Luca Graziani

Dr. Luca Graziani

La Sapienza Università di Roma
+3

Research Focus & Metrics

Academic Career Length

17Years (2010-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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31 August 2020 in General Relativity and Gravitation
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EBEnrico Barausse
Enrico Barausse
EBEmanuele Berti
Emanuele Berti
THThomas Hertog
Thomas Hertog
SHScott A. Hughes
Scott A. Hughes
Philippe JetzerPhilippe Jetzer
Philippe Jetzer
MZM. Zumalacarregui
M. Zumalacarregui

1 March 2022 in The Astrophysical Journal
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STSandro Tacchella
Sandro Tacchella
SFSteven L. Finkelstein
Steven L. Finkelstein
MBMicaela Bagley
Micaela Bagley
MDMark Dickinson
Mark Dickinson
HFHenry C. Ferguson
Henry C. Ferguson
LYL. Y. Aaron Yung
L. Y. Aaron Yung
We present a detailed stellar population analysis of 11 bright (H < 26.6) galaxies at z = 9–11 (three spectroscopically confirmed) to constrain the chemical enrichment and growth of stellar mass of early galaxies. We use the flexible Bayesian spectral energy distribution (SED) fitting code Prospector with a range of star formation histories (SFHs), a flexible dust attenuation law, and a self-consistent model of emission lines. This approach allows us to assess how different priors affect our results and how well we can break degeneracies between dust attenuation, stellar ages, metallicity, and emission lines using data that probe only the rest-frame ultraviolet (UV) to optical wavelengths. We measure a median observed UV spectral slope β = − 1.87 − 0.43 + 0.35 for relatively massive star-forming galaxies ( 9 < log ( M ⋆ / M ⊙ ) < 10 ), consistent with no change from z = 4 to z = 9–10 at these stellar masses, implying rapid enrichment. Our SED-fitting results are consistent with a star-forming main sequence with sublinear slope (0.7 ± 0.2) and specific star formation rates of 3–10 Gyr−1. However, the stellar ages and SFHs are less well constrained. Using different SFH priors, we cannot distinguish between median mass-weighted ages of ∼ 50–150 Myr, which corresponds to 50% formation redshifts of z 50 ∼ 10–12 at z ∼ 9 and is of the order of the dynamical timescales of these systems. Importantly, models with different SFH priors are able to fit the data equally well. We conclude that the current observational data cannot tightly constrain the mass-buildup timescales of these z = 9–11 galaxies, with our results consistent with SFHs implying both a shallow and steep increase in the cosmic SFR density with time at z > 10.

1 March 2026 in Journal of Cosmology and Astroparticle Physics
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AAAdrian Abac
Adrian Abac
RARaul Abramo
Raul Abramo
SASimone Albanesi
Simone Albanesi
AAAngelica Albertini
Angelica Albertini
AAAlessandro Agapito
Alessandro Agapito
AZAndreas Zmija
Andreas Zmija
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.

22 September 2021 in Nature
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YFY. Fudamoto
Y. Fudamoto
POP. A. Oesch
P. A. Oesch
SSS. Schouws
S. Schouws
MSM. Stefanon
M. Stefanon
RSR. Smit
R. Smit
CWC. White
C. White

3 March 2022 in Monthly Notices of the Royal Astronomical Society
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PDP Dayal
P Dayal
AFA Ferrara
A Ferrara
LSL Sommovigo
L Sommovigo
RBR Bouwens
R Bouwens
POP A Oesch
P A Oesch
RER Endsley
R Endsley
We include a fully coupled treatment of metal and dust enrichment into the Delphi semi-analytic model of galaxy formation to explain the dust content of 13 Lyman break galaxies (LBGs) detected by the Atacama Large millimetre Array (ALMA) REBELS Large Program at z ≃ 7. We find that the galaxy dust mass, Md, is regulated by the combination of Type II supernova dust production, astration, shock destruction, and ejection in outflows; grain growth (with a standard time-scale τ0 = 30 Myr) plays a negligible role. The model predicts a dust-to-stellar mass ratio of |$\sim 0.07\!-\!0.1{{\ \rm per\ cent}}$| and a UV-to-total star formation rate relation such that log(ψUV) = −0.05 [log(ψ)]2 + 0.86 log(ψ) − 0.05 (implying that 55–80 per cent of the star formation is obscured) for REBELS galaxies with stellar mass |$M_* = 10^{9}\!-\!10^{10} \rm M_\odot$|⁠. This relation reconciles the intrinsic UV luminosity of LBGs with their observed luminosity function at z = 7. However, 2 out of the 13 systems show dust-to-stellar mass ratios (⁠|$\sim 0.94\!-\!1.1{{\ \rm per\ cent}}$|⁠) that are up to 18 times larger than expected from the fiducial relation. Due to the physical coupling between dust and metal enrichment, even decreasing τ0 to very low values (0.3 Myr) only increases the dust-to-stellar mass ratio by a factor of ∼2. Given that grain growth is not a viable explanation for such high observed ratios of the dust-to-stellar mass, we propose alternative solutions.

28 June 2022 in Monthly Notices of the Royal Astronomical Society
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HIHanae Inami
Hanae Inami
HAHiddo S B Algera
Hiddo S B Algera
SSSander Schouws
Sander Schouws
LSLaura Sommovigo
Laura Sommovigo
RBRychard Bouwens
Rychard Bouwens
PWPaul van der Werf
Paul van der Werf
We report 18 dust continuum detections (≥3.3σ) at ∼88 and 158 |$\mu{\rm m}$| out of 49 ultraviolet (UV)-bright galaxies (MUV < −21.3 mag) at |$z$| > 6.5, observed by the Cycle-7 Atacama Large Millimeter/submillimeter Array (ALMA) Large Program, Reionization-Era Bright Emission Line Survey (REBELS) and its pilot programs. This has more than tripled the number of dust continuum detections known at |$z$| > 6.5. Out of these 18 detections, 12 are reported for the first time as part of REBELS. In addition, 15 of the dust continuum detected galaxies also show a [C ii]|$_{\rm 158\,{\rm \mu m}}$| emission line, providing us with accurate redshifts. We anticipate more line emission detections from six targets (including three continuum detected targets) where observations are still ongoing. We estimate that all of the sources have an infrared (IR) luminosity (LIR) in a range of |$3\!-\!8 \times 10^{11}\, {\rm L_\odot }$|⁠, except for one with |$L_{\rm IR} = 1.5^{+0.8}_{-0.5} \times 10^{12}\, \, {\rm L_{\odot }}$|⁠. Their fraction of obscured star formation is significant at |${\gtrsim} 50{{\ \rm per\ cent}}$|⁠, despite being UV-selected galaxies. Some of the dust continuum detected galaxies show spatial offsets (∼0.5–1.5 arcsec) between the rest-UV and far-IR emission peaks. These separations could imply spatially decoupled phases of obscured and unobscured star formation, but a higher spatial resolution observation is required to confirm this. REBELS offers the best available statistical constraints on obscured star formation in UV-luminous galaxies at |$z$| > 6.5.