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A strictly pseudoconvex boundary point has a local holomorphic separator

Statement

Assume the Axiom of Choice (AC). Let D⊆Cn, n≥1, be a domain and let p∈∂D be a boundary point such that ∂D is of class C2 near p and strongly pseudoconvex at p. In this item, zj denotes the canonical coordinate zj−1 for 1≤j≤n, with the same relabeling for derivatives and form coefficients. There are a neighbourhood U of p and a C2 function ρ:U→R with D∩U={z∈U:ρ(z)<0},dρ(p)≠0, and Lρ(p;v)>0for every v≠0 with ∑j=1n∂ρ∂zj(p)vj=0.

Then there are a neighbourhood V⊆U of p and a holomorphic function h:V→C such that h(p)=0andRe⁡h(z)<0 for every z∈(D∩V)∖{p}.

In particular h has no zero on (D∩V)∖{p}. Moreover the separator is quantitative in suitable coordinates: there are a holomorphic chart w centred at p, a radius δ>0 and a constant c>0 such that h=wn in this chart and Re⁡wn≤−c∣w∣2 at every point of D corresponding to ∣w∣<δ.

Facts & Assumptions

Given: The Axiom of Choice; a domain D⊆Cn; a boundary point p∈∂D with C2 boundary near p; a C2 defining function ρ on a neighbourhood U of p with D∩U={ρ<0}, dρ(p)≠0, and Lρ(p;v)>0 for every nonzero complex tangent vector v at p.

[F1]

For u∈C2 open set and a, v as above, the Levi form is Lu(a;v):=∑j,k∂2u∂zj∂zˉk(a)vjvk‾, and u is strictly plurisubharmonic when Lu(a;v)>0 for all a and all v≠0 (The Levi form and strict plurisubharmonicity).

[F2]

With ρ a C2 defining function of a domain on a neighbourhood of a boundary point p, the complex tangent vectors at p are those with ∑jρzj(p)vj=0, and the Levi form is evaluated on that subspace (Levi pseudoconvex domains).

[F3]

Two C2 defining functions near the same boundary point have Levi forms on complex tangent vectors differing by a positive scalar factor; in particular the strict positivity demanded at p does not depend on the choice of ρ (Levi pseudoconvexity does not depend on the defining function).

[F4]

For a C2 scalar field near a, f(a+h)=f(a)+∇f(a)⋅h+12⟨Hf(a)h,h⟩+o(∥h∥2) (Second-order Taylor expansion f(a+h)=f(a)+∇f(a)⋅h+12hTHf(a)h+o(∥h∥2)).

[F5]

The Wirtinger operators in several variables satisfy Df(a)h=∑k((∂zkf(a))hk+(∂zˉkf(a))hk‾) for real totally differentiable f, and ρ real-valued is recovered from its Wirtinger partials by this identity (Wirtinger operators in Cm).

[F6]

AC states that every family of nonempty sets has a choice function (The Axiom of Choice).

Choice use. AC is the ambient hypothesis stated in the lemma. The normalization, the multiplication by the positive function g, the choice of the polynomial q and the final pullback are all explicit formulas, so neither [F6] nor any weaker selection principle is consumed by the construction itself; the cited suppliers are used as stated.

Proof

technique · direct
1.1F2F5F6given

With U and ρ as given, the only rephrasing needed is the description of the complex tangent space: by [F2] the complex tangent vectors at p form the kernel of the C-linear form ℓ(v):=∑aρza(p)va, and ℓ≠0 because dρ(p)≠0 (if all Wirtinger partials of ρ vanished at p, then Dρ(p)=0 by [F5]); relabel the indices so that ρzn(p)≠0, so that ker⁡ℓ has complex dimension n−1 and the hypothesis of the statement says that ∑a,bρzazˉb(p)vavb‾>0 for every 0≠v∈ker⁡ℓ. The Axiom of Choice [F6] is the ambient hypothesis of the statement, and this step selects nothing.

2.1F4F5step 1.1algebra

Expansion of ρ at p in complex notation: applying the second-order Taylor expansion [F4] to the C2 function ρ and rewriting its linear and quadratic terms with the differential identity of [F5] (for the linear term Dρ(p)h=∑a(ρza(p)ha+ρzˉa(p)ha‾)=2Re⁡ℓ(h), because ρ is real; for the quadratic term, substituting the real coordinates ξa=(ha+ha‾)/2 and ηa=(ha−ha‾)/(2i) into the real Hessian form and collecting the hahb, hahb‾, ha‾hb‾ terms), one obtains with ℓ(h):=∑aρza(p)ha, A(h):=∑a,bρzazb(p)hahb and Q0(h):=∑a,bρzazˉb(p)hahb‾ the expansion ρ(p+h)=2Re⁡ℓ(h)+Re⁡A(h)+Q0(h)+o(∣h∣2) as h→0.

3.1F1F2F3step 1.1step 2.1algebra

First normalization: define the holomorphic affine map Φ by Φ(ζ)a:=pa+ζa for 1≤a<n and Φ(ζ)n:=pn+c(ζn−2∑1≤a<nρza(p)ζa) with c:=(2ρzn(p))−1, so that ℓ(Φ(ζ)−p)=ζn/2 and the Jacobian of Φ is triangular with diagonal entries 1 and c≠0; shrinking U makes Φ a biholomorphism onto a neighbourhood of 0, and ρ1:=ρ∘Φ is a C2 defining function of D1:=Φ−1(D∩U) near 0 with expansion ρ1(ζ)=Re⁡ζn+Q1(ζ)+Re⁡A1(ζ)+o(∣ζ∣2) from step 2.1, where Q1(ζ)=∑a,bρ1,ζaζˉb(0)ζaζb‾ and A1(ζ)=∑a,bρ1,ζaζb(0)ζaζb. The hypothesis survives: ℓ1(w):=∑aρ1,ζa(0)wa equals ℓ(Lw)=wn/2 for the linear part L of Φ, and for v≠0 with ℓ1(v)=0 the chain rule gives Lv∈ker⁡ℓ∖{0} together with Lρ1(0;v)=Lρ(p;Lv)>0 by step 1.1.

4.1F1step 3.1algebra

Multiplication by a positive function: for t>0 put gt(ζ):=1+tRe⁡ζn and ρt:=gtρ1, a C2 defining function of the same domain near 0 with gt(0)=1 and dρt(0)=dρ1(0)≠0. Writing ℓ1(ζ)=ζn/2 and Lt:=tℓ1 and using the identity 2Re⁡(X)2Re⁡(Y)=2Re⁡(XY‾)+2Re⁡(XY), multiplication of the expansion of step 3.1 by gt=1+2Re⁡Lt gives ρt(ζ)=2Re⁡[ℓ1(ζ)+12A1(ζ)+Lt(ζ)ℓ1(ζ)]+[Q1(ζ)+2Re⁡(Lt(ζ)ℓ1(ζ)‾)]+o(∣ζ∣2), the O(∣ζ∣3) terms of 2Re⁡(Lt)(Re⁡A1+Q1) having been absorbed into o(∣ζ∣2); thus the holomorphic quadratic part of ρt is Bt:=ζn/2+A1/2+tζn2/4 and its Hermitian quadratic part is the Hermitian form Ht(v):=Q1(v)+(t/2)∣vn∣2 in the variable v.

5.1step 1.1step 4.1algebra

Ht is positive definite for all large t: the hypothesis of step 1.1 says Q1(v)>0 for 0≠v with vn=0, so on the hyperplane E:={vn=0} there is δ>0 with Q1(v)≥δ∣v∣2, while the Hermitian form Q1 satisfies ∣Q1(v,w)∣≤C∣v∣∣w∣ for v,w∈E with a constant C independent of t. Decomposing v=v′+λen with v′∈E and λ=vn gives Ht(v)=Q1(v′)+2Re⁡Q1(v′,λen)+∣λ∣2Q1(en)+(t/2)∣λ∣2≥δ∣v′∣2−2C∣v′∣∣λ∣+(Q1(en)+t/2)∣λ∣2, and 2C∣v′∣∣λ∣≤(δ/2)∣v′∣2+(2C2/δ)∣λ∣2 because (δ/2∣v′∣−2/δC∣λ∣)2≥0. Choosing t>0 with Q1(en)+t/2≥1+2C2/δ therefore gives Ht(v)≥(δ/2)∣v′∣2+∣λ∣2≥c∣v∣2 for all v, where c:=min⁡(δ/2,1)>0 and ∣v∣2=∣v′∣2+∣λ∣2; fix such a t and write ρt and H for ρt and Ht.

6.1step 4.1step 5.1algebra

Killing the holomorphic quadratic part: let q(ζ):=−A1(ζ)−(t/2)ζn2 and define the holomorphic polynomial map Φ2(w):=w+q(w)en, which fixes the first n−1 coordinates and sends wn to wn+q(w); since DΦ2(0)=I it is a local biholomorphism fixing 0, and with ρ^:=ρt∘Φ2 one computes for z=Φ2(w) that ℓ1(w+q(w)en)=wn/2+q(w)/2 and A1(w+q(w)en)=A1(w)+O(∣w∣3), hence 2Re⁡Bt(Φ2(w))=Re⁡wn+Re⁡[q(w)+A1(w)+(t/2)wn2]+O(∣w∣3)=Re⁡wn+O(∣w∣3), while H(Φ2(w))=H(w)+O(∣w∣3) because H is quadratic; therefore ρ^(w)=Re⁡wn+H(w)+o(∣w∣2), and ρ^ is a C2 defining function near 0 of the image of D under the change of coordinates.

7.1step 5.1step 6.1algebra∎

Conclusion: since ρ^(w)−Re⁡wn−H(w)=o(∣w∣2), after shrinking the ball to a radius δ>0 on which Φ2 is biholomorphic and ∣ρ^(w)−Re⁡wn−H(w)∣≤(c/2)∣w∣2, every w with ∣w∣<δ, w≠0 and ρ^(w)<0 satisfies Re⁡wn=ρ^(w)−H(w)−(ρ^(w)−Re⁡wn−H(w))≤0−c∣w∣2+(c/2)∣w∣2=−(c/2)∣w∣2<0; define V:=Φ(Φ2(B(0,δ)))⊆U and h(z):=wn(z) where w=Φ2−1(Φ−1(z)) is the inverse chart, so that h is holomorphic on V, h(p)=0, and Re⁡h<0 on (D∩V)∖{p} because those points correspond exactly to the parameters ∣w∣<δ, w≠0, ρ^(w)<0, and the displayed inequality is the quantitative bound Re⁡wn≤−(c/2)∣w∣2 in the chart w with the constant c/2>0 of step 5.1.

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