.
Let be a highest weight Harish-Chandra module with highest weight . When the associated variety of is not maximal, that is, not equal to the nilradical of the corresponding parabolic subalgebra, we prove that the unitarity of can be determined by a simple condition on the value of , where is half the sum of positive roots and is the highest root. In the proof, certain distinguished antichains of positive noncompact roots play a key role.
By using these antichains, we are also able to provide a uniform formula for the Gelfand–Kirillov dimension of all highest weight Harish-Chandra modules, generalizing our previous result for the case of unitary highest weight Harish-Chandra modules.
Key words and phrases:
Unitary highest weight module, associated variety, Gelfand–Kirillov dimension2020 Mathematics Subject Classification:
22E47, 17B101. Introduction
Let be a connected non-compact simple Lie group with finite center, and let be a maximal compact subgroup. From the work of Harish-Chandra (see comments in [BHXZ, §3.2]), it follows that infinite-dimensional highest weight Harish-Chandra modules for exist if and only if (, ) is a Hermitian symmetric pair. The problem of determining when a highest weight Harish-Chandra module is unitarizable has been extensively studied by various authors (see, for example, the references in [EHW]). The full classification was independently completed in [EHW] and [Ja1], though the classification itself is rather intricate. In this paper, we provide a simple and uniform characterization of unitarity for Harish-Chandra modules with a given associated variety, expressed in terms of the highest weight (see Theorem 1.1).
From now, we assume that is a Hermitian symmetric pair. We denote by the complexification of the compact group and by the complexified Lie algebras of . Then we have the usual decompositition of as a -representation. Let be a Cartan subalgebra. Then is a Cartan subalgebra of . Let and denote the root systems of and , respectively. Let be the positive system of , and define and . Let denote the unique maximal noncompact root of . Now choose so that is orthogonal to and ()=1. Let be -dominant integral and be the irreducible -module with highest weight . By letting the nilradical act by zero, we may consider as a module of the parabolic subalgebra . Then we define:
Let denote the irreducible quotient of , which is a highest weight module of .
From [EHW], is a highest weight Harish-Chandra module if and only if , where
Write for half the sum of positive roots in . Then we can write , with such that ()=0, and .
The associated variety of a highest weight Harish-Chandra module is known to be the closure of a single -orbit in (see §3 for more details). Furthermore, the closures of the -orbits in form a linear chain of varieties
where is the -rank of , i.e., the dimension of a Cartan subgroup of the group , which is also equal to the rank of the symmetric space . Therefore, if is a highest weight Harish-Chandra module with highest weight , then there is an integer such that the associated variety of is .
Denote
(1.1) |
for . Here is a real number associated with the Hermitian type Lie group , see Table 1.
In this paper, we will prove the following result.
Theorem 1.1.
Let and suppose with . Then
is unitarizable if and only if . |
Remark 1.2.
Note that when , it may happen that there is more than one point such that is unitarizable.
In [BH], we have found a uniform formula for the Gelfand–Kirillov dimensions of unitary highest weight Harish-Chandra modules. Now we want to generalize our formula to all highest weight Harish-Chandra modules.
Definition 1.3.
For , define:
Here denotes the smallest integer such that .
Definition 1.4.
Let .
-
(a)
If is of type , for , define
-
(b)
If is of type , for , define
In the special case when , we also write instead of (This coincides with our definition of in (1.1)).
Our new formula for the Gelfand–Kirillov dimensions of all highest weight Harish-Chandra modules is as follows.
Theorem (Theorem 6.3).
Suppose is a reduction point. Then
-
(a)
If is of type , then and
-
(b)
If is of type , then or and
2. Distinguished antichains of positive noncompact roots
Note that for any integer , the set
is an antichain in .
Let denote the set of simple roots in .
Lemma 2.1 ([Ja1, Lemma 4.1]).
Let , let be distinct elements of , and assume that for . Then . Furthermore, if , then and .
In light of this lemma, the Hasse diagram of is an upward planar graph of order dimension two and hence can be drawn on a two-dimensional orthogonal lattice that has been rotated by a -degree angle.
Example 2.2.
Let . Then we have
The antichains in are given in Appendix.
A subset is called a lower-order ideal if, for and , implies that .
Definition 2.3.
For , define the diagram of as the set
(2.1) |
viewed as a subposet of , where is the integral root system associated to .
By [BHXZ, Lem 2.2], the poset is a lower order ideal of when is integral.
An antichain in a poset is a subset consisting of pairwise noncomparable elements. The width of a poset is the cardinality of maximal antichain in the poset. Suppose , we use to denote the width of .
By inspection of the Hasse diagram of , we have the following lemma.
Lemma 2.4.
Suppose be a lower order ideal. If is the width of , then there exists an antichain of length such that all the roots in have the same height.
Lemma 2.5.
Let . If with , then for some .
Recall that is an antichain in .
Proof.
Suppose with .
When is simply-laced, by our main theorem in [BHXZ], is integral and . Assume that for all . Since is an antichain of length , it would follow that . Contradiction.
When is non-simply-laced and is even, by our main theorem in [BHXZ], is integral and . Assume that for all . Since is an antichain of length , it would follow that . Then . Contradiction!
When is non-simply-laced and is odd, by our main theorem in [BHXZ], is half-integral and . Assume that for all . Since is an antichain of length , it would follow that . Then . Contradiction!
∎
3. Gelfand–Kirillov dimension and associated variety
In this section, we will recall some preliminaries on Gelfand–Kirillov dimensions and associated varieties of highest weight modules. See [Vo78, Vo91] for more details.
Let be a finite generated -module. Fix a finite dimensional generating space of . Let be the standard filtration of . Set and where . Thus is a graded module of .
The Gelfand–Kirillov dimension of is defined by
The associated variety of is defined by
These two definitions are independent of the choice of , and (e.g., [NOT]). If is -invariant for a subalgebra , then
(3.1) |
When is a highest weight Harish-Chandra module, we can choose to be the finite dimensional -module generated by . Then is -invariant. In view of (3.1),
where the last isomorphism is induced from the Killing form. As shown in [Vo91], the associated variety is also -invariant. In fact, Yamashita [Hir01] proved that must be one of .
Lemma 3.1.
Let be a highest weight Harish-Chandra module. Then
for some .
We have the following table from [EHW]:
In [BH], we have found a uniform expression for the GK dimensions and associated varieties of unitary highest weight Harish-Chandra modules.
Proposition 3.2 ([BH]).
Suppose is a unitary highest weight Harish-Chandra module with highest weight . We denote , then
Denote . Then
-
(1)
If , we have
-
(2)
If , then is a non-negative integer and
The associated variety of is .
4. Proof of the main theorem: simply-laced cases
In this section, we assume that is simply-laced.
For any integer , is the antichain in such that and with minimal.
To prove our Theorem 1.1, we need the following useful lemma.
Lemma 4.1.
Let . If and , then, for any ,
Proof.
Let . Since is simply-laced, and . Thus,
∎
Now we can prove our Theorem 1.1. The idea is very simple. From Lemma 2.5, since , we have for some . Then . So if , we will have
This condition is very restrictive. In the following, we will give a case-by-case discussion for this condition, which will imply the unitarity of .
4.1. Case
For ,
(Here and in the following we write , where are the simple roots.)
4.2. Case
For ,
Fix . Then, since ,
In the first case, , and hence (-th Wallach representation).
In the second case, . It follows that
So is of the form
By [EW], [EHW] or [DES], is unitary.
In the first case, , and hence (unitary reduction point).
In the second case, . It follows that
So is of the form
By [EW], [EHW] or [DES], is unitary.
4.3. Case
For ,
Fix . Then, since ,
In the first case, we have . Hence (unitary reduction point).
In the second case, we have . Hence (unitary reduction point).
4.4. Case
By inspection of the Hasse diagram of ,
Fix . Then, since ,
4.5. Case
By inspection of the Hasse diagram of ,
Fix . Then, since ,
5. Proof of the main theorem: non-simply-laced cases
In this section, we assume that is not simply-laced.
For any integer , is the antichain in such that and with minimal.
The proof of Theorem 1.1 in non-simply-laced cases is similar to the simply-laced cases. We need Lemma 2.5 and the following useful lemma in the computation.
Lemma 5.1.
Let . If and , then, for any ,
and
Proof.
Let . Since is not simply-laced, if is a long root and if is a short root. . Thus, if is a long root, we have
If is a short root, we have
∎
5.1.
For ,
Fix . Then, since ,
Now suppose such that with and . By Lemma 2.5, for some . So if is even, by Lemma 5.1 we have
or
In the first case, and hence
By [EHW] or [EW], is unitary.
In the second case, and or at most one of equals to with the rest queal to . Hence
By [EHW] or [EW], is unitary.
If is odd, we have
then the arguments are similar to the above case.
5.2.
For ,
Fix . Then, since ,
In the first case, it follows that (1st Wallach representation).
In the second case, we have (unitary reduction point).
6. A uniform formula for the Gelfand–Kirillov dimension
In our previous paper [BH], we found a uniform formula for the Gelfand–Kirillov dimensions of all unitary highest weight modules. Now we will give a new formula for the Gelfand–Kirillov dimensions of all highest weight Harish-Chandra modules.
We recall the definition of in the introduction. Then we have the following lemma.
Lemma 6.1.
Suppose is of type . For , we have
Proof.
It is easy to verify (case-by-case) that
For , we have
∎
We recall the main theorem in [BHXZ].
Proposition 6.2 ([BHXZ]).
Suppose is a highest weight Harish-Chandra module with highest weight and . Let . Then is given as follows.
-
(a)
If is simply laced and is integral, then .
-
(b)
If is non-simply laced and is integral, then
-
(c)
If is non-simply laced and is half-integral, then
-
(d)
In all other cases .
In the following, we give the new formula for the Gelfand–Kirillov dimensions of all highest weight Harish-Chandra modules.
Theorem 6.3.
Suppose is a reduction point. Then
-
(a)
If is of type , then and
-
(b)
If is of type , then or and
Proof.
In the following, suppose .
(a) In type , if is a reduction point, then by [EHW].
Thus, we have
The formula then follows from our main theorem (in type ) in [BHXZ].
(b) In type , if is a reduction point, then by [EHW].
When is integral, then . Thus, when is even, we have
When is half-integral, then . Thus, when is odd, we have
In particular, . When is half-integral, we also know that is not finite-dimensional. Thus with
The formula then follows from our main theorem (in type ) in [BHXZ].
∎
The following result was firstly proved in [BH]. Now we give a new proof.
Corollary 6.4.
Suppose is a unitary highest weight Harish-Chandra module with highest weight . We denote , then
Proof.
First we suppose that is a unitary highest weight Harish-Chandra module and for some .
From Yamashita [Ya-94] we have for some . From Theorem 1.1, we will have since is unitarizable. Thus we must have , which implies that . So we must have .
Now we suppose that is a unitary highest weight Harish-Chandra module and . From Yamashita [Ya-94] we still have for some . If , by Theorem 1.1 we will have since is unitarizable. From our assumption, we will have , which implies that
This is a contradiction! So we must have and . ∎
Example 6.5.
Let and let be a highest weight Harish-Chandra module with highest weight . Here , and . From [EHW], we know the unitary reduction points correspond to and . For , we know
So , , .
Example 6.6.
Let and let be a highest weight Harish-Chandra module with highest weight . Here , and . From [EHW], we know the unitary reduction points correspond to and . For , we know
So , , , , , .
Acknowledgments
Z. Bai was supported by the National Natural Science Foundation of China (No. 12171344).
7. Appendix
The diagrams of .
:
For ,
:
For ,
:
:
:
:
:
For ,