Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:2610.33220

Quantum-Relativistic Anomalous Proper Time

Pablo L. Saldanha, Nelson Yokomizo

quant-phgr-qcSubmitted Oct 23, 2026• Announced Oct 27, 2026• 0 citations
arXivHTMLPDF

Abstract

We investigate surprising consequences of the hypothesis that gravity and proper time obey the quantum superposition principle. We show that, for a massive body prepared in a superposition of two positions and post-selected in a suitable final state, the elapsed proper time in another region of space can assume an anomalous effective value lying outside the range allowed by classical general relativity. Remarkably, the effective elapsed proper time can even become negative, corresponding to an effective evolution backward in time. We also propose an experiment to observe an anomalous effective proper time associated with the internal degrees of freedom of a quantum particle in an interferometer under Earth's gravitational field. The proposed experiment is, in principle, feasible with current technology, and its realization could provide the first experimental evidence of an interplay between quantum mechanics and general relativity beyond the effects of the Newtonian potential in flat spacetime.

AI Summary

The paper asks whether coherent superpositions of gravitational time dilation, combined with post-selection, can produce an effective elapsed proper time outside the range of the individual branches. It considers both a probe near a mass in a spatial superposition and an internal atomic clock traversing two heights in Earth’s classical gravitational field. Starting from weak-field evolution $e^{-iH\tau/\hbar}$, it derives the conditional probe dynamics for initial path amplitudes $\alpha,\beta$ and antisymmetric path post-selection. To first order, the evolution corresponds to $\tau_{\mathrm{ef}}=(\beta\tau_B-\alpha\tau_A)/(\beta-\alpha)$, the weak value of a branch-dependent proper-time operator. For positive real amplitudes, this lies outside $[\tau_A,\tau_B]$ and can become negative. The approximate post-selection probability is $|\beta-\alpha|^2/2$; averaging both output ports recovers the classical weighted proper time. An experimental proposal reads out the conditional internal-clock phase through Ramsey interferometry. For an optical transition near $6\times10^{14}\,\mathrm{Hz}$, a $10\,\mathrm{cm}$ average arm-height separation, $1\,\mathrm{s}$ interrogation, and $\beta=1/\sqrt{2}+0.1$, the predicted phase displacement relative to one branch is approximately $0.1$ radians. This configuration uses a classical gravitational field, not a superposition of gravitational fields. The effective-time description requires $\Delta E|\tau_{\mathrm{ef}}-\tau_A|/\hbar<1$, making the anomalous shift smaller than the clock’s single-system time uncertainty and requiring ensemble measurements. Environmental decoherence prevents the proposed macroscopic reversal interpretation. The gravitational-source-superposition scheme is acknowledged to be impractical, while maintaining atomic-clock precision within the proposed interferometer remains an experimental difficulty.

No sign of AI-generated textOverclaimsIncrementalStrong assumptionsMissing comparison

Central claim may not hold: The exact post-selected operation is generally nonunitary, so its approximate anomalous effective time is not an elapsed geometric proper time forbidden by general relativity. The negative-effective-time interpretation requires a sufficiently small amplified shift relative to the probe's inverse energy bandwidth and therefore does not demonstrate unrestricted backward evolution. The Earth-based proposal is described by quantum matter on a prescribed classical spacetime, so its anomalous post-selected phase cannot by itself exclude classical gravity.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

Comments
6 pages, 3 figures

Related papers

Quantum interferometric visibility as a witness of general relativistic proper time

Magdalena Zych, Fabio Costa, Igor Pikovski +1 more

Current attempts to probe general relativistic effects in quantum mechanics focus on precision measurements of phase shifts in matter–wave interferometry. Yet, phase shifts can always be explained as arising because of an Aharonov–Bohm effect, where a particle in a flat space–time is subject to an effective potential. Here we propose a quantum effect that cannot be explained without the general relativistic notion of proper time. We consider interference of a 'clock'—a particle with evolving internal degrees of freedom—that will not only display a phase shift, but also reduce the visibility of the interference pattern. According to general relativity, proper time flows at different rates in different regions of space–time. Therefore, because of quantum complementarity, the visibility will drop to the extent to which the path information becomes available from reading out the proper time from the 'clock'. Such a gravitationally induced decoherence would provide the first test of the genuine general relativistic notion of proper time in quantum mechanics. In the theory of general relativity time flows at different rates depending on the space–time geometry. Here, a drop in the visibility of a quantum 'clock' interference in a gravitational potential is predicted, which cannot be explained without the general relativistic notion of time.

arXiv:1105.4531•Nature Communications•Oct 18, 2011•251 citations

General relativistic effects in quantum interference of photons

Magdalena Zych, Fabio Costa, Igor Pikovski +2 more

Quantum mechanics and general relativity have been extensively and independently confirmed in many experiments. However, the interplay of the two theories has never been tested: all experiments that measured the influence of gravity on quantum systems are consistent with non-relativistic, Newtonian gravity. On the other hand, all tests of general relativity can be described within the framework of classical physics. Here we discuss a quantum interference experiment with single photons that can probe quantum mechanics in curved space-time. We consider a single photon traveling in superposition along two paths in an interferometer, with each arm experiencing a different gravitational time dilation. If the difference in the time dilations is comparable with the photon's coherence time, the visibility of the quantum interference is predicted to drop, while for shorter time dilations the effect of gravity will result only in a relative phase shift between the two arms. We discuss what aspects of the interplay between quantum mechanics and general relativity are probed in such experiments and analyze the experimental feasibility.

arXiv:1206.0965•Classical and Quantum Gravity•Oct 18, 2012•118 citations

Quantum clocks, gravitational time dilation, and quantum interference

Takeshi Chiba, Shunichiro Kinoshita

A proper time observable for a quantum clock is introduced and it is found that the proper time read by one clock conditioned on another clock reading a different proper time obeys classical time dilation in accordance with special relativistic kinematical time dilation. Here, we extend this proposal to a weak gravitational field in order to investigate whether the weak equivalence principle holds for quantum matter. We find that for general quantum states the quantum time dilation in a weak gravitational field obeys a similar gravitational time dilation found in classical relativity. However, unlike the special relativistic case, the time dilation involves the external time (a background coordinate time at the observer on the Earth) as well as the proper times of two clocks. We also investigate a quantum time dilation effect induced by a clock in a superposition of wave packets localized in momentum space or in position space and propose the setup to observe the gravitational effect in the quantum interference effect in the time dilation.

arXiv:2209.07638•Physical review. D/Physical review. D.•Dec 26, 2022•5 citations

Spacetime Quantum Reference Frames and superpositions of proper times

Flaminia Giacomini

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.

arXiv:2101.11628•Quantum•Jul 22, 2021•74 citations

Quantum time dilation in a gravitational field

Jerzy Paczos, Kacper Dębski, Piotr T. Grochowski +2 more

According to relativity, the reading of an ideal clock is interpreted as the elapsed proper time along its classical trajectory through spacetime. In contrast, quantum theory allows the association of many simultaneous trajectories with a single quantum clock, each weighted appropriately. Here, we investigate how the superposition principle affects the gravitational time dilation observed by a simple clock – a decaying two-level atom. Placing such an atom in a superposition of positions enables us to analyze a quantum contribution to a classical time dilation manifest in spontaneous emission. In particular, we show that the emission rate of an atom prepared in a coherent superposition of separated wave packets in a gravitational field is different from the emission rate of an atom in a classical mixture of these packets, which gives rise to a quantum gravitational time dilation effect. We demonstrate that this nonclassical effect also manifests in a fractional frequency shift of the internal energy of the atom that is within the resolution of current atomic clocks. In addition, we show the effect of spatial coherence on the atom's emission spectrum.

arXiv:2204.10609•Quantum•May 7, 2024•10 citations

Proper Time as an Emergent Ratio of Quantum Uncertainties: New Predictions for Quantum Time Dilation and Gravitational Effects

A.B.M Masum Billah Mim

We propose that time is not a fundamental background but emerges from the quantum uncertainties of position, momentum, and energy. This is captured by the postulate \(\Delta \tau = \frac{\Delta x \,\Delta p}{\gamma \,\Delta E}\),where \(\Delta \tau\) is the proper time interval, \(\Delta x,\Delta p,\Delta E\) are the standard quantum uncertainties, and \(\gamma = 1/\sqrt{1-v^2/c^2}\) is the Lorentz factor associated with the average velocity \(v\). Using the standard wave‑packet relation \(\Delta E = v \Delta p\), our equation reduces exactly to the special relativistic proper time \(\Delta \tau = \Delta x/(\gamma v)\), demonstrating consistency with all existing tests. However, for non‑classical quantum states where \(\Delta E \neq v \Delta p\) (e.g., a superposition of widely separated momenta), our equation predicts new measurable effects: (i) a significant modification of the decay length of unstable particles (muons), (ii) a dependence of clock rates on the spatial spread \(\Delta x\) even in flat spacetime, and (iii) a quantum correction to gravitational time dilation when the Lorentz factor is replaced by the general relativistic factor \(\Gamma\). These predictions are falsifiable and provide a concrete experimental window into the emergent nature of time.

•Apr 16, 2026•0 citations
We investigate surprising consequences of the hypothesis that gravity and proper time obey the quantum superposition principle. We show that, for a massive body prepared in a superposition of two positions and post-selected in a suitable final state, the elapsed proper time in another region of space can assume an anomalous effective value lying outside the range allowed by classical general relativity. Remarkably, the effective elapsed proper time can even become negative, corresponding to an effective evolution backward in time. We also propose an experiment to observe an anomalous effective proper time associated with the internal degrees of freedom of a quantum particle in an interferometer under Earth's gravitational field. The proposed experiment is, in principle, feasible with current technology, and its realization could provide the first experimental evidence of an interplay between quantum mechanics and general relativity beyond the effects of the Newtonian potential in flat spacetime.
The paper asks whether coherent superpositions of gravitational time dilation, combined with post-selection, can produce an effective elapsed proper time outside the range of the individual branches. It considers both a probe near a mass in a spatial superposition and an internal atomic clock traversing two heights in Earth’s classical gravitational field.
Starting from weak-field evolution e−iHτ/ℏe^{-iH\tau/\hbar}e−iHτ/ℏ, it derives the conditional probe dynamics for initial path amplitudes α,β\alpha,\betaα,β and antisymmetric path post-selection. To first order, the evolution corresponds to τef=(βτB−ατA)/(β−α)\tau_{\mathrm{ef}}=(\beta\tau_B-\alpha\tau_A)/(\beta-\alpha)τef​=(βτB​−ατA​)/(β−α), the weak value of a branch-dependent proper-time operator. For positive real amplitudes, this lies outside [τA,τB][\tau_A,\tau_B][τA​,τB​] and can become negative. The approximate post-selection probability is ∣β−α∣2/2|\beta-\alpha|^2/2∣β−α∣2/2; averaging both output ports recovers the classical weighted proper time.
An experimental proposal reads out the conditional internal-clock phase through Ramsey interferometry. For an optical transition near 6×1014 Hz6\times10^{14}\,\mathrm{Hz}6×1014Hz, a 10 cm10\,\mathrm{cm}10cm average arm-height separation, 1 s1\,\mathrm{s}1s interrogation, and β=1/2+0.1\beta=1/\sqrt{2}+0.1β=1/2​+0.1, the predicted phase displacement relative to one branch is approximately 0.10.10.1 radians. This configuration uses a classical gravitational field, not a superposition of gravitational fields.
The effective-time description requires ΔE∣τef−τA∣/ℏ<1\Delta E|\tau_{\mathrm{ef}}-\tau_A|/\hbar<1ΔE∣τef​−τA​∣/ℏ<1, making the anomalous shift smaller than the clock’s single-system time uncertainty and requiring ensemble measurements. Environmental decoherence prevents the proposed macroscopic reversal interpretation. The gravitational-source-superposition scheme is acknowledged to be impractical, while maintaining atomic-clock precision within the proposed interferometer remains an experimental difficulty.
Current attempts to probe general relativistic effects in quantum mechanics focus on precision measurements of phase shifts in matter–wave interferometry. Yet, phase shifts can always be explained as arising because of an Aharonov–Bohm effect, where a particle in a flat space–time is subject to an effective potential. Here we propose a quantum effect that cannot be explained without the general relativistic notion of proper time. We consider interference of a 'clock'—a particle with evolving internal degrees of freedom—that will not only display a phase shift, but also reduce the visibility of the interference pattern. According to general relativity, proper time flows at different rates in different regions of space–time. Therefore, because of quantum complementarity, the visibility will drop to the extent to which the path information becomes available from reading out the proper time from the 'clock'. Such a gravitationally induced decoherence would provide the first test of the genuine general relativistic notion of proper time in quantum mechanics. In the theory of general relativity time flows at different rates depending on the space–time geometry. Here, a drop in the visibility of a quantum 'clock' interference in a gravitational potential is predicted, which cannot be explained without the general relativistic notion of time.
Quantum mechanics and general relativity have been extensively and independently confirmed in many experiments. However, the interplay of the two theories has never been tested: all experiments that measured the influence of gravity on quantum systems are consistent with non-relativistic, Newtonian gravity. On the other hand, all tests of general relativity can be described within the framework of classical physics. Here we discuss a quantum interference experiment with single photons that can probe quantum mechanics in curved space-time. We consider a single photon traveling in superposition along two paths in an interferometer, with each arm experiencing a different gravitational time dilation. If the difference in the time dilations is comparable with the photon's coherence time, the visibility of the quantum interference is predicted to drop, while for shorter time dilations the effect of gravity will result only in a relative phase shift between the two arms. We discuss what aspects of the interplay between quantum mechanics and general relativity are probed in such experiments and analyze the experimental feasibility.
A proper time observable for a quantum clock is introduced and it is found that the proper time read by one clock conditioned on another clock reading a different proper time obeys classical time dilation in accordance with special relativistic kinematical time dilation. Here, we extend this proposal to a weak gravitational field in order to investigate whether the weak equivalence principle holds for quantum matter. We find that for general quantum states the quantum time dilation in a weak gravitational field obeys a similar gravitational time dilation found in classical relativity. However, unlike the special relativistic case, the time dilation involves the external time (a background coordinate time at the observer on the Earth) as well as the proper times of two clocks. We also investigate a quantum time dilation effect induced by a clock in a superposition of wave packets localized in momentum space or in position space and propose the setup to observe the gravitational effect in the quantum interference effect in the time dilation.
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.
According to relativity, the reading of an ideal clock is interpreted as the elapsed proper time along its classical trajectory through spacetime. In contrast, quantum theory allows the association of many simultaneous trajectories with a single quantum clock, each weighted appropriately. Here, we investigate how the superposition principle affects the gravitational time dilation observed by a simple clock – a decaying two-level atom. Placing such an atom in a superposition of positions enables us to analyze a quantum contribution to a classical time dilation manifest in spontaneous emission. In particular, we show that the emission rate of an atom prepared in a coherent superposition of separated wave packets in a gravitational field is different from the emission rate of an atom in a classical mixture of these packets, which gives rise to a quantum gravitational time dilation effect. We demonstrate that this nonclassical effect also manifests in a fractional frequency shift of the internal energy of the atom that is within the resolution of current atomic clocks. In addition, we show the effect of spatial coherence on the atom's emission spectrum.
We propose that time is not a fundamental background but emerges from the quantum uncertainties of position, momentum, and energy. This is captured by the postulate Δτ=Δx Δpγ ΔE\Delta \tau = \frac{\Delta x \,\Delta p}{\gamma \,\Delta E}Δτ=γΔEΔxΔp​,where Δτ\Delta \tauΔτ is the proper time interval, Δx,Δp,ΔE\Delta x,\Delta p,\Delta EΔx,Δp,ΔE are the standard quantum uncertainties, and γ=1/1−v2/c2\gamma = 1/\sqrt{1-v^2/c^2}γ=1/1−v2/c2​ is the Lorentz factor associated with the average velocity vvv. Using the standard wave‑packet relation ΔE=vΔp\Delta E = v \Delta pΔE=vΔp, our equation reduces exactly to the special relativistic proper time Δτ=Δx/(γv)\Delta \tau = \Delta x/(\gamma v)Δτ=Δx/(γv), demonstrating consistency with all existing tests. However, for non‑classical quantum states where ΔE≠vΔp\Delta E \neq v \Delta pΔE=vΔp (e.g., a superposition of widely separated momenta), our equation predicts new measurable effects: (i) a significant modification of the decay length of unstable particles (muons), (ii) a dependence of clock rates on the spatial spread Δx\Delta xΔx even in flat spacetime, and (iii) a quantum correction to gravitational time dilation when the Lorentz factor is replaced by the general relativistic factor Γ\GammaΓ. These predictions are falsifiable and provide a concrete experimental window into the emergent nature of time.