The most general Lagrangian for non-linear electrodynamics coupled to an
axion a and a dilaton ϕ with SL(2,\mbox{\elevenmsb R}) invariant
equations of motion is -\half\left(\nabla\phi\right)^2 - \half
e^{2\phi}\left(\nabla a\right)^2 + \fraction{1}{4}aF_{\mu\nu}\star F^{\mu\nu} +
L_{\rm inv}(g_{\mu\nu},e^{-\frac{1}{2}\phi}F_{\rho\sigma}) where Linv(gμν,Fρσ) is a Lagrangian whose equations of motion are
invariant under electric-magnetic duality rotations. In particular there is a
unique generalization of Born-Infeld theory admitting SL(2,\mbox{\elevenmsb
R}) invariant equations of motion.Comment: 9 pages, LaTe