3. From Dunkl to Levi-Civita
3.3 Flat Hermitian forms for reflection arrangements
It may very well hold in a much greater generality.
Theorem 3.7. — Suppose that H is the reflection arrangement of a finite complex reflection group G. Then there exists a map from (RH)G to the space of nonzero Hermitian forms on the tangent bundle of V◦ (denoted κ→hκ) with the following properties: for every κ∈(RH)G,
(i)hκ is flat for ∇κ and invariant under G.
(ii)t ∈ R→ htκ is smooth (notice that h0 was already defined) and the associated curve of projectivized forms, t → [htκ] is real-analytic.
Moreover, hκ is unique up to scalar multiple (relative to (i) and (ii)).
Likewise there is a map from (RH)G to the space of nonzero Hermitian forms on the cotan-gent bundle of V◦ with analogous properties.
Example 3.8. — For V =C and Ω = κz−1dz, we can take hκ(z):= |z|−2κ|dz|2. Notice that we can expand this in powers of κ as
hκ(z)= ∞
k=0
κk(−log|z|2)k k! |dz|2.
We shall first prove that in the situation of Theorem 3.7 we can find such an hκ formally at κ = 0. For this we need the following notion, suggested by Example 3.8.
Let be given a complex manifold M and a smooth hypersurface D⊂M. We say that a function f on a neighborhood of p in M−D is logsingular of order ≤ k along D if there is a defining equation φ ofD at p such that f can be written as a polynomial of degree ≤k in log|φ| with coefficients that are real-analytic on Mp. Since φ is unique up to a unit as a factor, log|φ| is unique up to the addition of a real-analytic function on Mp and so any generator of OM,p(−D) will do for this purpose.
We say that a differential η on a neighborhood of p in M−D is logsingular of order ≤ k along D at p if it is a linear combination of real-analytic forms on Mp and
|φ|−1d|φ| =Re(dφ/φ) and with logsingular functions of order ≤k as coefficients, but with the coefficient of |φ|−1d|φ| being of order ≤ k −1 (read equal to zero when k=0).
Lemma 3.9. — In this situation we have:
(i)log|w| is algebraically independent over the ring of real-analytic functions on Mp. (ii) Any logsingular differential of order ≤k atp that is closed is the differential of a
logsin-gular function of order ≤k at p.
Proof. — The proof of (i) is left to the reader. For the proof of (ii) we use a re-traction Mp →Dp in order to identify Mp withDp×C0 and employ polar coordinates (r, θ) on the second coordinate. Ifη is a logsingular differential of order≤k at p, then we can write
η= k
i=0
(logr)i(αi+girdθ)+
k−1
i=0
(logr)ifir−1dr,
withαi a differential on Dp whose coefficients are real-analytic functions on Mp and fi
andgi real-analytic on Dp×R0×S1. Since limr↓0r(logr)i =0 fori ≥0, the integral of such a form over the circle{(p,r)}×S1 tends to zero as r tends to zero. Hence, ifη is closed, then the integral over any such circle is closed and the form can be integrated to a function on (M−D)p. A straightforward verification shows that this function is
logsingular of order ≤k.
Lemma 3.10. — In the situation of Theorem 3.7, let κ∈(RH)G. Then there exists a for-mal expansion hsκ = ∞
k=0skhk in G-invariant Hermitian forms with initial coefficient h0=h0
and such thathk is logsingular of order ≤k along the smooth part of the arrangement and with the property that hsκ is flat for ∇sκ.
Proof. — The flatness of hsκ means that for every pair v,v ∈V (when regarded as translation invariant vector fields onV) we have
d(hsκ(v,v))= −shsκ(Ωκ(v),v)−shsκ(v,Ωκ(v)), whereΩκ(v)=
HκHπH(v)⊗ωH, which boils down to
d(hk+1(v,v))= −hk(Ωκ(v),v)−hk(v,Ωκ(v)), k=0,1,2, ... . (∗)
In other words, we must show that we can solve (∗)inductively by G-invariant forms.
In case we can solve (∗), then it is clear that a solution will be unique up to a con-stant.
The first step is easy: if we choose our defining equation φH ∈ V∗ for H to be such that φH, φH =1, then
h1(v,v):= −κH
H
πH(v), πH(v)log|φH|2
will do. Suppose that for some k ≥ 1 the forms h0, ...,hk have been constructed. In order that (∗) has a solution for hk+1 we want the right-hand side (which we shall denote by ηk(v,v)) to be exact. It is certainly closed: if we agree that h(ω⊗v, ω⊗v) stands for h(v,v)ω∧ω, then
dηk(v,v)=hk−1(Ωκ∧Ωκ(v),v)−hk−1(Ωκ(v),Ωκ(v)) +hk−1(Ωκ(v),Ωκ(v))+hk−1(v,Ωκ∧Ωκ(v))
=hk−1(Ωκ∧Ωκ(v),v)+hk−1(v,Ωκ∧Ωκ(v))=0
(since Ωκ∧Ωκ = 0). So in order to complete the induction step, it suffices by Lem-ma 3.9 that to prove that ηk is logsingular of order ≤ k+1 along the arrangement:
since the complement in V of the singular part of the arrangement is simply con-nected, we then write ηk as the differential of a Hermitian form hk+1 on V that is logsingular of order ≤ k+1 along the arrangement and averaging such hk+1 over its G-transforms makes it G-invariant as well.
Our induction assumption says that near H◦ we can expand hk in log|φH| uniquely as:
hk = k
i=0
(log|φH|)ihk,i
wherehk,i is a real-analytic Hermitian form on TVH◦. Now ηk = −
H∈H
k i=0
κH(log|φH|)i hk,i
πH(v),v
ωH+hk,i
v, πH(v) ωH
.
The terms indexed byH =Hare linear combinations of differentials that are regular atH◦ with logsingular coefficients of order ≤k and hence are logsingular of order≤k alongH◦. So it remains to show thathk,i(πH(v),v)ωH+hk,i(v, πH(v))ωH is logsingular of order≤k+1alongH◦. To see this, let GH be the group of complex reflections in G with mirrorH. Each termhk,i is invariant underGH (acting on the germVH◦), because hk and |φH| are (and the uniqueness of the expansion in powers of log|φH|). Since πH
is the projection onto an eigenspace ofGH, we find that if a⊥H andb∈H, then the real-analytic function hk,i(a,b) on Mp transforms under GH with the same character as φH. Hence this function is divisible by φH with real-analytic quotient. So
α:=hk,i(πH(v),v)ωH−hk,i(πH(v), πH(v))ωH
=hk,i(πH(v),v−πH(v))dφH
φH is real-analytic. Hence
hk,i(πH(v),v)ωH+hk,i(v, πH(v)ωH
=hk,i(πH(v), πH(v))(ωH+ωH)+α+α
=2hk,i(πH(v), πH(v))d|φH|
|φH| +α+α.
This shows that ηk is logsingular of order ≤k+1.
In order to prove Theorem 3.7, we begin with a few generalities regarding con-jugate complex structures. Denote by V† the complex vector space V with its conju-gate complex structure: scalar multiplication by λ∈C acts on V† as scalar multiplica-tion byλ∈C in V. ThenV⊕V† has a natural real structure for which complex con-jugation is simply interchanging arguments. The ensuing concon-jugation onGL(V⊕V†) is, when restricted toGL(V)×GL(V†), also interchanging arguments, whereas on the space of bilinear forms onV×V†, it is given by h†(v,v):=h(v,v). So a real point of (V⊗V†)∗ is just a Hermitian form on V.
Fix a base point ∗ ∈ V◦ and identify T∗V◦ with V. For κ∈ (CH)G, we denote the monodromy representation of∇κ by ρκ∈Hom(π1(V◦,∗),GL(V)). Notice thatρκ depends holomorphically on κ. Then the same property must hold for
κ∈(CH)G→(ρκ)†∈Hom
π1(V◦,∗),GL(V†) .
Recall from 2.17 that (CH)G is invariant under complex conjugation.
Lemma 3.11. — Let H be the set of pairs (κ,[h])∈ (CH)G×P((V⊗V†)∗), where h ∈V×V† → C is invariant under ρκ⊗(ρκ)† and let p1 : H→ (CH)G be the projection.
Then H resp. p1(H) is a complex-analytic set defined over R (in (CH)G×P((V⊗V†)∗) resp.
(CH)G) and we have p1(H(R))=(RH)G.
Proof. — That H is complex-analytic and defined over R is clear. Since p1 is proper and defined over R, p1(H) is also complex-analytic and defined over R.
If κ ∈ (RH)G is in the image of H, then there exists a nonzero bilinear map h : V×V† → C invariant under ρκ⊗(ρκ)†. But then both the ‘real part’ 12(h+h†) and the ‘imaginary part’ 2√1−1(h −h†) of h are Hermitian forms invariant under ρκ and clearly one of them will be nonzero. The lemma follows.
Proof of Theorem 3.7. — Now let L ⊂ (CH)G be a line defined over R. By the preceding discussion, there is a unique irreducible component L˜ of the preimage of L in H which contains (0,[h0]). The map L˜ → L is proper and the preimage of 0 is a singleton. Hence L˜ →L is an complex-analytic isomorphism. Since L is defined over R, so are L˜ and the isomorphismL˜ →L. The forms parametrized by L˜(R) de-fine a real line bundle overL(R). Such a line bundle is trivial in the smooth category and hence admits a smooth generating section with prescribed value in 0. We thus find a map κ →hκ with the stated properties. The proof for the map the Hermitian
form on the cotangent bundle is similar.
If h is a nondegenerate Hermitian form on the tangent bundle of V◦ which is flat for the Dunkl connection, then ∇ must be its Levi-Civita connection of h (for ∇ is torsion free); in particular, h determines ∇. Notice that to give a flat Hermitian form h amounts to giving a monodromy invariant Hermitian form on the translation space ofA. So h will be homogeneous in the sense that the pull-back ofh under scalar multiplication onV◦ by λ∈C× is |λ|2−2Re(κ0)h.
3.4. The hyperbolic exponent of a complex reflection group. — In case H is a