A topic on homogeneous vector bundles over elliptic orbits: A condition for the vector spaces of their cross-sections to be finite dimensional | Tomesphere
arXiv:1901.07818·math.DG·January 24, 2019
A topic on homogeneous vector bundles over elliptic orbits: A condition for the vector spaces of their cross-sections to be finite dimensional
This paper establishes a sufficient condition, based on root systems, for the vector spaces of holomorphic cross-sections of homogeneous vector bundles over elliptic orbits to be finite dimensional.
Contribution
It introduces a new criterion linking root systems to the finite dimensionality of cross-section spaces over elliptic orbits.
Findings
01
Provided a root system-based condition for finite dimensionality
02
Characterized when holomorphic cross-section spaces are finite dimensional
03
Enhanced understanding of vector bundle sections over elliptic orbits
Abstract
In this paper we consider the complex vector spaces of holomorphic cross-sections of homogeneous holomorphic vector bundles over elliptic adjoint orbits, and provide a sufficient condition for the vector spaces to be finite dimensional in view of root systems.
Equations128
\begin{array}[]{l}L:=C_{G}(T),\qquad\mbox{$\mathfrak{g}^{\lambda}:=\{X\in\mathfrak{g}_{\mathbb{C}}\,|\,\mathrm{ad}T(X)=i\lambda X\}$ for $\lambda\in\mathbb{R}$},\\
Q^{-}:=\{x\in G_{\mathbb{C}}\,|\,\mathrm{Ad}x\bigl{(}\bigoplus_{\mu\leq 0}\mathfrak{g}^{\mu}\bigr{)}\subset\bigoplus_{\mu\leq 0}\mathfrak{g}^{\mu}\},\end{array}
\begin{array}[]{l}L:=C_{G}(T),\qquad\mbox{$\mathfrak{g}^{\lambda}:=\{X\in\mathfrak{g}_{\mathbb{C}}\,|\,\mathrm{ad}T(X)=i\lambda X\}$ for $\lambda\in\mathbb{R}$},\\
Q^{-}:=\{x\in G_{\mathbb{C}}\,|\,\mathrm{Ad}x\bigl{(}\bigoplus_{\mu\leq 0}\mathfrak{g}^{\mu}\bigr{)}\subset\bigoplus_{\mu\leq 0}\mathfrak{g}^{\mu}\},\end{array}
\begin{split}&\mathcal{V}_{G_{\mathbb{C}}/Q^{-}}\!\!:=\!\!\left\{\begin{array}[]{@{}l@{\,\,}|l@{}}h:G_{\mathbb{C}}\to{\sf V}&\begin{array}[]{@{\!}l@{\!}}\mbox{(1) $h$ is holomorphic},\\
\mbox{(2) $h(xq)=\rho(q)^{-1}(h(x))$ for all $(x,q)\in G_{\mathbb{C}}\!\times\!Q^{-}$}\end{array}\end{array}\right\}\!\mbox{ and}\\
&\mathcal{V}_{G/L}\!\!:=\!\!\left\{\begin{array}[]{@{}l@{\,\,}|l@{}}\psi:GQ^{-}\to{\sf V}&\begin{array}[]{@{\!}l@{\!}}\mbox{(1) $\psi$ is holomorphic},\\
\mbox{(2) $\psi(yq)=\rho(q)^{-1}(\psi(y))$ for all $(y,q)\in GQ^{-}\!\times\!Q^{-}$}\end{array}\end{array}\right\}\end{split}
\begin{split}&\mathcal{V}_{G_{\mathbb{C}}/Q^{-}}\!\!:=\!\!\left\{\begin{array}[]{@{}l@{\,\,}|l@{}}h:G_{\mathbb{C}}\to{\sf V}&\begin{array}[]{@{\!}l@{\!}}\mbox{(1) $h$ is holomorphic},\\
\mbox{(2) $h(xq)=\rho(q)^{-1}(h(x))$ for all $(x,q)\in G_{\mathbb{C}}\!\times\!Q^{-}$}\end{array}\end{array}\right\}\!\mbox{ and}\\
&\mathcal{V}_{G/L}\!\!:=\!\!\left\{\begin{array}[]{@{}l@{\,\,}|l@{}}\psi:GQ^{-}\to{\sf V}&\begin{array}[]{@{\!}l@{\!}}\mbox{(1) $\psi$ is holomorphic},\\
\mbox{(2) $\psi(yq)=\rho(q)^{-1}(\psi(y))$ for all $(y,q)\in GQ^{-}\!\times\!Q^{-}$}\end{array}\end{array}\right\}\end{split}
dimCVGC/Q−<∞
dimCVGC/Q−<∞
\left\{\begin{array}[]{@{}l}\begin{array}[]{@{}ll}L:=C_{G}(T),&L_{\mathbb{C}}:=C_{G_{\mathbb{C}}}(T),\end{array}\\
\mbox{$\mathfrak{g}^{\lambda}:=\{X\in\mathfrak{g}_{\mathbb{C}}\,|\,\mathrm{ad}T(X)=i\lambda X\}$ for $\lambda\in\mathbb{R}$},\\
\begin{array}[]{@{}lll}\mathfrak{u}^{\pm}:=\bigoplus_{\lambda>0}\mathfrak{g}^{\pm\lambda},&U^{\pm}:=\exp\mathfrak{u}^{\pm},&Q^{\pm}:=N_{G_{\mathbb{C}}}(\mathfrak{l}_{\mathbb{C}}\oplus\mathfrak{u}^{\pm}),\end{array}\end{array}\right.
\left\{\begin{array}[]{@{}l}\begin{array}[]{@{}ll}L:=C_{G}(T),&L_{\mathbb{C}}:=C_{G_{\mathbb{C}}}(T),\end{array}\\
\mbox{$\mathfrak{g}^{\lambda}:=\{X\in\mathfrak{g}_{\mathbb{C}}\,|\,\mathrm{ad}T(X)=i\lambda X\}$ for $\lambda\in\mathbb{R}$},\\
\begin{array}[]{@{}lll}\mathfrak{u}^{\pm}:=\bigoplus_{\lambda>0}\mathfrak{g}^{\pm\lambda},&U^{\pm}:=\exp\mathfrak{u}^{\pm},&Q^{\pm}:=N_{G_{\mathbb{C}}}(\mathfrak{l}_{\mathbb{C}}\oplus\mathfrak{u}^{\pm}),\end{array}\end{array}\right.
T∈k,
T∈k,
Gu={gu∈GC∣θˉ(gu)=gu}.
Gu={gu∈GC∣θˉ(gu)=gu}.
(Eα−E−α),i(Eα+E−α)∈gu
(Eα−E−α),i(Eα+E−α)∈gu
\mbox{$\bar{\theta}_{*}(E_{\alpha})=-E_{-\alpha}$ for all $\alpha\in\triangle$}.
\mbox{$\bar{\theta}_{*}(E_{\alpha})=-E_{-\alpha}$ for all $\alpha\in\triangle$}.
\left\{\begin{array}[]{@{}l}\mathscr{W}:=N_{G_{u}}(i\mathfrak{h}_{\mathbb{R}})/C_{G_{u}}(i\mathfrak{h}_{\mathbb{R}}),\\
\mbox{$\zeta([w])\eta:={}^{t}\!\mathrm{Ad}w^{-1}(\eta)$ for $[w]\in\mathscr{W}$ and $\eta\in(\mathfrak{h}_{\mathbb{C}})^{*}$},\end{array}\right.
\left\{\begin{array}[]{@{}l}\mathscr{W}:=N_{G_{u}}(i\mathfrak{h}_{\mathbb{R}})/C_{G_{u}}(i\mathfrak{h}_{\mathbb{R}}),\\
\mbox{$\zeta([w])\eta:={}^{t}\!\mathrm{Ad}w^{-1}(\eta)$ for $[w]\in\mathscr{W}$ and $\eta\in(\mathfrak{h}_{\mathbb{C}})^{*}$},\end{array}\right.
\mbox{$w_{\alpha}:=\exp(\pi/2)(E_{\alpha}-E_{-\alpha})$ for $\alpha\in\triangle$}.
\mbox{$w_{\alpha}:=\exp(\pi/2)(E_{\alpha}-E_{-\alpha})$ for $\alpha\in\triangle$}.
\mbox{$\mathcal{O}:=U^{+}Q^{-}\cup\bigl{(}\bigcup_{\mbox{\scriptsize{$\beta\in\Pi_{\triangle}$ with $\beta(T)\neq 0$}}}w_{\beta}^{-1}U^{+}Q^{-}\bigr{)}$}.
\mbox{$\mathcal{O}:=U^{+}Q^{-}\cup\bigl{(}\bigcup_{\mbox{\scriptsize{$\beta\in\Pi_{\triangle}$ with $\beta(T)\neq 0$}}}w_{\beta}^{-1}U^{+}Q^{-}\bigr{)}$}.
\displaystyle\!\mathcal{V}_{G_{\mathbb{C}}/Q^{-}}\!\!:=\!\!\left\{\begin{array}[]{@{}l@{\,\,}|l@{}}h:G_{\mathbb{C}}\to{\sf V}&\begin{array}[]{@{\!}l@{\!}}\mbox{(1) $h$ is holomorphic},\\
\mbox{(2) $h(xq)=\rho(q)^{-1}(h(x))$ for all $(x,q)\in G_{\mathbb{C}}\!\times\!Q^{-}$}\end{array}\end{array}\right\}\!,\!\!\!\!
\displaystyle\!\mathcal{V}_{G_{\mathbb{C}}/Q^{-}}\!\!:=\!\!\left\{\begin{array}[]{@{}l@{\,\,}|l@{}}h:G_{\mathbb{C}}\to{\sf V}&\begin{array}[]{@{\!}l@{\!}}\mbox{(1) $h$ is holomorphic},\\
\mbox{(2) $h(xq)=\rho(q)^{-1}(h(x))$ for all $(x,q)\in G_{\mathbb{C}}\!\times\!Q^{-}$}\end{array}\end{array}\right\}\!,\!\!\!\!
\displaystyle\!\mathcal{V}_{G/L}\!\!:=\!\!\left\{\begin{array}[]{@{}l@{\,\,}|l@{}}\psi:GQ^{-}\to{\sf V}&\begin{array}[]{@{\!}l@{\!}}\mbox{(1) $\psi$ is holomorphic},\\
\mbox{(2) $\psi(yq)=\rho(q)^{-1}(\psi(y))$ for all $(y,q)\in GQ^{-}\!\times\!Q^{-}$}\end{array}\end{array}\right\}\!\!\!\!\!\!
\mbox{$\displaystyle{d(\psi_{1},\psi_{2}):=\sum_{n=1}^{\infty}\dfrac{1}{2^{n}}\dfrac{d_{n}(\psi_{1},\psi_{2})}{1+d_{n}(\psi_{1},\psi_{2})}}$ for $\psi_{1},\psi_{2}\in\mathcal{V}_{G/L}$}.
\mbox{$\displaystyle{d(\psi_{1},\psi_{2}):=\sum_{n=1}^{\infty}\dfrac{1}{2^{n}}\dfrac{d_{n}(\psi_{1},\psi_{2})}{1+d_{n}(\psi_{1},\psi_{2})}}$ for $\psi_{1},\psi_{2}\in\mathcal{V}_{G/L}$}.
\mbox{$\bigl{(}\varrho(g)\psi\bigr{)}(y):=\psi(g^{-1}y)$ for $\psi\in\mathcal{V}_{G/L}$, $y\in GQ^{-}$}.
\mbox{$\bigl{(}\varrho(g)\psi\bigr{)}(y):=\psi(g^{-1}y)$ for $\psi\in\mathcal{V}_{G/L}$, $y\in GQ^{-}$}.
\mbox{all the eigenvalues of $\mathrm{ad}iT$ are integer}.
\mbox{all the eigenvalues of $\mathrm{ad}iT$ are integer}.
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TopicsAdvanced Algebra and Geometry · Geometry and complex manifolds · Algebraic Geometry and Number Theory
Full text
A topic on homogeneous vector bundles over elliptic orbits: A condition for the vector spaces of their cross-sections to be finite dimensional
Nobutaka Boumuki
Division of Mathematical Sciences, Faculty of Science and TechnologyOita University, 700 Dannoharu, Oita-shi, Oita 870-1192, JAPAN
In this paper we consider the complex vector spaces of holomorphic cross-sections of homogeneous holomorphic vector bundles over elliptic adjoint orbits, and provide a sufficient condition for the vector spaces to be finite dimensional in view of root systems.
This work was supported by JSPS KAKENHI Grant Number JP 17K05229.
1. Introduction
For a connected real semisimple Lie group G, the adjoint orbit AdG(T)=G/CG(T) of G through an elliptic element T∈g is called an elliptic (adjoint) orbit.
Here an element T∈g is said to be elliptic, if adT is a semisimple linear transformation of g and all the eigenvalues of adT are purely imaginary.
It is known that elliptic orbits can be geometrically characterized as follows (cf. Dorfmeister-Guan [4, 5]):
Any elliptic orbit G/CG(T) is a homogeneous pseudo-Kähler manifold of G.
Conversely, a homogeneous pseudo-Kähler manifold M of G is an elliptic orbit whenever G acts on M almost effectively.
Accordingly there is no essential difference between elliptic orbits and homogeneous pseudo-Kähler manifolds of real semisimple Lie groups.
Let us give examples of elliptic orbits.
A complex projective space CPn is one of the Hermitian symmetric spaces of compact type, any Hermitian symmetric space Gu/K of compact type is one of the complex flag manifolds (which are also called generalized flag manifolds or Kähler C-spaces), and all complex flag manifolds GC/Q are elliptic orbits.
These are examples of elliptic orbits which are compact.
As a non-compact example, one knows that all symmetric bounded domains D in Cn are elliptic orbits.
In this paper, we deal with such spaces.
Now, let us explain our research background.
Let GC be a connected complex semisimple Lie group, let G be a connected closed subgroup of GC such that g is a real form of gC, and let T be a non-zero elliptic element of g.
Setting
[TABLE]
one has an elliptic orbit G/L, a complex flag manifold GC/Q− and L=G∩Q−; besides, it turns out that ι:G/L→GC/Q−, gL↦gQ−, is a G-equivariant real analytic embedding whose image is a simply connected domain in GC/Q−, and that GQ− is a domain in GC.
Henceforth, we assume G/L to be a domain in GC/Q− and it to be a homogeneous complex manifold of G via this ι.
In addition, let V be a finite dimensional complex vector space and let ρ:Q−→GL(V), q↦ρ(q), be a holomorphic homomorphism.
Denote by GC×ρV the fiber bundle over the complex flag manifold GC/Q−, with standard fiber V and structure group Q−, which is associated to the principal fiber bundle πC:GC→GC/Q−, x↦xQ−, and denote by ι♯(GC×ρV) the restriction of the bundle GC×ρV to the domain G/L⊂GC/Q−.
Then one may assume that
[TABLE]
are the complex vector spaces of holomorphic cross-sections of the bundles GC×ρV and ι♯(GC×ρV), respectively.
Here, we remark that the vector space VGC/Q− is always finite dimensional,
[TABLE]
because GC/Q− is a connected compact complex manifold; but, in contrast, VG/L is not necessarily finite dimensional—for example, dimCVG/L=∞ in the case where G/L is a symmetric bounded domain in Cn and VG/L is the vector space O(T1,0(G/L)) of holomorphic vector fields on it.
This poses us the following problem:
“What is a condition for dimCVG/L<∞ ?”
In this paper we partially solve this problem.
The main purpose of this paper is to provide a sufficient condition so that all the holomorphic mappings ψ∈VG/L can be continued analytically from GQ− to GC.
In view of a root system △ of gC, we assert the following statement (see Subsection 3.1, Theorem 3.1):
Suppose that (S) there exists a fundamental root system Π△ of △ satisfying
(s1)* α(−iT)≥0 for all α∈Π△, and*
(s2)* gβ⊂kC for every β∈Π△ with β(T)=0.*
Then, all the holomorphic mappings ψ∈VG/L extend uniquely to holomorphic ones ψ^∈VGC/Q− and dimCVG/L=dimCVGC/Q−<∞.
Pay attention to that in the case where the above supposition (S) holds, the vector space VG/L is finite dimensional for any complex vector space V of dimCV<∞ and any holomorphic homomorphism ρ:Q−→GL(V).
Hence, in particular, one can deduce that in this case, the group Hol(G/L) of holomorphic automorphisms of G/L is a (finite dimensional) Lie group.
This paper consists of four sections.
In Section 2 we mainly review known facts about elliptic orbits, generalized Bruhat decompositions and homogeneous holomorphic vector bundles.
In Section 3 we state the main result in this paper (Theorem 3.1) and demonstrate it by taking a continuous representation ϱ of G on VG/L, a generalized Bruhat decomposition of GC and the second Riemann removable singularity theorem into account.
Finally in Section 4, we give some examples which satisfy the supposition (S) in Theorem 3.1, and give an example which does not so.
We will see that the (S) cannot hold for any symmetric bounded domain D in Cn, cf. Example 4.2.
2. Preliminaries
In this section we first fix the notation utilized in this paper, and afterwards review known facts about elliptic orbits, generalized Bruhat decompositions and homogeneous holomorphic vector bundles.
We will give two Lemmas 2.6 and 2.14, Corollary 2.20 and Proposition 2.33 especially needed in Section 3.
2.1. Notation
Throughout this paper, for a Lie group G, we denote its Lie algebra by the corresponding Fraktur small letter g, and utilize the following notation:
(n1)
i:=−1,
(n2)
Ad, ad : the adjoint representation of G, g,
(n3)
CG(T):={g∈G∣Adg(T)=T} for an element T∈g,
(n4)
NG(m):={g∈G∣Adg(m)⊂m} for a vector subspace m⊂g,
(n5)
m⊕n : the direct sum of vector spaces m and n,
(n6)
GL(V) : the general linear group on a complex vector space V.
Besides, we sometimes denote by f∣A the restriction of a mapping f to a set A.
2.2. Elliptic orbits
Kobayashi [7] has introduced the notion of elliptic orbit, which is as follows:
Let g be a real semisimple Lie algebra and G a connected Lie group with Lie algebra g.
An element T∈g is said to be elliptic, if adT is a semisimple linear transformation of g and all the eigenvalues of adT are purely imaginary.
The adjoint orbit AdG(T)=G/CG(T) of G through an elliptic element T∈g is called an elliptic (adjoint) orbit.
Now, let GC be a connected complex semisimple Lie group, let G be a connected closed subgroup of GC such that g is a real form of gC, and let T be a non-zero elliptic element of g.
Then we set
[TABLE]
where gλ={0} in the case where λ is different from the eigenvalues of adT, we denote by exp:gC→GC the exponential mapping, and uT± will stand for the above u± for once in Lemma 2.6.
Since T∈g is elliptic, there exists a Cartan decomposition g=k⊕p of g such that
[TABLE]
where k is a maximal compact subalgebra of g.
Noting that the center Z(G) of G is finite due to Z(G)⊂Z(GC) and that gu:=k⊕ip is a compact real form of gC, we denote by K and Gu the maximal compact subgroups of G and GC corresponding to the subalgebras k⊂g and gu⊂gC, respectively.
In addition, we denote by the (anti-holomorphic) Cartan involution θˉ of GC such that
Since GC is connected semisimple and T∈g is an elliptic element of gC also, one shows that LC=CGC(T) is connected.
The rest of proof is trivial.
∎
Let GC be a connected complex semisimple Lie group, let G be a connected closed subgroup of GC such that g is a real form of gC, and let T be a non-zero elliptic element of g.
Fix a Cartan decomposition g=k⊕p with T∈k, and take a maximal torus ihR of gu=k⊕ip containing T.
Then, there exists an elliptic element T′∈g such that
Us* is a simply connected, closed complex nilpotent subgroup of GC whose Lie algebra coincides with us, and exp:us→Us is biholomorphic, for each s=±.*
2. (2)
Qs* is a connected, closed complex parabolic subgroup of GC such that
Qs=LC⋉Us(semidirect) and qs=(lC⊕us)=⨁μ≥0gsμ, for each s=±.*
3. (3)
U+×Q−∋(u,q)↦uq∈GC* is a holomorphic embedding whose image is a dense, domain in GC.*
4. (4)
L* is a connected closed subgroup of G, and the homogeneous space G/L is simply connected.*
5. (5)
L=G∩Q−.
6. (6)
ι:G/L→GC/Q−, gL↦gQ−, is a G-equivariant real analytic embedding whose image is a simply connected domain in GC/Q−.
7. (7)
In general, there are several kinds of invariant complex structures on the elliptic orbit G/L.
In this paper we deal with the complex structure on G/L induced by ι:G/L→GC/Q−, gL↦gQ−.
Here, the imaginary unit i∈C gives rise to a GC-invariant complex structure J on the complex flag manifold GC/Q− in a natural way.
In the setting (2.2); the following two items hold for given finite elements x1,x2,…,xj∈GC:
(1)
The intersection GQ−∩x1U+Q−∩⋯∩xjU+Q− is a non-empty open subset of GC.
2. (2)
The union GQ−∪x1U+Q−∪⋯∪xjU+Q− is a dense, domain in GC.
2.3. Root systems and generalized Bruhat decompositions
We review fundamental results about root systems and modify a generalized Bruhat decomposition of GC for our situation (see Proposition 2.18-(3)).
The setting (2.2), (2.3) and (2.4) remains valid in this subsection.
2.3.1. Root systems and Weyl groups
Let ihR be a maximal torus of gu=k⊕ip containing the element T, let △=△(gC,hC) be the (non-zero) root system of gC relative to hC, where hC is the complex vector subspace of gC generated by ihR, and let gα be the root subspace of gC for α∈△.
For each root α∈△, there exists a unique Hα∈hC such that α(H)=BgC(Hα,H) for all H∈hC, where BgC is the Killing form of gC.
Then hR=spanR{Hα∣α∈△}, and for every α∈△ there exists a vector Eα∈gα satisfying
[TABLE]
(cf. Helgason [6, Lemma 3.1, p.257–258]).
Here, it is immediate from (2.4) that gu=ihR⊕⨁α∈△spanR{Eα−E−α}⊕spanR{i(Eα+E−α)}, and
[TABLE]
Define a Weyl group W of GC and an action ζ of W on the dual space (hC)∗ by
[TABLE]
where [w] stands for the left coset wCGu(ihR).
By use of Eα in (2.10) we set
[TABLE]
Needless to say, wα belongs to NGu(ihR) and so [wα]∈W for every root α∈△; besides, ζ([wα]) is the reflection along α which leaves △ invariant.
We need
Lemma 2.14**.**
Let kC be the complex subalgebra of gC generated by k.
For a root β∈△=△(gC,hC) with β(T)=0, the following (a), (b) and (c) are equivalent:
[TABLE]
Therefore, wβ=exp(π/2)(Eβ−E−β) belongs to K∩NGu(ihR) whenever one of the (a), (b) and (c) holds.
Proof..
Since (a) ⇔ (b) is obvious, we only confirm (b) ⇔ (c).
(b) ⇒ (c): This follows by (2.11), θˉ∗(kC)⊂kC and k={Y∈kC∣θˉ∗(Y)=Y}.
(c) ⇒ (b):
Suppose that (Eβ−E−β)∈k.
Then, from (2.3) one obtains
[TABLE]
and so 0=β(T)∈iR yields (Eβ+E−β)∈ik.
Hence Eβ=(1/2)(Eβ−E−β+Eβ+E−β)∈k+ik⊂kC.
∎
2.3.2. Generalized Bruhat decompositions
We continue to obey the setting of Paragraph 2.3.1.
Our first aim in this paragraph is to state Proposition 2.17 which is a result of Kostant [9, 10] and the second one is to modify a generalized Bruhat decomposition of GC for our situation.
For the aim, we are going to fix two Iwasawa decompositions of GC first.
Let Π△ be a fundamental root system111There is such a system with (s1)—for example, consider the lexicographic linear ordering on the dual space (hR)∗ associated with a real base −iT=:A1,A2,…,Aℓ of hR. of △=△(gC,hC) satisfying
[TABLE]
Relative to this Π△ we fix the set △+ of positive roots, and put △−:=−△+.
Then (s1) yields β(−iT)≥0 for all β∈△+.
Setting ns:=⨁β∈△sgβ and bs:=hC⊕ns (s=±) one has Iwasawa decompositions gC=gu⊕hR⊕n± of gC; moreover, it follows from (2.2) and gC=n+⊕hC⊕n− that
[TABLE]
Denote by GC=GuHRN± the Iwasawa decompositions of GC corresponding to the gC=gu⊕hR⊕n±, respectively.
where Lu:=CGu(T).
Note that u±=⨁α∈△(u±)gα due to (2.15), that Φ[w] is a closed subsystem of △ for any [w]∈W, and that W1 is a Weyl group of LC.
Hereafter, let us assume that W1 is a subgroup of W via NLu(ihR)/CLu(ihR)∋τCLu(ihR)↦τCGu(ihR)∈NGu(ihR)/CGu(ihR).
Now, we are in a position to state the proposition:
For any [w]∈W, it follows that △+=Φ[w]∪Φ[wκ](disjoint union), where [κ] is the unique element of W such that ζ([κ])△−=△+.
2. (2)
If [σ]∈W1, then \zeta([\sigma])^{-1}\bigl{(}\triangle^{+}(\mathfrak{l}_{\mathbb{C}})\bigr{)}\subset\triangle^{+} and \zeta([\sigma])^{-1}\bigl{(}\triangle^{-}(\mathfrak{l}_{\mathbb{C}})\bigr{)}\subset\triangle^{-}.
3. (3)
For each [w]∈W there exists a unique ([τ],[σ])∈W1×W1 such that [w]=[τσ].
4. (4)
For a [σ]∈W1, the following items (4.i) and (4.ii) hold:**
(4.i)
n[σ]=0* if and only if [e]=[σ].*
2. (4.ii)
n[σ]=1* if and only if there exists a β∈Π△ satisfying β(T)=0 and [wβ]=[σ].*
Here n[σ] is the cardinal number of the set Φ[σ], and e is the unit element of GC.
With the same notation and setting as in Proposition 2.17;* let r:=dimCu+.*
(1)
For each [σ]∈W1 we set
[TABLE]
Then, Uσ+ is a simply connected closed complex nilpotent subgroup of U+ and it is biholomorphic to the (r−n[σ])-dimensional complex Euclidean space*;** furthermore, N+σ−1Q−=σ−1Uσ+Q−.*
2. (2)
For a [σ]∈W1, the following items (2.i) and (2.ii) hold:**
(2.i)
dimCUσ+=r=dimCU+* if and only if [e]=[σ].*
2. (2.ii)
dimCUσ+=r−1* if and only if there exists a β∈Π△ satisfying β(T)=0 and [wβ]=[σ].*
3. (3)
(1) We only prove that dimCUσ+=r−n[σ] and N+σ−1Q−=σ−1Uσ+Q− for any [σ]∈W1.
In view of (2.16), ζ([κ])△−=△+ and △(u+)⊂△+ we see
[TABLE]
This implies that △σ consists of (r−n[σ])-elements, so that dimCUσ+=r−n[σ].
The Proposition 2.17-(1) above and Lemma 6.2 in Kostant [10, p.124] yield
[TABLE]
where we remark that ⨁β∈Φ[σ−1]gζ([σ])β⊂n−⊂q−, and that either ζ([σ])γ∈△+(lC) or ζ([σ])γ∈△(u+) holds for every γ∈Φ[σ−1κ]; besides, the above computation is independent of the choice of representative σ∈[σ].
(3) The arguments below will be similar to those in the proof of Lemma 5.6 in Takeuchi [12, p.21] or Proposition 6.1 in Kostant [10, p.123].
By virtue of (1), it suffices to confirm that GC=⋃[σ]∈W1N+σ−1Q− (disjoint union).
Setting B+:=NGC(b+) we fix the Bruhat decomposition GC=⋃[w]∈WN+w−1B+ (disjoint union).
Then, it follows from ζ([κ])△−=△+ that GC=κ−1GC=⋃[w]∈WN−(wκ)−1B+=⋃[w]∈WN−w−1B+, namely
[TABLE]
In a similar way we have
[TABLE]
where n1±:=⨁α∈△±(lC)gα, N1−:=expn1− and B1+:=NLC(hC⊕n1+).
This, together with Q+=LCU+ and B+=B1+U+, assures that for any [σ]∈W1,
[TABLE]
where σ−1N1−⊂N−σ−1 follows from [σ]∈W1 and Proposition 2.17-(2).
Consequently, (2.19) and Proposition 2.17-(3) allow us to assert that
[TABLE]
Thus GC=⋃[σ]∈W1N+σ−1Q− (disjoint union) because of θˉ(GC)=GC, θˉ(N−)=N+, θˉ(σ)=σ and θˉ(Q+)=Q−.
∎
The following corollary will play a role later (recall (2.13) for wβ):
Corollary 2.20**.**
Let GC be a connected complex semisimple Lie group, let G be a connected closed subgroup of GC such that g is a real form of gC, and let T be a non-zero elliptic element of g.
Set U+, Q− as (2.2), fix a Cartan decomposition g=k⊕p with T∈k, and take a maximal torus ihR of gu=k⊕ip containing T.
Consider the root system △=△(gC,hC) and a fundamental root system Π△ of △ such that (s1)α(−iT)≥0 for all α∈Π△.
Now, let
[TABLE]
Then, O is a dense domain in GC.
Furthermore, any holomorphic function f on O can be continued analytically to the whole GC.
Proof..
Proposition 2.7-(3) implies that O is a dense domain in GC.
Proposition 2.18 tells us that e^{-1}U^{+}_{e}Q^{-}\cup\bigl{(}\bigcup_{\mbox{\scriptsize{\beta\in\Pi_{\triangle}with\beta(T)\neq 0}}}w_{\beta}^{-1}U^{+}_{w_{\beta}}Q^{-}\bigr{)} is a subset of O, and moreover, GC−O must be of complex codimension 2 or more.
Therefore any holomorphic function f on O can be continued analytically to the whole GC, by the second Riemann removable singularity theorem (which is sometimes called Hartogs’s continuation theorem).
Here dimCGC≥3, since GC is complex semisimple.
∎
2.4. Homogeneous holomorphic vector bundles
In this subsection we recall elementary facts about homogeneous holomorphic vector bundles.
Let GC be a connected complex semisimple Lie group, let G be a connected closed subgroup of GC such that g is a real form of gC, and let T be a non-zero elliptic element of g.
Define the closed subgroups L⊂G and Q−⊂GC by (2.2).
Then, we assume that the elliptic orbit G/L is a domain in the complex flag manifold GC/Q− and is a homogeneous complex manifold of G via ι:G/L→GC/Q−, gL↦gQ−.
Now, for a complex vector space V of dimCV<∞ and a holomorphic homomorphism ρ:Q−→GL(V), q↦ρ(q), we denote by GC×ρV the fiber bundle over GC/Q−, with standard fiber V and structure group Q−, which is associated to the principal fiber bundle πC:GC→GC/Q−, x↦xQ−, and denote by ι♯(GC×ρV) the restriction of the bundle GC×ρV to the domain G/L⊂GC/Q−.
In this setting, one may assume that
[TABLE]
are the complex vector spaces of holomorphic cross-sections of the bundles GC×ρV and ι♯(GC×ρV), respectively.
Remark 2.29**.**
One knows that dimCVGC/Q−<∞ because GC/Q− is a connected compact complex manifold.
e.g. Kodaira [8, p.161].
From now on, we are going to set a topology for the VG/L.
Since GC is connected, it satisfies the second countability axiom.
Hence GQ− satisfies the same axiom also and is a locally compact Hausdorff space, since GQ− is open in GC.
Consequently there exist non-empty open subsets On⊂GQ− such that (i) GQ−=⋃n=1∞On (countable union) and (ii) the closure On in GQ− is compact for each n∈N.
Taking a norm ∥⋅∥ on the vector space V, we define dn by dn(ψ1,ψ2):=sup{∥ψ1(a)−ψ2(a)∥:a∈On} for n∈N, ψ1,ψ2∈VG/L; and furthermore we define
[TABLE]
This d is called the Fréchet metric on VG/L.
Then, one can show the lemma below (e.g. refer to [2, Paragraph 2.4.4]), where ϱ:G→GL(VG/L), g↦ϱ(g), is a homomorphism defined by
[TABLE]
Lemma 2.32**.**
In the setting (2.28), (2.30) and (2.31); the following four items hold for the Fréchet metric d on VG/L:
(1)
(VG/L,d)* is a complete metric space.*
2. (2)
The metric topology for (VG/L,d) coincides with the topology of uniform convergence on compact sets*;** and besides it also coincides with the locally convex topology determined by a countable number of seminorms {pn}n∈N, where pn(ψ):=dn(ψ,0) for n∈N, ψ∈VG/L.*
3. (3)
Both VG/L×VG/L∋(ψ1,ψ2)↦ψ1+ψ2∈VG/L and C×VG/L∋(α,ψ)↦αψ∈VG/L are continuous mappings.
4. (4)
G×VG/L∋(g,ψ)↦ϱ(g)ψ∈VG/L* is a continuous mapping.*
Lemma 2.32 implies that VG/L=(VG/L,d) is a Fréchet space and that ϱ is a continuous representation of the Lie group G on VG/L.
Therefore
Proposition 2.33** (e.g. van den Ban [13, p.24]).**
In the setting (2.28), (2.30) and (2.31); for a compact subgroup K′ of G we set
[TABLE]
Then, (VG/L)K′ is dense in VG/L with respect to the metric topology for (VG/L,d).
We end this section with the following remark: the set (VG/L)K′ in Proposition 2.33 accords with the set of K′-finite vectors in VG/L for the continuous representation ϱ of G on VG/L.
This section consists of two subsections.
In Subsection 3.1 we state Theorem 3.1 which is the main result in this paper; and in Subsection 3.2 we demonstrate the theorem.
G is a connected closed subgroup of GC such that g is a real form of gC,
•
T is a non-zero elliptic element of g,
•
g=k⊕p is a Cartan decomposition of g with T∈k,
•
ihR is a maximal torus of gu=k⊕ip containing T,
•
△=△(gC,hC) is the root system of gC relative to hC, where hC is the complex vector subspace of gC generated by ihR,
•
gα is the root subspace of gC for α∈△,
•
L=CG(T),
•
Q− is the closed complex subgroup of GC defined by (2.2),
•
kC is the complex subalgebra of gC generated by k,
•
V is a finite dimensional complex vector space,
•
ρ:Q−→GL(V), q↦ρ(q), is a holomorphic homomorphism,
•
VGC/Q− and VG/L are the complex vector spaces defined by (2.24) and (2.28), respectively.
Now, we are in a position to state
Theorem 3.1**.**
In the setting of Subsection \refsubsec−3.1; suppose that (S) there exists a fundamental root system Π△ of △ satisfying
(s1)*
α(−iT)≥0 for all α∈Π△, and*
(s2)*
gβ⊂kC for every β∈Π△ with β(T)=0.*
Then, the complex vector space VGC/Q− is linear isomorphic to VG/L via F:VGC/Q−→VG/L, h↦h∣GQ−, and therefore dimCVG/L=dimCVGC/Q−<∞.
Here h∣GQ− stands for the restriction of h to GQ−⊂GC.
3.2. Proof of Theorem 3.1
The setting of Theorem 3.1 remains valid in this subsection.
In addition, we take the closed complex subgroup U+ defined by (2.2) and the maximal compact subgroup K⊂G corresponding to the subalgebra k⊂g into consideration.
Our goal in Subsection 3.2 is to complete the proof of Theorem 3.1.
We are going to show two Lemmas 3.5 and 3.6, Proposition 3.7 and Corollary 3.10, and obtain the goal from them.
Remark 3.2**.**
For the element T concerning Theorem 3.1, one may assume that
[TABLE]
Let us explain the reason why.
Let T′ be the element in Lemma 2.6.
Then for any root α∈△, one can assert that α(iT)>0, α(iT)=0 and α(iT)<0 if and only if α(iT′)>0, α(iT′)=0 and α(iT′)<0, respectively.
In particular, for any β∈Π△, β(T)=0 if and only if β(T′)=0.
Accordingly there are no changes in the topological group structures on L and Q−, and no change in the supposition (S) even if one substitutes T′ for T.
For this reason, we assume (3.3) hereafter.
Suppose that △(u+) consists of r-elements γ1,γ2,…,γr∈△, where r=dimCu+.
Then, {Eγj}j=1r is a complex base of u+=⨁α∈△(u+)gα=⨁j=1rgγj, and by virtue of (3.3) there exist n1,n2,…,nr∈N satisfying γj(T)=inj for each 1≤j≤r, so that
[TABLE]
for all λ∈R.
cf. (2.10) for Eγj, (2.16) for △(u+).
Lemma 3.5**.**
The mapping F:VGC/Q−→VG/L, h↦h∣GQ−, is injective linear.
Proof..
It is enough to confirm that F is injective.
That comes from the theorem of identity, since h:GC→V is holomorphic, GC is connected and GQ− is open in GC.
∎
Lemma 3.6**.**
(1)
Let φ be a K-finite vector in VG/L for the representation ϱ defined by (2.31), and let Vφ be the complex vector subspace of VG/L generated by {ϱ(k)φ:k∈K}.
Then, there exist a complex base {φa}a=1mφ of Vφ and μ1,μ2,…,μmφ∈R such that
[TABLE]
for all 1≤a≤mφ=dimCVφ and λ∈R.
3. (2)
There exist a complex base {vb}b=1k of V and θ1,θ2,…,θk∈R such that
[TABLE]
for all 1≤b≤k=dimCV and λ∈R.
Proof..
(1) Let S1:={expλT∣λ∈R}.
Then, it follows from T∈k that S1 is a real one-dimensional torus and S1⊂K.
Therefore, since Vφ is ϱ(K)-invariant and mφ=dimCVφ<∞, there exist ϱ(S1)-invariant complex vector subspaces V1,V2,…,Vmφ⊂Vφ and μ1,μ2,…,μmφ∈R such that Vφ=V1⊕V2⊕⋯⊕Vmφ, dimCVa=1 and
[TABLE]
for all 1≤a≤mφ and λ∈R.
Hence we can get the conclusion by taking a non-zero element of Va for each 1≤a≤mφ.
(2) One can conclude (2) by arguments similar to those above.
Indeed; there exist ρ(S1)-invariant complex vector subspaces V1,…,Vk⊂V and θ1,…,θk∈R such that V=V1⊕⋯⊕Vk, dimCVb=1 and ρ(expλT)=eiθbλid on Vb for all 1≤b≤k and λ∈R, because of S1⊂Q− and k=dimCV<∞.
∎
Proposition 3.7**.**
Let {φa}a=1mφ and {vb}b=1k be the complex bases of Vφ and V in Lemma 3.6, respectively.
For y∈GQ− we express φa(y)∈V as
[TABLE]
Then, for each 1≤b≤k there exists a unique polynomial (holomorphic) function φab′ on Cr≅U+ of finite degree such that
[TABLE]
Therefore, for a given ϕ∈Vφ there exists a unique holomorphic mapping ϕ′:U+→V such that ϕ=ϕ′∣U+∩GQ−.
Proof..
Denote by z1,z2,…,zr the canonical coordinates of the first kind associated with the complex base {Eγj}j=1r of u+ (see Remark 3.2 for Eγj).
Here, it turns out that U+≅Cr via
[TABLE]
Noting that U+∩GQ− is an open subset of U+ containing the unit e∈GC and that the restriction φab∣U+∩GQ− is a holomorphic function on U+∩GQ−, we obtain an R>0 so that the following (i) and (ii) hold for O:=\{u\in U^{+}:\mbox{|z^{j}(u)|<R,1\leq j\leq r}\}:
(i)
O is an open subset of U+∩GQ− containing e, and
2. (ii)
on O we can express φab∣U+∩GQ− as
[TABLE]
(the Taylor expansion of φab∣U+∩GQ− at e=(0,0,…,0)).
Remark that O is stable under every inner automorphism of S1={expλT∣λ∈R}, cf. (3.4).
For any λ∈R and u∈O we have
[TABLE]
and hence e^{i\theta_{b}\lambda}\varphi_{a}^{b}(u)=e^{i\mu_{a}\lambda}\varphi_{a}^{b}\bigl{(}(\exp\lambda T)u\exp(-\lambda T)\bigr{)}.
This, together with (ii) and (3.4), yields
[TABLE]
in case of u=exp(z1Eγ1+z2Eγ2+⋯+zrEγr).
Therefore one shows that
[TABLE]
Differentiating this equation at λ=0, we deduce that
[TABLE]
for all 1≤b≤k and m1,m2,…,mr≥0.
It follows from n1,n2,…,nr∈N and (3.8) that for each b, all the coefficients αm1m2⋯mrb vanish whenever θb−μa∈N∪{0}; and that with respect to m1,m2,…,mr with θb−μa=n1m1+n2m2+⋯+nrmr, the coefficient αm1m2⋯mrb vanishes even if θb−μa∈N∪{0}.
These imply that
[TABLE]
must be a polynomial function on O of finite degree.
Consequently, for each 1≤b≤k, φab(z1,…,zr) can extend uniquely to a polynomial function φab′(z1,…,zr) on Cr≅U+ of finite degree.
∎
Remark 3.9**.**
In Proposition 3.7 we have concluded that for any ϕ∈Vφ, the restriction ϕ∣U+∩GQ− can be continued analytically to U+, without the supposition (s2) in Theorem 3.1.
Let φ be any K-finite vector in VG/L for the representation ϱ defined by (2.31), and let Vφ be the complex vector subspace of VG/L generated by {ϱ(k)φ:k∈K}.
Suppose that (S) there exists a fundamental root system Π△ of △ satisfying
(s1)*
α(−iT)≥0 for all α∈Π△, and*
(s2)*
gβ⊂kC for every β∈Π△ with β(T)=0.*
Then, it follows that φ∈Vφ⊂F(VGC/Q−).
Proof..
Take any ϕ∈Vφ.
By Proposition 3.7 there exists a unique holomorphic mapping ϕ′:U+→V such that ϕ=ϕ′∣U+∩GQ−.
Proposition 2.7-(3) enables us to construct the holomorphic extension ϕ′′:U+Q−→V of ϕ′ from
[TABLE]
Here, it follows from (U+Q−∩GQ−)=(U+∩GQ−)Q−, ϕ=ϕ′∣U+∩GQ−, ϕ∈VG/L and (2.28)-(2) that
[TABLE]
Now, Lemma 2.14 and (s2) assure that wβ∈K for every β∈Π△ with β(T)=0.
This enables us to obtain
[TABLE]
since Vφ is ϱ(K)-invariant.
Accordingly for each β∈Π△ with β(T)=0, there exists a unique holomorphic mapping (ϱ(wβ)ϕ)′′:U+Q−→V such that
[TABLE]
Then, we define a holomorphic mapping ϕ^ from
[TABLE]
into V as follows:
[TABLE]
Here O is a dense, domain in GC (cf. Corollary 2.20).
Let us confirm that the definition (3.11) is well-defined.
Corollary 2.9-(1) implies that the intersection
[TABLE]
is a non-empty open subset of GC.
For any element y of the intersection above and any β∈Π△ with β(T)=0 we have wβy∈U+Q− and wβy∈KGQ−⊂GQ−; and thus
[TABLE]
in terms of wβy,y∈U+Q−∩GQ−.
For this reason (3.11) is well-defined by the theorem of identity and it follows that ϕ=ϕ^ on O∩GQ−.
From Corollary 2.20, there exists the analytic continuation ϕ^′:GC→V of ϕ^:O→V.
This ϕ^′ satisfies ϕ^′(xq)=ρ(q)−1(ϕ^′(x)) for all (x,q)∈GC×Q−, by the theorem of identity, ϕ=ϕ^′∣GQ−, (2.28)-(2) and ϕ∈VG/L.
Consequently it is immediate from (2.24) that ϕ^′∈VGC/Q−, so that ϕ=ϕ^′∣GQ−=F(ϕ^′)∈F(VGC/Q−).
This provides us with Vφ⊂F(VGC/Q−).
∎
By Lemma 3.5 and Remark 2.29 it suffices to conclude
[TABLE]
Let (VG/L)K be the set of K-finite vectors in VG/L for the representation ϱ defined by (2.31).
From Corollary 3.10 we obtain
[TABLE]
Now, let ψ be an arbitrary element of VG/L.
On the one hand; Proposition 2.33 assures that there exists a sequence {φn}n=1∞⊂(VG/L)K satisfying
[TABLE]
On the other hand; since VG/L=(VG/L,d) is a Hausdorff topological vector space and dimCF(VGC/Q−)=dimCVGC/Q−<∞, it turns out that F(VGC/Q−) is closed in VG/L.
Thus, it follows from (3.13) that ψ=limn→∞φn∈F(VGC/Q−), so that (3.12) holds.
∎
4. Examples
Let us give some examples which satisfy the supposition (S) in Theorem 3.1 and an example which does not so.
Recall that the supposition is as follows:
(S) there exists a fundamental root system Π△ of △ satisfying
(s1) α(−iT)≥0 for all α∈Π△, and
(s2) gβ⊂kC for every β∈Π△ with β(T)=0.
Example 4.1** (G/L=SU(p,q)/S(U(h)×U(p−h,q)), p+q≥2, 0<h<p).**
Let GC:=SL(p+q,C), G:=SU(p,q), gu:=su(p+q) and
[TABLE]
where p+q≥2.
Denote by △=△(gC,hC) the root system of gC relative hC, define simple roots αk∈△ (1≤k≤p+q−1) as
[TABLE]
and set Π△:={αk}k=1p+q−1.
Here, the dual base {Zk}k=1p+q−1 of Π△={αk}k=1p+q−1 is
[TABLE]
where In is the unit matrix of degree n.
Let Th:=iZh, 0<h<p, and
[TABLE]
In the setting above, it follows that Th is an elliptic element of g, ihR is a maximal torus of gu containing Th, g=k⊕p, gu=k⊕ip and (s1) α(−iTh)≥0 for all α∈Π△.
Moreover,
(1)
for β∈Π△={αk}k=1p+q−1, β(Th)=0 if and only if β=αh,
2. (2)
gαh=spanC{Eh,h+1},
where gαh is the root subspace of gC for αh and Eh,h+1 is the matrix whose (h,h+1)-element is 1 and whose other elements are all [math].
Since 0<h<p, we have (s2)
[TABLE]
For this reason, the supposition (S) in Theorem 3.1 holds for this example.
Incidentally, L=CG(Th)=S(U(h)×U(p−h,q)), and Theorem 3.1 implies that the complex Lie algebra O(T1,0(G/L)) of holomorphic vector fields on G/L=SU(p,q)/S(U(h)×U(p−h,q)) is isomorphic to sl(p+q,C), where p+q≥2, 0<h<p.
Unfortunately, there are examples of elliptic orbits to which we cannot apply Theorem 3.1.
Example 4.2**.**
The supposition (S) in Theorem 3.1 cannot hold for any symmetric bounded domain D in Cn at all.
Let us explain the reason why.
In order to do so, we consider an elliptic orbit G/L=G/CG(T) in the setting of Subsection 3.1, and put u:=[T,g].
Since adT∈End(g) is semisimple and l=cg(T) one can decompose g as g=l⊕u, and furthermore decompose it as follows:
is a necessary condition for the (s2) to hold.
However, if G/L is a symmetric bounded domain in Cn (where G is the identity component of Hol(G/L)), then k∩l=k, p∩l={0}, k∩u={0} and p∩u=p.
For this reason, the supposition (S) cannot hold for the D at all.
The following example is interesting, we think:
Example 4.3** (G/L=G2(2)/(SL(2,R)⋅T1)).**
Let gC be the exceptional complex simple Lie algebra (g2)C of the type G2.
Assume that the Dynkin diagram of △=△(gC,hC) is as follows (cf. Bourbaki [3, p.289]222There is a minor misprint in [3]: p.289, ↓ 9, Add α2 to (II) Positive roots.):
First of all, let us set a non-compact real form g of gC.
Define a compact real form gu of gC by hR:=spanR{Hα∣α∈△}, gu:=ihR⊕⨁α∈△spanR{Eα−E−α}⊕spanR{i(Eα+E−α)}, and denote by {Z1,Z2}⊂hR the dual base of Π△={α1,α2} (cf. Paragraph 2.3.1 for Hα, Eα).
By use of this Z2 we set
[TABLE]
Then θ is an involutive automorphism of the complex Lie algebra gC such that θ(gu)⊂gu, and we define a non-compact real form g⊂gC in the following way:
[TABLE]
Remark here that gu=k⊕ip, k=sp(1)⊕sp(1) and g=g2(2); besides,
[TABLE]
where kC is the complex subalgebra of gC generated by k.
In this setting, a given T∈ihR is an elliptic element of g and we know that for l:=cg(T),
(a)
l=sl(2,R)⊕t1 in case of T=i(Z1−2Z2),
2. (b)
l=sl(2,R)⊕t1 in case of T=i(Z1−3Z2).
cf. Proposition 5.5 [1, p.1157].
We investigate the cases (a) and (b), individually.
Case (a): Let T:=i(Z1−2Z2) and Πa:={2α1+α2,−3α1−2α2}.
Then Πa is a fundamental root system of △ such that (s1) α(−iT)≥0 for all α∈Πa.
Indeed, it follows from αk(Zj)=δkj that (2α1+α2)(−iT)=0 and (−3α1−2α2)(−iT)=1.
Since (4.4) yields θ(E−3α1−2α2)=E−3α1−2α2, we have (s2) g−3α1−2α2⊂kC.
Therefore the supposition (S) in Theorem 3.1 holds in this case.
Case (b): Let T:=i(Z1−3Z2) and Πb:={α1,−3α1−α2}.
Then, Πb is a fundamental root system of △ such that (s1) α1(−iT)=1 and (−3α1−α2)(−iT)=0.
\alpha_{1}$$-3\alpha_{1}-\alpha_{2}$$\Pi_{b}:
From (4.4) one obtains (s2) θ(Eα1)=Eα1.
Hence the supposition (S) in Theorem 3.1 holds in this case, also.
We end this paper with a comment on Example 4.3, G/L=G2(2)/(SL(2,R)⋅T1).
In both the cases (a) and (b), the supposition (S) in Theorem 3.1 holds.
So, in each case Theorem 3.1 implies that the complex Lie algebra O(T1,0(G/L)) of holomorphic vector fields on G/L is isomorphic to O(T1,0(GC/Q−)).
Then,
a.
O(T1,0(G/L)) is isomorphic to (g2)C in case (a); but, in contrast,
2. b.
O(T1,0(G/L)) is isomorphic to so(7,C) in case (b).
cf. the proof of Theorem 7.1 in Oniščik [11, p.238–239].
Acknowledgements
The author would like to express his sincere gratitude to Professor Soji Kaneyuki for the valuable suggestions in Kyoto, 24 October 2005.
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