Transverse expansion of the metric at null infinity
Marc Mars, Gabriel Sánchez-Pérez
TL;DR
This work develops a comprehensive, coordinate-free framework for solving the conformal Einstein equations to infinite order at null infinity in arbitrary dimensions and topologies. By employing hypersurface data and a transverse expansion formalism, the authors identify the free data encoded on ${\mathscr I}$ that determine the asymptotic geometry and prove a uniqueness theorem: two asymptotically flat spacetimes with the same free data are isometric to infinite order at ${\mathscr I}$. They establish an existence theorem ensuring such data can be realized by a smooth ambient spacetime, provided obstructions vanish. The analysis reveals obstruction tensors (Coulombian and radiative) whose vanishing is essential for smooth realizations and links these obstructions to the Bach tensor in 4D and the Fefferman–Graham obstruction in higher dimensions, offering a path toward higher-dimensional Bondi-type quantities and asymptotic dynamics.
Abstract
In this paper we analyze the conformal Einstein equations to all orders at null infinity without imposing any restriction on the spacetime dimension, the topology of $\mathscr{I}$, or fall-off conditions for the Weyl tensor. In particular, we study how the equations constrain the geometry of null infinity when it is assumed to be foliated by cross-sections, not necessarily spheres. Our approach is coordinate-free and treats the conformal factor $Ω$ as a dynamical variable. After identifying the free data at $\mathscr{I}$, we show that any two asymptotically flat spacetimes sharing the same free data at null infinity are necessarily isometric to infinite order. In addition, we provide a detached definition of null infinity and prove an existence theorem for asymptotically flat spacetimes solving the field equations to infinite order at $\mathscr{I}$ realizing the prescribed initial data.
