“…For the case of a positive cosmological constant, there is no asymptotic spatial boundary, and the picture is not as clean. One can, however, look at the asymptotic symmetries at timelike infinity [30][31][32]; or impose boundary conditions on a tube, which can be viewed as the world line of an observer [33]; or continue to negative Λ [34]; or perhaps obtain a central charge directly from the symmetries of the phase space [35]. One obtains a consistent answer: a "puncture" with SL(2, C) holonomy conjugate to…”