I offer my perspective on some recent developments in quantum-gravity phenomenology. Among these I stress that some novel opportunities might arise from the analysis of quantum-gravity effects for macroscopic system, but progress in this direction requires in particular a proper description of the total momentum of a macroscopic body when quantum properties of spacetime are taken into account. Also significant are the potentialities for a reach phenomenology associated with effects of dual gravity lensing.Keywords: Loop quantum gravity; deformed hypersurface-deformation algebra; noncommutativity.
Preliminary remarksThe relatively new field of quantum-gravity phenomenology is growing at a very fast pace. I am working at an update my "living review" of the field 1 , and in the process of doing this it as natural to pause for trying to put in focus which recent developments might have a particularly strong impact on the field in the coming years. I offer these thoughts here, focusing mainly on the two such topics for which I also can offer a small contribution toward the development of the relevant formalisms. The first of these topics is the one of quantum-gravity effects for macroscopic systems, for which in particular I shall here offer a contribution to the debate on the total momentum of a macroscopic body in a quantum spacetime. The other topic is dual gravity lensing, a class of effects that only recently surfaced in the quantum-gravity literature and for which I shall here offer a possible setup for its phenomenological study.
Total momentum of a macroscopic body in a quantum spacetimeAn emerging line of study within quantum-gravity phenomenology concerns the effects of quantum gravity on macroscopic bodies 2-10 . One of the most promising approaches for providing guidance to these studies is aimed at formulating manifestations of the Planck scale on momentum space 11-14 . In the relevant quantumgravity pictures there are nonlinearities of the law of composition of momenta which are suppressed by the Planck scale and would be unobservably small for particles at energies we presently can access, but in the analysis of a macroscopic body one might have to add up very many of such minute nonlinearities. The opportunities for phenomenology reside in this mechanism of "amplification", but I shall be here concerned with the fact that in order for the phenomenology to be viable this am-