For a real-valued C2C^2 function uu on an open subset of Cd\mathbb C^d, the Levi form at zz is the Hermitian form

Lu(z;v)=∑j,k=1d∂2u∂zj∂zˉk(z)vjvk‾,v∈Cd.\mathcal L_u(z;v)= \sum_{j,k=1}^d \frac{\partial^2u}{\partial z_j\partial\bar z_k}(z) v_j\overline{v_k}, \qquad v\in\mathbb C^d.

Its matrix is (uzjzˉk)j,k\bigl(u_{z_j\bar z_k}\bigr)_{j,k}.

Real-coordinate formula

Using ∂zj=12(∂xj−i∂yj)\partial_{z_j}=\tfrac12(\partial_{x_j}-i\partial_{y_j}) and ∂zˉj=12(∂xj+i∂yj)\partial_{\bar z_j}=\tfrac12(\partial_{x_j}+i\partial_{y_j}), the Levi matrix is a particular Hermitian combination of the blocks of the real .

Positivity

A C2C^2 function is exactly when its Levi form is represented by a . A uniform lower bound by a positive Hermitian form is .

References
  1. Steven G. Krantz, Function Theory of Several Complex Variables, 2nd ed., AMS Chelsea, 2001. Publisher record.