J/A+A/686/A68       Temperature profiles for galaxy clusters   (Rossetti+, 2024)

CHEX-MATE: Robust reconstruction of temperature profiles in galaxy clusters with XMM-Newton. Rossetti M., Eckert D., Gastaldello F., Rasia E., Pratt G.W., Ettori S., Molendi S., Arnaud M., Balboni M., Bartalucci I., Batalha R.M., Borgani S., Bourdin H., De Grandi S., De Luca F., De Petris M., Forman W., Gaspari M., Ghizzardi S., Iqbal A., Kay S., Lovisari L., Maughan B.J., Mazzotta P., Pointecouteau E., Riva G., Sayers J., Sereno M. <Astron. Astrophys. 686, A68 (2024)> =2024A&A...686A..68R 2024A&A...686A..68R (SIMBAD/NED BibCode)
ADC_Keywords: Clusters, galaxy ; X-ray sources ; Effective temperatures Keywords: galaxies: clusters: general - galaxies: clusters: intracluster medium Abstract: The "Cluster HEritage project with XMM-Newton: Mass Assembly and Thermodynamics at the Endpoint of structure formation" (CHEX-MATE) is a multi-year Heritage program, to obtain homogeneous XMM-Newton observations of a representative sample of 118 galaxy clusters. The observations are tuned to reconstruct the distribution of the main thermodynamic quantities of the ICM up to R500 and to obtain individual mass measurements, via the hydrostatic-equilibrium equation, with a precision of 15-20%. Temperature profiles are a necessary ingredient for the scientific goals of the project and it is thus crucial to derive the best possible temperature measurements from our data. This is why we have built a new pipeline for spectral extraction and analysis of XMM-Newton data, based on a new physically motivated background model and on a Bayesian approach with Markov Chain Monte Carlo (MCMC) methods, that we present in this paper for the first time. We applied this new method to a subset of 30 galaxy clusters representative of the CHEX-MATE sample and show that we can obtain reliable temperature measurements up to regions where the source intensity is as low as 20% of the background, keeping systematic errors below 10%. We compare the median profile of our sample and the best fit slope at large radii with literature results and we find a good agreement with other measurements based on XMM-Newton data. Conversely, when we exclude from our analysis the most contaminated regions, where the source intensity is below 20 of the background, we find significantly flatter profiles, in agreement with predictions from numerical simulations and independent measurements with a combination of Sunyaev-Zeldovich and X-ray imaging data. Description: Table containing the temperature profiles used in the paper. The first column shows the name of the cluster, while the second and third ones show the sky extension R500 in arcminutes and the mean temperature, estimated in the annulus between 0.15 and 0.75R500. Columns 4 and 5 report the coordinates of the center used for spectral extraction (the peak in Bartalucci et al., 2023A&A...674A.179B 2023A&A...674A.179B), while columns 6 and 7 show the center of the radial bin R and the width dR (annulus included between R-dR and R+dR). Columns 8, 9, and 10 report the best fit temperature and its errors (downward and upward) obtained with our baseline MCMC procedure, while column 11 shows the SOU/BKG ratio in the radial bin. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tablec1.dat 87 355 Temperature profiles for the clusters of our sample -------------------------------------------------------------------------------- See also: J/A+A/594/A27 : Planck Sunyaev-Zeldovich sources (PSZ2) (Planck+, 2016) Byte-by-byte Description of file: tablec1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 17 A17 --- Name Cluster Name 19- 23 F5.2 arcmin R500 Cluster size 25- 29 F5.2 keV Tmean Mean cluster temperature 31- 38 F8.4 deg RAdeg Center right ascension (J2000) 40- 47 F8.4 deg DEdeg Center declination (J2000) 49- 55 F7.4 arcmin Radius Distance of the radial bin from the center 57- 62 F6.4 arcmin Width Width of the radial bin 64- 68 F5.2 keV T Best-fit temperature in the radial bin 70- 73 F4.2 keV e_T Downward error on temperature 75- 78 F4.2 keV E_T Upward error on temperature 80- 87 F8.2 --- SOU/BKG SOU/BKG in the radial bin (1) -------------------------------------------------------------------------------- Note (1): Even a large error on the background model will not affect significantly the best fit parameters in a region where the source outshines the background, such as in the central regions of galaxy clusters, conversely, in the external regions where the source intensity is comparable to, or often even smaller than, the background level, even a few percent error in the estimates of the background may affect significantly our temperature measurements. To quantify this, following Leccardi & Molendi (2008A&A...486..359L 2008A&A...486..359L), we define the indicator SOU/BKG for all DR1 clusters and for all regions where we extracted spectra.. We compute it as (OBS-BKG)/BKG, where OBS is the observed count rate and BKG is the predicted count-rate by the best fit model of all the background components. -------------------------------------------------------------------------------- Acknowledgements: Maria-Chiara Rossetti, mariachiara.rossetti(at)inaf.it References: CHEX-MATE Collaboration, 2021A&A...650A.104C 2021A&A...650A.104C Campitiello et al., 2022A&A...665A.117C 2022A&A...665A.117C Oppizzi et al., 2023A&A...672A.156O 2023A&A...672A.156O Bartalucci et al., 2023A&A...674A.179B 2023A&A...674A.179B Bourdin et al., 2023A&A...678A.181B 2023A&A...678A.181B, Cat. J/A+A/678/A181 Iqbal et al., 2023A&A...679A..51I 2023A&A...679A..51I
(End) Patricia Vannier [CDS] 13-Mar-2024
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