Cartan's lemma (potential theory)
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Short description: Mathematical Lemma
In potential theory, a branch of mathematics, Cartan's lemma, named after Henri Cartan, is a bound on the measure and complexity of the set on which a logarithmic Newtonian potential is small.
Statement of the lemma
The following statement can be found in Levin's book.[1]
Let μ be a finite positive Borel measure on the complex plane C with μ(C) = n. Let u(z) be the logarithmic potential of μ:
- [math]\displaystyle{ u(z) = \frac{1}{2\pi}\int_\mathbf{C} \log|z-\zeta|\,d\mu(\zeta) }[/math]
Given H ∈ (0, 1), there exist discs of radii ri such that
- [math]\displaystyle{ \sum_i r_i \lt 5H }[/math]
and
- [math]\displaystyle{ u(z) \ge \frac{n}{2\pi}\log \frac{H}{e} }[/math]
for all z outside the union of these discs.
Notes
- ↑ B.Ya. Levin, Lectures on Entire Functions
Original source: https://en.wikipedia.org/wiki/Cartan's lemma (potential theory).
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