Asymptotic symmetries of AdS4 quantum gravity and gauge theory are derived
by coupling the dual CFT3 to Chern-Simons gauge theory and 3D gravity in a
"probe" large-level limit. The infinite-dimensional symmetries are shown to
arise when one is restricted to boundary subspaces with effectively
two-dimensional geometry. A canonical example of such a restriction occurs
within the 4D subregion described by a Wheeler-DeWitt wavefunctional of AdS4
quantum gravity. An AdS4 analog of Minkowski "super-rotation" asymptotic
symmetry is probed by 3D Einstein gravity, yielding CFT2 structure, via
AdS3 foliation of AdS4 and the AdS3/CFT2 correspondence. The
maximal asymptotic symmetry is however probed by 3D conformal gravity. Both 3D
gravities have Chern-Simons formulation, manifesting their topological
character. Chern-Simons structure is also shown to be emergent in the Poincare
patch of AdS4, as soft/boundary limits of 4D gauge theory, rather than "put
in by hand", with a finite effective Chern-Simons level. Several of the
considerations of asymptotic symmetry structure are found to be simpler for
AdS4 than for Mink4, such as non-zero 4D particle masses, 4D
non-perturbative "hard" effects, and consistency with unitarity. The last of
these, in particular, is greatly simplified, because in some set-ups the time
dimension is explicitly shared by each level of description: Lorentzian
AdS4, CFT3 and CFT2. The CFT2 structure clarifies the sense in
which the infinite asymptotic charges constitute a useful form of "hair" for
black holes and other complex 4D states. An AdS4 (holographic) "shadow"
analog of Minkowski "memory" effects is derived. Lessons from AdS4 provide
hints for better understanding Minkowski asymptotic symmetries, the 3D
structure of its soft limits, and Minkowski holography.Comment: typos corrected, references added, discussions of boundary conditions
corrected and clarifie