A. Saro’s research while affiliated with University of Trieste and other places

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Publications (206)


Figure 1 (left) shows ΛCDM constraints in the Ω m -σ 8 plane as obtained by SPT clusters, DES 3 × 2pt, and our joint analysis SPT clusters þ DES 3 × 2pt. The constraints on a selection of parameters are presented in Table I. The joint constraints lie at the intersection of the two individual probes. The degeneracy direction mostly follows the degeneracy of the 3 × 2pt result; the parameter combination that is constrained with the smallest absolute uncertainty is σ 8 ðΩ m =0.3Þ 0.494 , which is essentially S 8 . The ratio of the areas of the 95% credible region in Ω m -σ 8 space for SPT clusters, DES 3 × 2pt, and the joint analysis is 3.3∶2.1∶1. While the two probes cannot individually constrain the Hubble constant, the joint analysis breaks some of the parameter degeneracies and we recover h ¼ 0.73 AE 0.07 (see also Fig. 6 in the Appendix B). However, this result is not strong enough to inform the Hubble tension. In the Ω m -σ 8 plane shown in Fig. 1, the 95% credible region of the SPT cluster þ DES 3 × 2pt analysis is 15% larger than for Planck 2018 TT; TE; EE þ lowE [58]. We quantify the two-parameter difference with a PTE of 0.22 (1.2σ). Our measurement S 8 ¼ 0.796 AE 0.013 differs from the Planck measurement S 8 ¼ 0.831 AE 0.017 at 1.6σ. We
FIG. 1. Constraints on Ω m and σ 8 (68% and 95% credibility) in ΛCDM with massive neutrinos. The two panels show the same parameter ranges. Dashed lines show lines of constant S 8 ≡ σ 8 ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi Ω m =0.3 p . Left: the individual lensing-informed SPT cluster abundance and DES 3 × 2pt results, along with their combination. We also show the constraints from Planck TT; TE; EE þ lowE primary CMB anisotropies and the combination with our joint analysis. Right: comparison of our SPT clusters þ DES 3 × 2pt results with a selection of external single-probe and multiprobe analyses.
Multiprobe cosmology from the abundance of SPT clusters and DES galaxy clustering and weak lensing
  • Article
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March 2025

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6 Reads

Physical Review D

S. Bocquet

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E. Krause

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H. Zohren

Cosmic shear, galaxy clustering, and the abundance of massive halos each probe the large-scale structure of the Universe in complementary ways. We present cosmological constraints from the joint analysis of the three probes, building on the latest analyses of the lensing-informed abundance of clusters identified by the South Pole Telescope (SPT) and of the auto- and cross-correlation of galaxy position and weak lensing measurements ( 3 × 2 pt ) in the Dark Energy Survey (DES). We consider the cosmological correlation between the different tracers and we account for the systematic uncertainties that are shared between the large-scale lensing correlation functions and the small-scale lensing-based cluster mass calibration. Marginalized over the remaining Λ cold dark matter ( Λ CDM ) parameters (including the sum of neutrino masses) and 52 astrophysical modeling parameters, we measure Ω m = 0.300 ± 0.017 and σ 8 = 0.797 ± 0.026 . Compared to constraints from primary cosmic microwave background (CMB) anisotropies, our constraints are only 15% wider with a probability to exceed of 0.22 ( 1.2 σ ) for the two-parameter difference. We further obtain S 8 ≡ σ 8 ( Ω m / 0.3 ) 0.5 = 0.796 ± 0.013 which is lower than the measurement at the 1.6 σ level. The combined SPT cluster, DES 3 × 2 pt , and datasets mildly prefer a nonzero positive neutrino mass, with a 95% upper limit ∑ m ν < 0.25 eV on the sum of neutrino masses. Assuming a w CDM model, we constrain the dark energy equation of state parameter w = − 1.1 5 − 0.17 + 0.23 and when combining with primary CMB anisotropies, we recover w = − 1.2 0 − 0.09 + 0.15 , a 1.7 σ difference with a cosmological constant. The precision of our results highlights the benefits of multiwavelength multiprobe cosmology and our analysis paves the way for upcoming joint analyses of next-generation datasets. Published by the American Physical Society 2025

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Selection Function of Clusters in Dark Energy Survey Year 3 Data from Cross-Matching with South Pole Telescope Detections

February 2025

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1 Read

Galaxy clusters selected based on overdensities of galaxies in photometric surveys provide the largest cluster samples. Yet modeling the selection function of such samples is complicated by non-cluster members projected along the line of sight (projection effects) and the potential detection of unvirialized objects (contamination). We empirically constrain the magnitude of these effects by cross-matching galaxy clusters selected in the Dark Energy survey data with the \rdmpr\, algorithm with significant detections in three South Pole Telescope surveys (SZ, pol-ECS, pol-500d). For matched clusters, we augment the \rdmpr\,catalog by the SPT detection significance. For unmatched objects we use the SPT detection threshold as an upper limit on the SZe signature. Using a Bayesian population model applied to the collected multi-wavelength data, we explore various physically motivated models to describe the relationship between observed richness and halo mass. Our analysis reveals the limitations of a simple lognormal scatter model in describing the data. We rule out significant contamination by unvirialized objects at the high-richness end of the sample. While dedicated simulations offer a well-fitting calibration of projection effects, our findings suggest the presence of redshift-dependent trends that these simulations may not have captured. Our findings highlight that modeling the selection function of optically detected clusters remains a complicated challenge, requiring a combination of simulation and data-driven approaches.


Euclid preparation. LXVI. Impact of line-of-sight projections on the covariance between galaxy cluster multi-wavelength observable properties: insights from hydrodynamic simulations

January 2025

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5 Reads

Astronomy and Astrophysics

Cluster cosmology can benefit from combining multi-wavelength studies. In turn, these studies benefit from a characterisation of the correlation coefficients among different mass-observable relations. In this work, we aim to provide information on the scatter, skewness, and covariance of various mass-observable relations in galaxy clusters in cosmological hydrodynamic simulations. This information will help future analyses improve the general approach to accretion histories and projection effects, as well as to model mass-observable relations for cosmology studies. We identified galaxy clusters in Magneticum Box2b simulations with masses of M_ 200c M _⊙ at redshifts of z=0.24 and z=0.90. Our analysis included properties such as richness, stellar mass, lensing mass, and concentration. Additionally, we investigated complementary multi-wavelength data, including X-ray luminosity, integrated Compton-y parameter, gas mass, and temperature. We then examined the impact of projection effects on mass-observable residuals and correlations. We find that at intermediate redshift (z=0.24), projection effects have the greatest impact of lensing concentration, richness, and gas mass in terms of the scatter and skewness of the log-residuals of scaling relations. The contribution of projection effects can be significant enough to boost a spurious hot- versus cold-baryon correlations and consequently hide underlying correlations due to halo accretion histories. At high redshift (z=0.9), the richness has a much lower scatter (of log-residuals), while the quantity that is most impacted by projection effects is the lensing mass. The lensing concentration reconstruction, in particular, is affected by deviations of the reduced-shear profile shape from that derived using a Navarro-Frenk-White (NFW) profile; the amount of interlopers in the line of sight, on the other hand, is not as important.


Multiprobe Cosmology from the Abundance of SPT Clusters and DES Galaxy Clustering and Weak Lensing

December 2024

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27 Reads

Cosmic shear, galaxy clustering, and the abundance of massive halos each probe the large-scale structure of the universe in complementary ways. We present cosmological constraints from the joint analysis of the three probes, building on the latest analyses of the lensing-informed abundance of clusters identified by the South Pole Telescope (SPT) and of the auto- and cross-correlation of galaxy position and weak lensing measurements (3×\times2pt) in the Dark Energy Survey (DES). We consider the cosmological correlation between the different tracers and we account for the systematic uncertainties that are shared between the large-scale lensing correlation functions and the small-scale lensing-based cluster mass calibration. Marginalized over the remaining Λ\LambdaCDM parameters (including the sum of neutrino masses) and 52 astrophysical modeling parameters, we measure Ωm=0.300±0.017\Omega_\mathrm{m}=0.300\pm0.017 and σ8=0.797±0.026\sigma_8=0.797\pm0.026. Compared to constraints from Planck primary CMB anisotropies, our constraints are only 15% wider with a probability to exceed of 0.22 (1.2σ1.2\sigma) for the two-parameter difference. We further obtain S8σ8(Ωm/0.3)0.5=0.796±0.013S_8\equiv\sigma_8(\Omega_\mathrm{m}/0.3)^{0.5}=0.796\pm0.013 which is lower than the Planck measurement at the 1.6σ1.6\sigma level. The combined SPT cluster, DES 3×\times2pt, and Planck datasets mildly prefer a non-zero positive neutrino mass, with a 95% upper limit mν<0.25 eV\sum m_\nu<0.25~\mathrm{eV} on the sum of neutrino masses. Assuming a wCDM model, we constrain the dark energy equation of state parameter w=1.150.17+0.23w=-1.15^{+0.23}_{-0.17} and when combining with Planck primary CMB anisotropies, we recover w=1.200.09+0.15w=-1.20^{+0.15}_{-0.09}, a 1.7σ1.7\sigma difference with a cosmological constant. The precision of our results highlights the benefits of multiwavelength multiprobe cosmology.


Euclid preparation: TBD. The impact of line-of-sight projections on the covariance between galaxy cluster multi-wavelength observable properties -- insights from hydrodynamic simulations

November 2024

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9 Reads

Cluster cosmology can benefit from combining multi-wavelength studies, which can benefit from characterising the correlation coefficients between different mass-observable relations. In this work, we aim to provide information on the scatter, the skewness, and the covariance of various mass-observable relations in galaxy clusters in cosmological hydrodynamic simulations. This information will help future analyses to better tackle accretion histories and projection effects and model mass observable relations for cosmology studies.We identify galaxy clusters in Magneticum Box2b simulations with mass M200c>1014MM_{\rm 200c}>10^{14} {\rm M}_\odot at redshift z=0.24 and z=0.90. Our analysis includes \Euclid-derived properties such as richness, stellar mass, lensing mass, and concentration. Additionally, we investigate complementary multi-wavelength data, including X-ray luminosity, integrated Compton-y parameter, gas mass, and temperature. The impact of projection effects on mass-observable residuals and correlations is then examined. At intermediate redshift (z=0.24), projection effects impact lensing concentration, richness, and gas mass the most in terms of scatter and skewness of log-residuals of scaling relations. The contribution of projection effects can be significant enough to boost a spurious hot- vs. cold-baryons correlation and consequently hide underlying correlations due to halo accretion histories. At high redshift (z=0.9), the richness has a much lower scatter (of log-residuals), and the quantity that is most impacted by projection effects is the lensing mass. Lensing concentration reconstruction, in particular, is affected by deviations of the reduced-shear profile shape from the one derived by an NFW profile rather than interlopers in the line of sight.




Euclid preparation. L. Calibration of the halo linear bias in Lambda(u)CDM cosmologies

September 2024

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14 Reads

Astronomy and Astrophysics

The mission, designed to map the geometry of the dark Universe, presents an unprecedented opportunity for advancing our understanding of the cosmos through its photometric galaxy cluster survey. Central to this endeavor is the accurate calibration of the mass- and redshift-dependent halo bias (HB), which is the focus of this paper. Our aim is to enhance the precision of HB predictions, which is crucial for deriving cosmological constraints from the clustering of galaxy clusters. Our study is based on the peak-background split (PBS) model linked to the halo mass function (HMF), and it extends it with a parametric correction to precisely align with results from an extended set of N-body simulations carried out with the code. Employing simulations with fixed and paired initial conditions, we meticulously analyzed the matter-halo cross-spectrum and modeled its covariance using a large number of mock catalogs generated with Lagrangian perturbation theory simulations with the code. This ensures a comprehensive understanding of the uncertainties in our HB calibration. Our findings indicate that the calibrated HB model is remarkably resilient against changes in cosmological parameters, including those involving massive neutrinos. The robustness and adaptability of our calibrated HB model provide an important contribution to the cosmological exploitation of the cluster surveys to be provided by the mission. This study highlights the necessity of continuously refining the calibration of cosmological tools such as the HB to match the advancing quality of observational data. As we project the impact of our calibrated model on cosmological constraints, we find that given the sensitivity of the survey, a miscalibration of the HB could introduce biases in cluster cosmology analysis. Our work fills this critical gap, ensuring the HB calibration matches the expected precision of the survey.


Euclid preparation. L. Calibration of the linear halo bias in Λ(ν)\Lambda(\nu)CDM cosmologies

September 2024

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7 Reads

The Euclid mission, designed to map the geometry of the dark Universe, presents an unprecedented opportunity for advancing our understanding of the cosmos through its photometric galaxy cluster survey. This paper focuses on enhancing the precision of halo bias (HB) predictions, which is crucial for deriving cosmological constraints from the clustering of galaxy clusters. Our study is based on the peak-background split (PBS) model linked to the halo mass function (HMF); it extends with a parametric correction to precisely align with results from an extended set of N-body simulations carried out with the OpenGADGET3 code. Employing simulations with fixed and paired initial conditions, we meticulously analyze the matter-halo cross-spectrum and model its covariance using a large number of mock catalogs generated with Lagrangian Perturbation Theory simulations with the PINOCCHIO code. This ensures a comprehensive understanding of the uncertainties in our HB calibration. Our findings indicate that the calibrated HB model is remarkably resilient against changes in cosmological parameters including those involving massive neutrinos. The robustness and adaptability of our calibrated HB model provide an important contribution to the cosmological exploitation of the cluster surveys to be provided by the Euclid mission. This study highlights the necessity of continuously refining the calibration of cosmological tools like the HB to match the advancing quality of observational data. As we project the impact of our model on cosmological constraints, we find that, given the sensitivity of the Euclid survey, a miscalibration of the HB could introduce biases in cluster cosmology analyses. Our work fills this critical gap, ensuring the HB calibration matches the expected precision of the Euclid survey. The implementation of our model is publicly available in https://github.com/TiagoBsCastro/CCToolkit.


Inferring intrahalo light from stellar kinematics. A deep learning approach

July 2024

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8 Reads

Astronomy and Astrophysics

Context. In the context of structure formation, disentangling the central galaxy stellar population from the stellar intrahalo light can help us shed light on the formation history of the halo as a whole, as the properties of the stellar components are expected to retain traces of the formation history. Many approaches are adopted to assess the task, depending on different physical assumptions (e.g. the light profile, chemical composition, and kinematical differences) and depending on whether the full six-dimensional phase-space information is known (much like in simulations) or whether one analyses projected quantities (i.e. observations). Aims. This paper paves the way for a new approach to bridge the gap between observational and simulation methods. We propose the use of projected kinematical information from stars in simulations in combination with deep learning to create a robust method for identifying intrahalo light in observational data to enhance understanding and consistency in studying the process of galaxy formation. Methods. Using deep learning techniques, particularly a convolutional neural network called U-Net, we developed a methodology for predicting these contributions in simulated galaxy cluster images. We created a sample of mock images from hydrodynamical simulations (including masking of the interlopers) to train, validate and test the network. Reinforced training (Attention U-Net) was used to improve the first results, as the innermost central regions of the mock images consistently overestimate the stellar intrahalo contribution. Results. Our work shows that adequate training over a representative sample of mock images can lead to good predictions of the intrahalo light distribution. The model is mildly dependent on the training size and its predictions are less accurate when applied to mock images from different simulations. However, the main features (spatial scales and gradients of the stellar fractions) are recovered for all tests. While the method presented here should be considered as a proof of concept, future work (e.g. generating more realistic mock observations) is required to enable the application of the proposed model to observational data.


Citations (51)


... As was done in previous SPT publications, A SZ is rescaled as γ × A SZ for each individual SPT field to account for the changes in noise levels between SPT surveys. We calculate γ by following Bocquet et al. (2024) and fit the scaling parameters of Equation 9 to the SPT-Deep cluster abundances assuming a fixed A SZ value following Bleem et al. (2015). For SPT-Deep we find a value of γ = 4.97 ± 0.24. ...

Reference:

The SPT-Deep Cluster Catalog: Sunyaev-Zel'dovich Selected Clusters from Combined SPT-3G and SPTpol Measurements over 100 Square Degrees
SPT clusters with DES and HST weak lensing. I. Cluster lensing and Bayesian population modeling of multiwavelength cluster datasets
  • Citing Article
  • October 2024

Physical Review D

... novae, baryon acoustic oscillations, cosmic shear, galaxy clustering, or CMB anisotropies. However, other cluster analyses did not support previous results (Lesci et al. 2022;Bocquet et al. 2024;Ghirardini et al. 2024). More than signs of physics beyond the ΛCDM model, the tension might be due to unaccounted for systematic uncertainties related to incomplete or impure samples or biased mass calibration. ...

SPT clusters with DES and HST weak lensing. II. Cosmological constraints from the abundance of massive halos
  • Citing Article
  • October 2024

Physical Review D

... where f rand and f obs are the richness distributions along random and candidate lines of sight (Klein et al. 2019;Klein et al. 2024b). Estimation of this statistic using a cluster sample drawn from only 100 square degrees is noisy. ...

SPT-SZ MCMF: an extension of the SPT-SZ catalogue over the DES region
  • Citing Article
  • June 2024

Monthly Notices of the Royal Astronomical Society

... The noise levels of the SPTpol 500d field are comparable to those of the SPTpol 100d field, with a rough noise level of 5.2 µK-arcmin at 150 GHz and 11.3 µK-arcmin at 95 GHz. Details of the SPTpol 500d map construction can be found in Bleem et al. (2024), hereafter B24. ...

Galaxy Clusters Discovered via the Thermal Sunyaev-Zel’dovich Effect in the 500-square-degree SPTpol Survey
  • Citing Article
  • February 2024

The Open Journal of Astrophysics

... For any two models M1 and M2 we use ∆DIC = DIC M1 − DIC M2 to quantify the evidence of the dataset favoring a model. Popularly, −2 ≤ ∆DIC ≤ 0 is considered as weak preference of M1 over M2, −6 ≤ ∆DIC < −2 indicates that that data moderately favors M1 over M2, −10 ≤ ∆DIC < −6 is usually taken as a strong evidence that M1 outperforms M2, and ∆DIC < −10 is considered as a very strong evidence for the preference of M1 over M2 [82,[98][99][100]. ...

Euclid preparation. XXXV. Covariance model validation for the two-point correlation function of galaxy clusters

Astronomy and Astrophysics

... To maximize the precision that can be reached to infer cosmological parameters, a common approach in the literature is to use many probes simultaneously in the same analysis. For instance, SNe Ia, CMB, BAOs, Weak Gravitational Lensing, Large-Scale Structure, Cosmic Chronometers (CC), GWs, GRBs, HII Galaxies, Starburst Galaxies, QSO, AGNs, Strong Lensing, galaxy clusters, and Multi-Messenger Probes (Freedman, 2021;Bora and Holanda, 2023;Brieden et al., 2023;Bucko et al., 2023;Cruz et al., 2023;Du et al., 2023a;Gupta, 2023b;Kumar, 2023;Lu and Gong, 2023;Sakr, 2023;Smith et al., 2023;Rogers and Poulin, 2023;Yang et al., 2023;Zhang et al., 2023c;Camilleri et al., 2024;Chatterjee et al., 2024;Cortês and Liddle, 2024;Fumagalli et al., 2024;Liu et al., 2024b;Peng and Piao, 2024;Roy, 2024;Sudharani et al., 2024;Taule et al., 2024). ...

Cosmological constraints from the abundance, weak lensing, and clustering of galaxy clusters: Application to the SDSS

Astronomy and Astrophysics

... The redshift independence of the tSZ signal also provides a means to detect clusters at high redshifts (z > 1), which represents a critical era in astrophysics where significant suppression of star formation occurs in cluster galaxy populations (Elbaz et al. 2007;Alberts et al. 2016;Darvish et al. 2016;Nantais et al. 2017). The low-redshift cluster environment is dominated by quiescent galaxies whose star formation appears to be quenched by a combination of environmental processes, including mergers and ram-pressure stripping of their hot halos and cool gas disks (Bahé & McCarthy 2014;Pintos-Castro et al. 2019;Kim et al. 2023). However, the specific star formation rate of massive galaxies, including the central brightest cluster galaxies, has been shown to increase by ∼ 2 orders of magnitudes between z ∼ 0 to z ∼ 1.5 (Tran et al. 2010;Schreiber et al. 2015;Bonaventura et al. 2017). ...

A Gradual Decline of Star Formation since Cluster Infall: New Kinematic Insights into Environmental Quenching at 0.3 < z < 1.1

The Astrophysical Journal

... Changes in the shape of the SHMF could potentially impact α. Recently Ragagnin et al. (2023) investigated the cosmological dependence of the satellite galaxy abundance in the Magneticum hydrodynamical simulations. They find that the normalization of the satellite abundance function, i.e. ...

Dependency of high-mass satellite galaxy abundance on cosmology in Magneticum simulations

Astronomy and Astrophysics

... There is some evidence for radio AGN driving environmental quenching in z ∼ 1 clusters (L. Shen et al. 2019), and a proto-ICM has been detected in the Spiderweb protocluster at z = 2.156 (the highest redshift detection of hot intracluster gas to date; L. Di Mascolo et al. 2023). While the UMG in MAG-0959 hosts an X-ray AGN (with luminosity L 2-10 keV = (6.4 ...

Forming intracluster gas in a galaxy protocluster at a redshift of 2.16

Nature

... Efforts are being made on the fronts of both observations and simulations to collect large amounts of high-quality data and all the mock data required to analyze them. In -1 -JCAP01(2025)082 the former front, surveys are observing deeper into the Universe, with better image quality and photometric accuracy -see DESI [5], J-PAS [6], examples of wider surveys, such as Euclid [7,8] and Roman [9], or even going deeper, e.g. JWST [10]. ...

Euclid preparation: XXIV. Calibration of the halo mass function in Λ( ν )CDM cosmologies

Astronomy and Astrophysics