The Loewner-Kufarev Energy and Foliations by Weil-Petersson Quasicircles

Abstract

We study foliations by chord-arc Jordan curves of the twice punctured Riemann sphere $\mathbb C \smallsetminus \{0\}$ using the Loewner-Kufarev equation. We associate to such a foliation a function on the plane that describes the "local winding" along each leaf. Our main theorem is that this function has finite Dirichlet energy if and only if the Loewner driving measure $ρ$ has finite Loewner-Kufarev energy, defined by $$S(ρ) = \frac{1}{2}\iint_{S^1 \times \mathbb{R}} ν_t'(θ)^2 \, d θd t$$ whenever $ρ$ is of the form $ν_t(θ)^2 d θd t$, and set to $\infty$ otherwise. Moreover, if either of these two energies is finite they are equal up to a constant factor, and in this case, the foliation leaves are Weil-Petersson quasicircles. This duality between energies has several consequences. The first is that the Loewner-Kufarev energy is reversible, that is, invariant under inversion and time-reversal of the foliation. Furthermore, the Loewner energy of a Jordan curve can be expressed using the minimal Loewner-Kufarev energy of those measures that generate the curve as a leaf. This provides a new and quantitative characterization of Weil-Petersson quasicircles. Finally, we consider conformal distortion of the foliation and show that the Loewner-Kufarev energy satisfies an exact transformation law involving the Schwarzian derivative. The proof of our main theorem uses an isometry between the Dirichlet energy space on the unit disc and $L^2(2ρ)$ that we construct using Hadamard's variational formula expressed by means of the Loewner-Kufarev equation. Our results are related to $κ$-parameter duality and large deviations of Schramm-Loewner evolutions coupled with Gaussian random fields.

Figures (3)

• Figure 1.1: Illustration of the winding function $\varphi$.
• Figure 4.1: Left: Leaves of the foliation corresponding to the measure that equals $\pi^{-1}\sin^2(\theta / 2) \,\mathrm{d} \theta \mathrm{d} t$ for $0 \leqslant t < 1$ and is uniform for $t \geqslant 1$, drawn at equidistant times. Right: Density plot of the winding function corresponding to the same measure, where lighter color represents a larger value. The winding function is harmonic, but non-zero, in the part foliated after time $1$.
• Figure 9.1: Conformal distortion of a foliation. The mapping $\psi$ is conformal in a neighborhood of the hull $K$ generated by $\rho$, which is mapped to another hull $\tilde{K}$, generated by a measure $\tilde{\rho}$. Proposition \ref{['prop:conformal-distortion']} computes the difference of the Loewner--Kufarev energies of $\rho$ and $\tilde{\rho}$.

Theorems & Definitions (129)

• Theorem 1.1: Weil--Petersson leaves
• Theorem 1.2: Energy duality
• Remark
• Theorem 1.3: Energy reversibility
• Theorem 1.4: Characterization of Weil--Petersson quasicircles
• Proposition 1.5: Complex identity
• Theorem 1.6: Conformal distortion
• Theorem 1.7: Disk energy duality
• Theorem 1.8: Foliation disintegration isometry
• Remark