On the semisimple orbits of restricted Cartan type Lie algebras W, S and H
Hao Chang and Ke Ou
School of Mathematics and Statistics, Central China Normal University, 430079 Wuhan, People’s Republic of China
[email protected]
School of Statistics and Mathematics, Yunnan University of Finance and Economics, 650221 Kunming, People’s Republic of China
[email protected]
Abstract.
In this short note,
we give a description of semisimple orbits in
the restricted Cartan type Lie algebras W,S,H.
Key words and phrases:
Weyl groups, Lie algebras of Cartan type, semisimple orbits.
2010 Mathematics Subject Classification:
17B05, 17B50
1. Introduction
Let (g,[p]) be a restricted Lie algebra with connected automorphism group Gg:=Autp(g)∘.
The algebraic group Gg acts naturally on the constructible set Sg of semisimple elements of g.
A basic problem is to understand the set Sg/Gg of semisimple Gg-orbits.
In the classical case,
where g:=Lie(G) is the Lie algebra of a connected reductive group G,
all maximal tori of g are G-conjugate (hence Gg-conjugate) and there is a bijective correspondence Sg/G→t/W,
where t is a maximal torus and W its corresponding Weyl group (cf. [5, (7.12)]).
If g is not an algebraic Lie algebra,
then maximal tori are not necessarily Gg-conjugate.
In fact,
for the non-classical simple Lie algebras (which,
by the classification theorem of Block-Wilson-Premet-Strade (cf. [9]),
are of Cartan type provided that the characteristic of k is larger than 5),
the maximal tori are not all conjugate under the action
of the automorphism group ([9, Chapter 7]).
In this paper, we study Lie algebras of Cartan type g:=W,S,H.
In these cases, g possesses finitely many Gg-conjugacy classes of maximal tori.
These algebras have a natural filtration
[TABLE]
by [p]-stable subspaces.
Let ⟨x⟩p denote the torus generated by a semisimple element x∈Sg.
We define a function
[TABLE]
whose fibers are Gg-stable.
Given a maximal torus tg of g,
we consider the Weyl group W(g,tg) relative to tg,
defined via W(g,tg):=NGg(tg)/CGg(tg),
where NGg(tg) and CGg(tg) are the normalizer and the centralizer of tg in Gg,
respectively.
Using basic results on tori,
due to Demushkin [2, 3],
every maximal torus tg⊆g has the same dimension μ(g).
Moreover,
up to conjugacy,
every integer 0≤r≤μ(g) gives rise to a unique maximal torus tg,r
such that Indg(x)≤r for all x∈tg,r and tg,rr:=Indg−1(r)∩tg,r=∅.
The W(g,tg,r)-orbits on tg,r are distinguished by the values of invariant functions,
and the invariants were determined by the second author in [7, Proposition 3.2]. Actually, in the case r=μ(g), the isomorphism W(g,tg,μ(g))≅GLμ(g)(Fp) was established in [8] and [1], and the invariant functions on tg,μ(g) under GLμ(g)(Fp) action were determined in a classical work of L. Dickson [4].
The main result reads:
Theorem**.**
Let r∈{0,1,…,μ(g)}.
Then there is a bijective correspondence
[TABLE]
More details refer to Theorem 3.6.
We will give description the quotients tg,rr/W(g,tg,r) by employing p-polynomials in Proposition 3.7 respectively.
Throughout this paper, k denotes an algebraically closed field of characteristic char(k)=:p>3.
Acknowledgments. This work is supported by NSFC (No. 11801204),
NSF of Yunnan Province (No. 2020J0375),
the Fundamental Research Funds of YNUFE (No. 80059900196).
We are indebted to the referee for
carefully reading the manuscript and providing numerous comments.
2. Preliminaries
2.1. Cartan type Lie algebras type W,S,H
Let A(n):=k[X1,…,Xn]/(X1p,…,Xnp) be the truncated polynomial ring in n variables.
We write xi for the image of Xi in A(n).
Note that A(n) is a finite-dimensional local algebra,
with maximal ideal m:=⟨x1,…,xn⟩.
The Lie algebra W(n):=Der(A(n)) is called the n-th Jacobson-Witt algebra.
It is an A(n)-module in an obvious way,
and has a standard basis {x1α1⋯xnαn∂i; 0≤αj<p,1≤i≤n}
where ∂i denotes the partial derivative with respect to the variable xi.
Define the linear map div:W(n)→A(n) by
[TABLE]
The Lie algebra S(n) is defined via S(n):={∂∈W(n); div(∂)=0}
and the derived algebra S(n)(1) is called special algebra.
If n≥3,
then S(n)(1) is restricted and simple.
Let us move on to the family H(2m).
For i∈{1,…,2m}, we put
[TABLE]
In addition, we define
[TABLE]
Let H(2m):={i=1∑2mfi∂i∈W(2m); σ(i)∂j′(fi)=σ(j)∂i′(fj) 1≤i,j≤2m}.
The Lie subalgebra H(2m)(2) of H(2m) is simple and restricted, and we call it a Hamiltonian algebra.
From now on we will (by abuse of notation) write W(n),
S(n) and H(n) for the corresponding simple derived subalgebra,
with the convention that n=2m for the Hamiltonian type.
Suppose that g=X(n), where X∈{W,S,H}. By definition, it possesses a restricted Z-grading
[TABLE]
Given such an algebra g,
we consider the associated descending filtration (g(i))i≥−1,
defined via
[TABLE]
2.2. Automorphism groups
Let us gather some facts on automorphisms.
It is well known that we have an isomorphism Aut(A(n))≅Autp(W(n));
φ↦σφ,
given by
[TABLE]
for all ∂∈W(n).
If g∈{W,S,H},
then the group Autp(g) is connected, i.e. Gg=Autp(g),
and we have
[TABLE]
Moreover,
the group Gg is a semidirect product G0⋉U,
where G0 consists of those
automorphisms preserving the Z-grading (2.1) of g and U is the unipotent radical ([10]).
It is a consequence of the semidirect product decomposition that
[TABLE]
for every g∈Gg and i∈Z.
Recall that the Poisson Lie algebra structure on A(2m) is given by {f,g}=DH(f)(g) for all f,g∈A(2m) (cf. [9, Section 4.2]),
where the linear map DH is defined by
[TABLE]
For ease of reference we record the following well-known result:
Lemma 2.1**.**
[9, Theorem 7.3.4, 7.3.6]**
Let φ∈Aut(A(n)).
Then σφ induces an automorphism of S(n) if and only if
[TABLE]
and σφ induces an automorphism of H(n) if and only if
[TABLE]
for some a∈k∖{0} and all i,j.
2.3. Maximal tori
Given a restricted Lie algebra (g,[p]),
we let μ(g) denote the maximal dimension of all tori t⊆g and let
[TABLE]
be the set of tori of maximal dimension.
In the case of restricted Cartan type Lie algebras,
every maximal torus has maximal dimension (cf. [9, Section 7.5]).
Assume that g∈{W,S,H}.
Since the natural filtration (2.2) is stable under the action of Gg,
it follows that the function
[TABLE]
is constant on the Gg-orbits of Tor(g).
As shown by Demushkin in [2, 3],
there are exactly μ(g)+1 orbits O0,…,Oμ(g) in Tor(g) under the Gg-action,
and these have the following description:
[TABLE]
For each of the three Cartan types we have canonical orbit representatives tg,r of Or
given by
[TABLE]
where
[TABLE]
[TABLE]
[TABLE]
2.4. Weyl groups of W,S,H
Let (g,[p]) be a restricted Lie algebra with connected automorphism group Gg,
t⊆g be a torus and we let NGg(t) and CGg(t) be the normalizer and the centralizer of t in Gg,
respectively.
The group
[TABLE]
is referred to as the Weyl group of g relative to t.
For the three Cartan types W,S and H,
we are interested in the Weyl group relative to maximal torus.
Let t∈Tor(g).
Since W(g,g.t)≅W(g,t) for every g∈Gg,
the Weyl group W(g,t) only depends on the orbit Gg.t⊆Tor(g).
We may hence assume that t=tg,r (2.8),
(2.9),
(2.10) for some 0≤r≤μ(g).
The following result was proved by Jensen in [6],
Prop. 3.6:
Proposition 2.2**.**
Assume g∈{W,S,H}.
Then
W(g,tg,r)≅(W1×W2)⋉W3,
with
[TABLE]
[TABLE]
[TABLE]
3. Semisimple orbits in W,S,H
3.1. Semisimple elements in the standard tori
Assume that g∈{W,S,H}.
If x∈Sg is a semisimple element,
then ⟨x⟩p denotes the torus generated by x.
We define a function
[TABLE]
The index of an element x is defined as Indg(x).
In view of Section 2.3,
we have Indg(Sg)={r∈N0; 0≤r≤μ(g)}.
Given r∈{0,1,…,μ(g)},
it follows from (2.4) that each fiber Indg−1(r) is Gg-stable.
Clearly, Sg is the disjoint union of all fibers, i.e.,
[TABLE]
Indeed,
dimktg,r/(tg,r∩g(0))=r implies that
[TABLE]
We denote by tg,rr:=tg,r∩Indg−1(r) the set of those elements of tg,r whose index is r.
If r=0, then (3.2) yields tg,00=tg,0.
Note that the dimension Indg(x) does not change when x is replaced by its Gg-conjugate.
Observing (2.8), (2.9) and (2.10),
we conclude that Indg−1(0) is just the Gg-saturation Gg.tg,0.
We put yi:=xi+1.
In order to describe the set Indg−1(r),
we introduce the following notations:
[TABLE]
[TABLE]
[TABLE]
[TABLE]
The following lemma is well-known. We provide a proof here for convenience.
Lemma 3.1**.**
Given a restricted Lie algebra (l,[p]), we let t⊆l be a torus with basis {t1,…,tn} such that ti[p]=ti for 1≤i≤n.
If t=∑i=1nλiti∈t, then t=⟨t,t[p],⋯,t[p]n−1⟩ if and only if λ1,…,λn are Fp-linearly independent.
Proof.
It is clear that {t,t[p],⋯,t[p]n−1} is linearly independent if and only if det((λipj−1)1≤i,j≤n)=0.
Since det((λipj−1)1≤i,j≤n)=∏i=1n∏a1,⋯,ai−1∈Fp(a1λ1+⋯+ai−1λi−1+λi) (see [4, Section 2] for example), we have det((λipj−1)1≤i,j≤n)=0 if and only if λ1,…,λn are Fp-linearly independent.
∎
Lemma 3.2**.**
Keep the notations as above.
Let 1≤r≤μ(g) and tg,r be the standard maximal torus with basis {d1g,r,…,dμ(g)g,r}.
Suppose that d=∑i=1μ(g)λidig,r∈tg,r.
Then d∈tg,rr if and only if λ1,…,λr are Fp-linearly independent.
Proof.
If λ1,…,λr are linearly independent over the prime field Fp,
then the coset of d modulo tg,r∩g(0) generates an r dimensional torus by Lemma 3.1,
so that Indg(d)=dimk⟨d⟩p/(⟨d⟩p∩g(0))=r, i.e. d∈tg,rr.
Conversely, if λ1,…,λr are Fp-linearly dependent,
then
[TABLE]
where m<r, αi∈k and each ti is a linear combination of d1g,r,…,dμ(g)g,r
with coefficients in Fp.
In this case
[TABLE]
and it is immediately clear that Indg(d)<r.
∎
Lemma 3.3**.**
Suppose that d=∑i=1μ(g)λidig,r∈tg,r.
If λ1,…,λr are Fp-linearly dependent,
then there exists σφ∈Gg such that σφ(d)∈tg,r−1.
Proof.
By assumption,
there exist ui∈Fp such that ∑i=1ruiλi=0.
We may assume without loss of generality that ur=−1,
so that λr=∑i=1r−1uiλi.
We put (u):=(u1,…,ur−1) and define y(u):=y1u1⋯yr−1ur−1.
Assume first that g=W(n).
We define an automorphism of A(n) by
[TABLE]
Using (2.3)(see also the formula in [2, p. 234])) one can show by direct computation that
[TABLE]
Assume now g=S(n).
Define φ∈Aut(A(n)) by
[TABLE]
As det(∂i(φ(xj)))=1,
Lemma 2.1 ensures that σφ∈Gg.
Then we have:
[TABLE]
Finally the case g=H(n),
with n=2m for some m≥1.
Using multi-index notation (see [9, Section 2.1]),
we define
[TABLE]
Observing det(∂i(φ(xj)))=1,
we thus obtain φ∈Aut(A(n)).
Moreover, we claim that
[TABLE]
We just deal with i=r,
the other cases are similar.
Suppose that 1≤j≤m.
Since both φ(xr) and φ(xj) lie in the algebra A(m),
it follows that {φ(xr),φ(xj)}=0.
If m+1≤j≤m+r−1,
then
[TABLE]
[TABLE]
Now for m+r≤j≤2m,
so that {φ(xr),φ(xj)}={xr+y(u)−1,xj}=δr′,j.
This establishes our claim.
Consequently,
Lemma 2.1 implies that σφ∈Gg.
By the same token,
we have
[TABLE]
∎
Corollary 3.4**.**
Assume g∈{W,S,H} and let x∈Sg be a semisimple element of g.
Then
[TABLE]
Let r∈{0,1,…,μ(g)}.
In particular, up to conjugacy,
there exists a unique maximal torus t such that t∩Indg−1(r)=∅ and Indg(x)≤r for all x∈t.
Proof.
We put l:=min{r; Gg.x∩tg,r=∅, 0≤r≤μ(g)}.
we may assume that x∈tg,l.
Now Lemma 3.2 and Lemma 3.3 in conjunction with the minimality of l yields x∈tg,ll.
Consequently,
Indg(x)=l.
To verify the last assertion,
we note that Indg(x)≤r for all x∈tg,i and i≤r (3.2).
In view of (3.6),
we obtain tg,i∩Indg−1(r)=∅ whenever i<r.
This proves the uniqueness.
∎
3.2. Semisimple orbits
In this section,
we turn to the set Indg−1(r)/Gg
for the restricted Cartan type Lie algebra g∈{W,S,H}.
We have seen in the foregoing section that the set Indg−1(r) coincides with the Gg-saturation Gg.tg,rr.
It will be necessary to consider the Gg-conjugacy relation on the set tg,rr.
Lemma 3.5**.**
Assume that g∈{W,S,H} with connected automorphism group Gg.
Let d,t∈tg,rr.
If d and t are conjugate under Gg,
then there exists σψ∈NGg(tg,r) such that σψ(d)=t.
Proof.
Let σφ∈Gg be such that σφ(d)=t.
We write d=∑i=1μ(g)βidig,r as well as t=∑i=1μ(g)αidig,r.
Define
[TABLE]
Setting β=(β1,⋯,βμ(g)) and α=(α1,⋯,αμ(g)),
we apply (2.3) in conjunction with (3.3)-(3.5) to see that
[TABLE]
[TABLE]
[TABLE]
As a result,
fi is a weight vector with respect to the canonical action of t on A(n).
We claim that
(†) there exists matrices A,B,τ such that β=α(A0Bτ),
where A=(aij)∈GLr(Fp),B=(bij) and τ∈W1 (2.11).
Suppose that g=W(n).
Since φ∈Aut(A(n)),
the weight space decomposition ensures that
[TABLE]
[TABLE]
where τ is a permutation on {r+1,…,n}.
Assume now g=S(n).
We put αn:=−∑j=1n−1αj.
The same argument shows that
[TABLE]
[TABLE]
where τ is a permutation on {r+1,…,n}.
Finally consider the case g=H(2m).
As σφ∈Gg,
it follows that fj has the form (modulo the corresponding weight space) z1a1j⋯zrarj
with weight ∑i=1rαiai,j for every j∈{1,…,r}.
For r+1≤j≤m,
combining (2.6) with (3.9) one obtains that
fj has the term z1b1j⋯zrbrjxτ(j),
where τ is a permutation on {r+1,…,m,m+r+1,⋯,2m}.
In view of (2.6),
{fj,fj′} is a non-zero constant.
Direct computation shows that τ(j′)=τ(j)′.
so that τ can be identified with an element of Sm−r⋉Z2m−r,
where the copies of Z2 act by ′.
Consequently,
fj has weight ∑i=1rαibij+σ(τ(j))αω(j) with (ω,a)=τ∈Sm−r⋉Z2m−r.
Thanks to Lemma 3.2,
both {α1,⋯,αr} and {β1,⋯,βr} are Fp-linearly independent.
It follows that A∈GLr(Fp).
This proves (†).
Now, Proposition 2.2 ensures the existence of σψ.
∎
Theorem 3.6**.**
Assume that g∈{W,S,H}.
Let r∈{0,1,…,μ(g)}.
Then there is a bijective correspondence
[TABLE]
Proof.
Let x∈Indg−1(r).
Corollary 3.4 readily yields Gg.x∩tg,r=∅.
It follows that Indg−1(r) coincides with the Gg-saturation Gg.tg,rr.
The assertion now follows from Lemma 3.5.
∎
3.3. Quotients
In this section, we would like to give a description of the quotients tg,rr/W(g,tg,r) by employing p-polynomials.
Recall that a p-polynomial is a polynomial of the form
[TABLE]
For each x∈g, define f(x):=alx[p]l+al−1x[p]l−1+⋯+a0x∈g.
Let t⊆g be a torus.
Given a semisimple element x∈t,
there exists a monic p-polynomial fx(t) of lowest degree such that fx(x)=0.
It is unique and we call it the minimal p-polynomial of x.
By general theory, the orbit of an element x∈t with respect to the whole group Autp(t) is completely determined by the
minimal p-polynomial of x.
In the case r=μ(g),
according to Proposition 2.2 (see also [8, Theorem 1] and [1, Theorem 5.3]),
there is an isomorphism W(g,tg,μ(g))≅GLμ(g)(Fp).
Let x,y∈tg,μ(g).
The foregoing observation implies that x and y are in the same W(g,tg,μ(g))-orbit if and only if fx=fy.
For general r, let x∈tg,r.
We denote by xˉ the image of x under the canonical projection π:tg,r→tg,r/(tg,r∩g(0)).
Let fxˉ(t) be the minimal p-polynomial of xˉ.
It follows that fxˉ(t) is the monic p-polynomial of smallest degree such that fxˉ(x)∈g(0).
Proposition 3.7**.**
Keep the notations as before.
Let x,y∈tg,r.
Then x and y are in the same W(g,tg,r)-orbit if and only if fxˉ=fyˉ and
fxˉ(x),fyˉ(y) lie in the same W1-orbit (2.11).
Proof.
Let σ∈W(g,tg,r) be such that σ(x)=y.
The Weyl group W(g,tg,r) leaves invariant the subtorus tg,r∩g(0).
It follows that σ∈Autp(tg,r/(tg,r∩g(0))) and σ(xˉ)=yˉ.
Consequently, fxˉ=fyˉ.
Now, let fxˉ(t)=fyˉ(t)=tpl+al−1tpl−1+⋯+a0t.
We have
[TABLE]
Since W(g,tg,r) acts on the subtorus tg,r∩g(0) via the classical Weyl group W1,
there exists an element w∈W1 such that σ(fxˉ(x))=w(fxˉ(x))=fyˉ(y).
Conversely, denote f:=fxˉ=fyˉ. Let τ∈W1 be such that τ(f(x))=f(y).
We write x=(x′,x′′) and y=(y′,y′′) with x′,y′∈tg,r′ and x′′,y′′∈tg,r′′ (see (2.7)).
It is easy to see that f is also the minimal p-polynomial of x′ and y′.
General theory provides an invertible matrix A∈GLr(Fp) such that x′A=y′.
Since the p-polynomial is additive,
it follows that τ(f(x))=τ(f(x′+x′′))=τ(f(x′′))=f(y)=f(y′+y′′)=f(y′′).
As a result, f(x′+y′′−τ(x′′))=0.
Hence, f is the minimal p-polynomial of x′+y′′−τ(x′′).
By the same token, there exists an invertible matrix (BDCE)∈GLμ(g)(Fp) such that (x′,0)(BDCE)=(x′,y′′−τ(x′′)).
Consequently, (x′,x′′)(A0Cτ)=(y′,y′′),
and our assertion now follows
directly from Proposition 2.2.
∎
4. Normalizers and centralizers in W(n)
In this section,
g always denotes the n-th Jacobson-Witt algebra.
For convenience, we set tr:=tg,r, 0≤r≤n (see (2.8)).
We shall compute NGg(t) and CGg(t) for every t∈Tor(g).
Up to conjugacy,
we may thus assume that t=tr for some r∈{0,1,…,n}.
It should be noted that the isomorphisms
[TABLE]
were established by Premet (see [8, p. 139]).
Recall that tr=∑i=1nkzi∂i,
where zi=yi for 1≤i≤r and zi=xi for r+1≤i≤n (3.3).
Proposition 4.1**.**
Assume r∈{0,…,n}.
Then
[TABLE]
(∗)
If 1≤j≤r,
φ(zj)=∏i=1rzimij,
where (mij)1≤i,j≤r∈GLr(Fp).
If r+1≤j≤n,
φ(zj)=ajzτ(j)∏l=1rzlmlj,
where aj∈k∗, τ∈Sn−r,mlj∈Fp.
Proof.
Let φ∈Aut(A(n)) be such that σφ∈NGg(tr).
There exists an invertible matrix (mij)∈GLn(k) such that
[TABLE]
We put fj:=φ(zj),
then it is a simple exercise in linear algebra to show
[TABLE]
Note that {z1a1⋯znan; 0≤a1,…,an<p} is a k-basis of A(n)
consisting of weight vectors.
Our assertion follows from (4.2) in conjunction with the weight space decomposition.
∎
Corollary 4.2**.**
CGg(tr)≅(k∗)n−r.
In particular, CG(tr)=NG(tr)∘.
Proof.
As σφ∈CGg(tr),
direct computation shows that the weights zi and φ(zi) are the same.
The assertion follows by applying the similar argument as in Proposition 4.1.
∎