A weighted extremal function and equilibrium measure

preprint2015arXivOpen access

Abstract

Let K=Rn⊂CnK={\bf R}^n\subset {\bf C}^n and Q(x):=12log⁡(1+x2)Q(x):=\frac{1}{2}\log (1+x^2) where x=(x1,...,xn)x=(x_1,...,x_n) and x2=x12+⋯+xn2x^2 = x_1^2+\cdots +x_n^2. Utilizing extremal functions for convex bodies in Rn⊂Cn{\bf R}^n\subset {\bf C}^n and Sadullaev's characterization of algebraicity for complex analytic subvarieties of Cn{\bf C}^n we prove the following explicit formula for the weighted extremal function VK,QV_{K,Q}: VK,Q(z)=12log⁡([1+∣z∣2]+{[1+∣z∣2]2−∣1+z2∣2}1/2)V_{K,Q}(z)=\frac{1}{2}\log \bigl( [1+|z|^2] + \{ [1+|z|^2]^2-|1+z^2|^2\}^{1/2}) where z=(z1,...,zn)z=(z_1,...,z_n) and z2=z12+⋯+zn2z^2 = z_1^2+\cdots +z_n^2. As a corollary, we find that the Alexander capacity Tω(RPn)T_ω({\bf R} {\bf P}^n) of RPn{\bf R} {\bf P}^n is 1/21/\sqrt 2. We also compute the Monge-Ampère measure of VK,QV_{K,Q}: (ddcVK,Q)n=n!1(1+x2)n+12dx.(dd^cV_{K,Q})^n = n!\frac{1}{(1+x^2)^{\frac{n+1}{2}}}dx.

Explore this paper’s authors, topics and related work.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Reviews 0

Write a reviewWrite

No reviews yet.

Discussion 0

Add a commentWrite

No comments yet.