Math 2.0

Several complex variables and analytic spaces Definition

Levi form

Builds on Hermitian formSmooth functionOpen set

Definition

Let U⊆ℂnU \subseteq \C^n be an open set and let ρ ⁣:U→ℝ\rho \colon U \to \R be a function of class C2C^2 (see smooth function). The Levi form of ρ\rho at a point p∈Up \in U is the Hermitian form Lρ(p;w)=∑j,k=1n∂2ρ∂zj∂zˉk(p) wjwˉk,w∈ℂn.L_\rho(p; w) = \sum_{j,k=1}^{n} \frac{\partial^2 \rho}{\partial z_j \partial \bar z_k}(p)\, w_j \bar w_k, \qquad w \in \C^n. It is also called the complex Hessian of ρ\rho.

Now let Ω⊆ℂn\Omega \subseteq \C^n be a domain with C2C^2 boundary. A defining function of Ω\Omega is a C2C^2 function ρ\rho on a neighbourhood UU of ∂Ω\partial\Omega with Ω∩U={z∈U:ρ(z)<0}\Omega \cap U = \set{z \in U : \rho(z) < 0} and dρ≠0d\rho \ne 0 on ∂Ω\partial\Omega. For p∈∂Ωp \in \partial\Omega, the complex tangent space of ∂Ω\partial\Omega at pp is Hp={w∈ℂn:∑j=1n∂ρ∂zj(p) wj=0}.H_p = \set{w \in \C^n : \sum_{j=1}^{n} \frac{\partial \rho}{\partial z_j}(p)\, w_j = 0}. The Levi form of ∂Ω\partial\Omega at pp is the restriction of Lρ(p;⋅)L_\rho(p; \cdot) to HpH_p.

Remarks

Example: for the unit ball, ρ(z)=∣z1∣2+⋯+∣zn∣2−1\rho(z) = \abs{z_1}^2 + \cdots + \abs{z_n}^2 - 1 has ∂2ρ/∂zj∂zˉk=δjk\partial^2 \rho / \partial z_j \partial \bar z_k = \delta_{jk}, so Lρ(p;w)=∣w∣2>0L_\rho(p; w) = \abs{w}^2 > 0 for every w≠0w \ne 0. Non-example of positivity: for the bidisc, near a boundary point p=(1,b)p = (1, b) with ∣b∣<1\abs{b} < 1, a defining function is ρ(z)=∣z1∣2−1\rho(z) = \abs{z_1}^2 - 1. Here Hp={w:w1=0}H_p = \set{w : w_1 = 0}, and Lρ(p;(0,w2))=0L_\rho(p; (0, w_2)) = 0, so the Levi form vanishes on HpH_p. If ρ\rho is replaced by another defining function hρh \rho with h>0h > 0, the Levi form of ∂Ω\partial\Omega at pp is multiplied by h(p)h(p). So its signature does not depend on the choice. The signature is also unchanged under holomorphic changes of coordinates.

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