The tension equation for a mapping $f:{ \mathbb C}\to { \mathbb C}$ is the nonlinear second order equation \[ \Delta f +\varphi(f) f_z f_{ \bar z} = 0\] Solutions are "harmonic" mappings. Here we give a complete description of the solution space of mappings of degree 1 to this equation when $\varphi$ is entire. Each solution is a quasiconformal surjection and when the set of normalised solutions is endowed with the Teichm\"uller metric, the solution space is isometric to the hyperbolic plane. More generally, for harmonic mappings $f:\Omega \to (\tilde{ \Omega},\rho)$ between domains in ${ \mathbb C}$, with $\rho(w)|dw|$ defining a flat metric we stablish a very strong maximum principle for the distortion - up to multiplicative factor $e^{ iv}$, $v$ real and harmonic, the Beltrami coefficient of $f^{ -1}$ is quasiregular - and thus open and discrete when nonconstant. This follows from the remarkable fact that the Beltrami coefficient of the inverse of a harmonic mapping itself satisfies a nonlinear homogeneous Beltrami equation.
Categories: math.CV