It is known that, using the Gaussian beam approximation, one can show that there
exist solutions of the wave equation on a general globally hyperbolic Lorentzian
manifold whose energy is localised along a given null geodesic for a finite, but
arbitrarily long, time. We show that the energy of such a localised solution is
determined by the energy of the underlying null geodesic. This result opens the
door to various applications of Gaussian beams on Lorentzian manifolds
that
do not admit a globally timelike Killing vector field. In particular, we
show that trapping in the exterior of Kerr or at the horizon of an extremal
Reissner–Nordström black hole necessarily leads to a “loss of derivative”
in a local energy decay statement. We also demonstrate the obstruction
formed by the red-shift effect at the event horizon of a Schwarzschild black
hole to scattering constructions from the future (where the red-shift turns
into a blue-shift): we construct solutions to the backwards problem whose
energies grow exponentially for a finite, but arbitrarily long, time. Finally, we
give a simple mathematical realisation of the heuristics for the blue-shift
effect near the Cauchy horizon of subextremal and extremal black holes: we
construct a sequence of solutions to the wave equation whose initial energies are
uniformly bounded, whereas the energy near the Cauchy horizon goes to
infinity.
Keywords
Gaussian beams, characterisation of energy, spacetime