Abstract

In general relativity, the description of spacetime relies on idealised rods and clocks, which identify a reference frame. In any concrete scenario, reference frames are associated to physical systems, which are ultimately quantum in nature. A relativistic description of the laws of physics hence needs to take into account such quantum reference frames (QRFs), through which spacetime can be given an operational meaning. Here, we introduce the notion of a spacetime quantum reference frame, associated to a quantum particle in spacetime. Such formulation has the advantage of treating space and time on equal footing, and of allowing us to describe the dynamical evolution of a set of quantum systems from the perspective of another quantum system, where the parameter in which the rest of the physical systems evolves coincides with the proper time of the particle taken as the QRF. Crucially, the proper times in two different QRFs are not related by a standard transformation, but they might be in a quantum superposition one with respect to the other.Concretely, we consider a system of N relativistic quantum particles in a weak gravitational field, and introduce a timeless formulation in which the global state of the N particles appears "frozen", but the dynamical evolution is recovered in terms of relational quantities. The position and momentum Hilbert space of the particles is used to fix the QRF via a transformation to the local frame of the particle such that the metric is locally inertial at the origin of the QRF. The internal Hilbert space corresponds to the clock space, which keeps the proper time in the local frame of the particle. Thanks to this fully relational construction we show how the remaining particles evolve dynamically in the relational variables from the perspective of the QRF. The construction proposed here includes the Page-Wootters mechanism for non interacting clocks when the external degrees of freedom are neglected. Finally, we find that a quantum superposition of gravitational redshifts and a quantum superposition of special-relativistic time dilations can be observed in the QRF.

Highlights

  • In both quantum theory and general relativity, spacetime is treated as an abstract entity

  • We have introduced the notion of a spacetime quantum reference frame, i.e., a reference frame in spacetime associated to a quantum system which can be in a superposition, or entangled from the point of view of another quantum system

  • We have developed a formulation to describe a set of relativistic quantum particles in a weak gravitational field from the perspective of such spacetime quantum reference frame

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Summary

Introduction

In both quantum theory and general relativity, spacetime is treated as an abstract entity. A spacetime formulation of QRFs is a crucial step towards a fully relational and covariant description of physics from the point of view of a quantum system, and could provide a natural setting for a quantum approach to time. When one of the particles, say particle 1, acts as a QRF, the external part of the quantum state is used to fix the QRF (in our case, the origin of the coordinate system in spacetime), while the internal part serves as a clock, ticking according to the proper time in each particle’s frame. We show how to build a fully relational model for quantum particles in spacetime and in a weak gravitational field This construction adopts the tools of QRFs, and unifies the framework for spatial QRFs [25, 26, 27] with time reference frames [36], the latter in the non-interacting case.

Extended symmetries and QRF changes
Gravitational redshift and relativistic time-dilation from a QRF
Discussion
A Mass dispersion relation in a weak gravitational field
B Comparison between relational approaches
D Action of the T1 operator on the position and momentum operators
E Explicit calculation of the “history state” in the frame of particle 1
F Limiting cases of the general N -particle model
Galilean case
Special-relativistic case
Newtonian case
G Explicit calculation of the “history state” with a quantum measurement
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