Giorgio Mentasti’s research while affiliated with Imperial College London and other places

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Publications (8)


FIG. 1: Comparison of projected and existing constraints on
FIG. 3: Upper panel: constraints on the space of parameters (Λ, M) in the generalized interaction modified gravity model (E36). The lines define the lower bounds in the region of parameters (Λ, M) that can be ruled out by a CaF/Sr clock pair over a three-year observation time. Particular theories are highlighted: the free scalar, cubic Galileon, and quartic Galileon corresponding to each of the three regimes identified in Eq. (12), and also generalized ones that include DBI [62].
FIG. 4: Projected bounds from clocks on quintessence dark energy, over an observation time of 3 years. A CaF/Sr clock pair was used for the bottom plot.
FIG. 5: Constraints on the space of parameters (M, m) in the Dark Matter model defined in (23) after marginalizing over the unknown phase δ , for an observation time of T = 3 yr. Also plotted are constraints from NANOGrav [46] and Yb/Cs clocks [38, 44] which were drawn from [47], as well as Sr/H/Si clocks [43], and the MICROSCOPE satellite [22]. The best torsion balance curves [72] sit approximately one order of magnitude below the MICROSCOPE line and hence are not included in the figure. Planned atom interferometry experiments will also be sensitive to the higher end of this mass range (10 −19 eV ≲ m ≲ 10 −11 eV) within the next few years [73].
FIG. 6: Plot of ∆µ µ (= −d) vs month and year for each optical clock used in the analysis.

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Prospects for detecting new dark physics with the next generation of atomic clocks
  • Preprint
  • File available

April 2025

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25 Reads

Benjamin Elder

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Giorgio Mentasti

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[...]

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Andrew J. Tolley

Wide classes of new fundamental physics theories cause apparent variations in particle mass ratios in space and time. In theories that violate the weak equivalence principle (EP), those variations are not uniform across all particles and may be detected with atomic and molecular clock frequency comparisons. In this work we explore the potential to detect those variations with near-future clock comparisons. We begin by searching published clock data for variations in the electron-proton mass ratio. We then undertake a statistical analysis to model the noise in a variety of clock pairs that can be built in the near future according to the current state of the art, determining their sensitivity to various fundamental physics signals. Those signals are then connected to constraints on fundamental physics theories that lead directly or indirectly to an effective EP-violating, including those motivated by dark matter, dark energy, the vacuum energy problem, unification or other open questions of fundamental physics. This work results in projections for tight new bounds on fundamental physics that could be achieved with atomic and molecular clocks within the next few years. Our code for this work is packaged into a forecast tool that translates clock characteristics into bounds on fundamental physics.

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Terrestrial Very-Long-Baseline Atom Interferometry: summary of the second workshop

April 2025

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191 Reads

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2 Citations

EPJ Quantum Technology

This summary of the second Terrestrial Very-Long-Baseline Atom Interferometry (TVLBAI) Workshop provides a comprehensive overview of our meeting held in London in April 2024 (Second Terrestrial Very-Long-Baseline Atom Interferometry Workshop, Imperial College, April 2024), building on the initial discussions during the inaugural workshop held at CERN in March 2023 (First Terrestrial Very-Long-Baseline Atom Interferometry Workshop, CERN, March 2023). Like the summary of the first workshop (Abend et al. in AVS Quantum Sci. 6:024701, 2024), this document records a critical milestone for the international atom interferometry community. It documents our concerted efforts to evaluate progress, address emerging challenges, and refine strategic directions for future large-scale atom interferometry projects. Our commitment to collaboration is manifested by the integration of diverse expertise and the coordination of international resources, all aimed at advancing the frontiers of atom interferometry physics and technology, as set out in a Memorandum of Understanding signed by over 50 institutions (Memorandum of Understanding for the Terrestrial Very Long Baseline Atom Interferometer Study).


The Science of the Einstein Telescope

March 2025

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131 Reads

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1 Citation

Einstein Telescope (ET) is the European project for a gravitational-wave (GW) observatory of third-generation. In this paper we present a comprehensive discussion of its science objectives, providing state-of-the-art predictions for the capabilities of ET in both geometries currently under consideration, a single-site triangular configuration or two L-shaped detectors. We discuss the impact that ET will have on domains as broad and diverse as fundamental physics, cosmology, early Universe, astrophysics of compact objects, physics of matter in extreme conditions, and dynamics of stellar collapse. We discuss how the study of extreme astrophysical events will be enhanced by multi-messenger observations. We highlight the ET synergies with ground-based and space-borne GW observatories, including multi-band investigations of the same sources, improved parameter estimation, and complementary information on astrophysical or cosmological mechanisms obtained combining observations from different frequency bands. We present advancements in waveform modeling dedicated to third-generation observatories, along with open tools developed within the ET Collaboration for assessing the scientific potentials of different detector configurations. We finally discuss the data analysis challenges posed by third-generation observatories, which will enable access to large populations of sources and provide unprecedented precision.


Terrestrial Very-Long-Baseline Atom Interferometry: Summary of the Second Workshop

December 2024

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243 Reads

This summary of the second Terrestrial Very-Long-Baseline Atom Interferometry (TVLBAI) Workshop provides a comprehensive overview of our meeting held in London in April 2024, building on the initial discussions during the inaugural workshop held at CERN in March 2023. Like the summary of the first workshop, this document records a critical milestone for the international atom interferometry community. It documents our concerted efforts to evaluate progress, address emerging challenges, and refine strategic directions for future large-scale atom interferometry projects. Our commitment to collaboration is manifested by the integration of diverse expertise and the coordination of international resources, all aimed at advancing the frontiers of atom interferometry physics and technology, as set out in a Memorandum of Understanding signed by over 50 institutions.


Cosmic Shimmering: the Gravitational Wave Signal of Time-Resolved Cosmic Shear Observations

October 2024

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6 Reads

We introduce a novel approach for detecting gravitational waves through their influence on the shape of resolved astronomical objects. This method, complementary to pulsar timing arrays and astrometric techniques, explores the time-dependent distortions caused by gravitational waves on the shapes of celestial bodies, such as galaxies or any resolved extended object. By developing a formalism based on that adopted in the analysis of weak lensing effects, we derive the response functions for gravitational wave-induced distortions and compute their angular correlation functions. Our results highlight the sensitivity of these distortions to the lowest frequencies of the gravitational wave spectrum and demonstrate how they produce distinct angular correlation signatures, including null and polarisation-sensitive correlations. These findings pave the way for future high-resolution surveys to exploit this novel observable, potentially offering new insights into the stochastic gravitational wave background and cosmological models.


Figure 2. Freuquency dependence of the noise PSD˜NPSD˜ PSD˜N α O (f ) as defined in equations (B14) and (B15) in [2]. As discussed in the text, for LISA we have chosen a value for the parameters P = 15, A = 3, and L L = 2.5 × 10 6 km, while the PSD of Taiji is computed assuming P = 8, A = 3, and L T = 3 × 10 6 km. A uniform discretization of 300 frequency values between 10 −4 Hz and 10 −1 Hz is employed.
Figure 6. Mollweide projection of the template morphology for the galactic GW signal arising from unresolved binaries. The template is unit normalized and in celestial coordinates.
Figure 7. Time evolution of the response functioñ R G LL,AA (f, t) during one year, for two specific frequencies chosen as an example. Only the real part is shown, as the imaginary part is sub-dominant. The points are the numerical values used in our analysis (taken with a time interval of one day), while the solid line is the fitting function (C.1), with A = 0.185 in both cases.
Probing the galactic and extragalactic gravitational wave backgrounds with space-based interferometers

June 2024

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16 Reads

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12 Citations

We employ the formalism developed in [1] and [2] to study the prospect of detecting an anisotropic Stochastic Gravitational Wave Background (SGWB) with the Laser Interferometer Space Antenna (LISA) alone, and combined with the proposed space-based interferometer Taiji. Previous analyses have been performed in the frequency domain only. Here, we study the detectability of the individual coefficients of the expansion of the SGWB in spherical harmonics, by taking into account the specific motion of the satellites. This requires the use of time-dependent response functions, which we include in our analysis to obtain an optimal estimate of the anisotropic signal. We focus on two applications. Firstly, the reconstruction of the anisotropic galactic signal without assuming any prior knowledge of its spatial distribution. We find that both LISA and LISA with Taiji cannot put tight constraints on the harmonic coefficients for realistic models of the galactic SGWB. We then focus on the discrimination between a galactic signal of known morphology but unknown overall amplitude and an isotropic extragalactic SGWB component of astrophysical origin. In this case, we find that the two surveys can confirm, at a confidence level ≳ 3σ, the existence of both the galactic and extragalactic background if both have amplitudes as predicted in standard models. We also find that, in the LISA-only case, the analysis in the frequency domain (under the assumption of a time average of data taken homogeneously across the year) provides a nearly identical determination of the two amplitudes as compared to the optimal analysis.


Observing gravitational waves with solar system astrometry

May 2024

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20 Reads

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3 Citations

The subtle influence of gravitational waves on the apparent positioning of celestial bodies offers novel observational windows [1,2,3,4]. We calculate the expected astrometric signal induced by an isotropic Stochastic Gravitational Wave Background (SGWB) in the short distance limit. Our focus is on the resultant proper motion of Solar System objects, a signal on the same time scales addressed by Pulsar Timing Arrays (PTA). We derive the corresponding astrometric deflection patterns, finding that they manifest as distinctive dipole and quadrupole correlations or, in some cases, may not be present. Our analysis encompasses both Einsteinian and non-Einsteinian polarisations. We estimate the upper limits for the amplitude of SGWBs that could be obtained by tracking the proper motions of large numbers of solar system objects such as asteroids. We find that for SGWBs with negative spectral indices, such as that generated by Super Massive Black Hole Binaries (SMBHB), the constraints from these observations could rival those from PTAs. With the Gaia satellite and the Vera C. Rubin Observatory poised to track an extensive sample of asteroids — ranging from 𝒪(10⁵) to 𝒪(10⁶), we highlight the significant future potential for similar surveys to contribute to our understanding of the SGWB.


FIG. 1. Forecast errors induced by the intrinsic variance of the dominant isotropic component in the measurement of the multipolar coefficients δ GW lm , for each l ≤ 8. These coefficients, introduced in Eq. (1), quantify the amplitude of the corresponding multipole of the SGWB relative to the isotropic component Ω 0 . The shaded bands highlight the range of σ δ GW lm
Intrinsic Limits on the Detection of the Anisotropies of the Stochastic Gravitational Wave Background

November 2023

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15 Reads

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11 Citations

Physical Review Letters

For any given network of detectors, and for any given integration time, even in the idealized limit of negligible instrumental noise, the intrinsic time variation of the isotropic component of the stochastic gravitational wave background (SGWB) induces a limit on how accurately the anisotropies in the SGWB can be measured. We show here how this sample limit can be calculated and apply this to three separate configurations of ground-based detectors placed at existing and planned sites. Our results show that in the idealized, best-case scenario, individual multipoles of the anisotropies at ℓ≤8 can only be measured to ∼10−5–10−4 level over five years of observation as a fraction of the isotropic component. As the sensitivity improves as the square root of the observation time, this poses a very serious challenge for measuring the anisotropies of SGWB of cosmological origin, even in the case of idealized detectors with arbitrarily low instrumental noise.

Citations (4)


... Atom interferometers based on single-photon transitions (SPTs) [7][8][9] have caught attention for potential applications in terrestrial large-baseline setups [10][11][12] for gravitationalwave [13,14] and dark-matter detectors [15,16], as well as in other practical scenarios beyond fundamental physics [1]. In ground-based experiments, the laser frequency must be chirped to remain on resonance with the atomic transition [17][18][19]. ...

Reference:

Finite-Speed-of-Light Effects in Atom Interferometry: Diffraction Mechanisms and Resonance Conditions
Terrestrial Very-Long-Baseline Atom Interferometry: summary of the second workshop

EPJ Quantum Technology

... One could also think of recursive schemes by which we first fix ℓ = 0, 1 via the MCMC before fitting for ℓ = 2 only. It should be noted, however, that the correlations between the monopole and anisotropies are also partly driven by LISA's complex and non-compact sky response functions [38] (see also [69,70]). Accounting for this factor introduces an additional layer of complexity to the analysis. At this stage, we defer a deeper investigation of these issues to future work and highlight that for the model-dependent fit such complications do not arise. ...

Probing the galactic and extragalactic gravitational wave backgrounds with space-based interferometers

... It is worthwhile to also explore alternative probes that could complement the PTA observations in the nHz regime. One such promising probe is astrometry -using the precise measurements of the positions of a very large number of distant sources to measure the effects of gravitational waves [17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. GW present between the Earth and the source induce deflections in the observed positions of these sources (hereafter we lump all such sources under the umbrella term 'stars'). ...

Observing gravitational waves with solar system astrometry

... The former effect is generally dominant and the correlator, normalized by the amplitude of ζ and by the fractional energy in sourced gravitational waves at interferometer frequencies, turned out to be of the order of 10 −4 ÷10 −2 . The observability of this correlation, influenced by the intrinsic variance of the isotropic component and instrumental noise [27,28], depends not only on the overall gravitational wave energy density, but also on the amplitude of anisotropies in the gravitational wave spectra. Studies on preheating at the end of inflation and on baryogenesis suggest that these anisotropies may be large [29,30]. ...

Intrinsic Limits on the Detection of the Anisotropies of the Stochastic Gravitational Wave Background

Physical Review Letters