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<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1017/pasa.2025.10033</dc:identifier><dc:language>eng</dc:language><dc:creator>Tanidis, Konstantinos</dc:creator><dc:creator>Asorey, Jacobo</dc:creator><dc:creator>Saraf, Chandra Shekhar</dc:creator><dc:creator>Hale, Catherine Laura</dc:creator><dc:creator>Bahr-Kalus, Benedict</dc:creator><dc:creator>Parkinson, David</dc:creator><dc:creator>Camera, Stefano</dc:creator><dc:creator>Norris, Ray</dc:creator><dc:creator>Hopkins, Andrew</dc:creator><dc:creator>Bilicki, Maciej</dc:creator><dc:creator>Gupta, Nikhel</dc:creator><dc:title>Cross-correlating the EMU Pilot Survey 1 with CMB lensing: Constraints on cosmology and galaxy bias with harmonic-space power spectra</dc:title><dc:identifier>ART-2025-144649</dc:identifier><dc:description>We measured the harmonic-space power spectrum of Galaxy clustering auto-correlation from the Evolutionary Map of the Universe Pilot Survey 1 data (EMU PS1) and its cross-correlation with the lensing convergence map of cosmic microwave background (CMB) from Planck Public Release 4 at the linear scale range from $\ell=2$ to 500. We applied two flux density cuts at $0.18$ and $0.4$ mJy on the radio galaxies observed at 944MHz and considered two source detection algorithms. We found the auto-correlation measurements from the two algorithms at the 0.18 mJy cut to deviate for $\ell\gtrsim250$ due to the different criteria assumed on the source detection and decided to ignore data above this scale. We report a cross-correlation detection of EMU PS1 with CMB lensing at $\sim$5.5$\sigma$, irrespective of flux density cut. In our theoretical modelling we considered the SKADS and T-RECS redshift distribution simulation models that yield consistent results, a linear and a non-linear matter power spectrum, and two linear galaxy bias models. That is a constant redshift-independent galaxy bias $b(z)=b_g$ and a constant amplitude galaxy bias $b(z)=b_g/D(z)$. By fixing a cosmology model and considering a non-linear matter power spectrum with SKADS, we measured a constant galaxy bias at $0.18$ mJy ($0.4$ mJy) with $b_g=2.32^{+0.41}_{-0.33}$ ($2.18^{+0.17}_{-0.25}$) and a constant amplitude bias with $b_g=1.72^{+0.31}_{-0.21}$ ($1.78^{+0.22}_{-0.15}$). When $\sigma_8$ is a free parameter for the same models at $0.18$ mJy ($0.4$ mJy) with the constant model we found $\sigma_8=0.68^{+0.16}_{-0.14}$ ($0.82\pm0.10$), while with the constant amplitude model we measured $\sigma_8=0.61^{+0.18}_{-0.20}$ ($0.78^{+0.11}_{-0.09}$), respectively. Our results agree at $1\sigma$ with the measurements from Planck CMB and the weak lensing surveys and also show the potential of cosmology studies with future radio continuum survey data.</dc:description><dc:date>2025</dc:date><dc:source>http://zaguan.unizar.es/record/162016</dc:source><dc:doi>10.1017/pasa.2025.10033</dc:doi><dc:identifier>http://zaguan.unizar.es/record/162016</dc:identifier><dc:identifier>oai:zaguan.unizar.es:162016</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA-FSE/E21-17R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/PID2022-138263NB-I00</dc:relation><dc:identifier.citation>PUBLICATIONS OF THE ASTRONOMICAL SOCIETY OF AUSTRALIA 42 (2025), e062 [18 pp.]</dc:identifier.citation><dc:rights>by</dc:rights><dc:rights>https://creativecommons.org/licenses/by/4.0/deed.es</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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