Early-type galaxy spin evolution in the Horizon-AGN simulation

The Astrophysical Journal University of Chicago Press

Authors:

H Choi, SK Yi, Y Dubois, T Kimm, JEG Devriendt, C Pichon

Abstract:

Using the Horizon-AGN simulation data, we study the relative role of mergers and environmental effects in shaping the spin of early-type galaxies (ETGs) after $z \simeq 1$. We follow the spin evolution of 10,037 color-selected ETGs more massive than 10$^{10} \rm \, M_{\odot}$ that are divided into four groups: cluster centrals (3%), cluster satellites (33%), group centrals (5%), and field ETGs (59%). We find a strong mass dependence of the slow rotator fraction, $f_{\rm SR}$, and the mean spin of massive ETGs. Although we do not find a clear environmental dependence of $f_{\rm SR}$, a weak trend is seen in the mean value of spin parameter driven by the satellite ETGs as they gradually lose their spin as their environment becomes denser. Galaxy mergers appear to be the main cause of total spin changes in 94% of central ETGs of halos with $M_{vir} > 10^{12.5}\rm M_{\odot}$, but only 22% of satellite and field ETGs. We find that non-merger induced tidal perturbations better correlate with the galaxy spin-down in satellite ETGs than mergers. Given that the majority of ETGs are not central in dense environments, we conclude that non-merger tidal perturbation effects played a key role in the spin evolution of ETGs observed in the local ($z < 1$) universe.

Enhanced constraints on large-scale structure from secondary CMB anisotropies

Abstract:

The large-scale structure of the Universe encodes invaluable information about the fundamental cosmological parameters, the physics of structure formation, and the thermodynamic history of the Universe. In this thesis, we explore how secondary anisotropies of the Cosmic Microwave Background (CMB), particularly the thermal Sunyaev-Zeldovich (tSZ) effect and CMB lensing, can improve constraints on the large-scale structure. We develop a framework to cross-correlate tSZ maps from the Planck satellite with the distribution of galaxies at low redshift using tomographic bins with data from the 2MASS Photometric Redshift catalogue and WISE x SuperCOSMOS. These cross-correlations enable precise measurements of the bias-weighted gas pressure, โŸจ๐‘PeโŸฉ, and the hydrostatic mass bias parameter, 1โˆ’bH,ย as a function of redshift.

This thesis is primarily based on two complementary studies employing galaxy clustering (๐›ฟ๐‘” ร— ๐›ฟ๐‘”), galaxy-tSZ cross-correlations (๐›ฟ๐‘” ร— y), and galaxy-CMB lensing cross-correlations (๐›ฟ๐‘” ร— K) to constrain cosmological and thermodynamic parameters across six redshift bins (๐‘ง โˆˆ [0.1, 0.6]).

In the first study, we use a combination of ๐›ฟ๐‘” ร— ๐›ฟ๐‘”ย and ๐›ฟ๐‘”ย ร— y to improve constraints on the thermal history of the Universe. We achieve ~6 \% precision on 1-bH across the six redshift bins, finding consistency with previous results and no evidence for significant redshift dependence. Our best-fit value of 1โˆ’๐‘H = 0.75 ยฑ 0.03 aligns well with joint analyses of Planck cluster counts and CMB anisotropies calibrated with CMB lensing. Additionally, our constraints on โŸจ๐‘๐‘ƒ๐‘’โŸฉ, accurate to ~10% per bin, represent the most precise measurements to date, providing a robust test of baryonic feedback and models of energy injection.

The second study incorporatess ๐›ฟ๐‘” ร— Kย  to enhance our tomographic analysis of structure growth and gas thermodynamics. Using CMB lensing as an additional tracer of large-scale structure, we constrain the amplitude of fluctuations of the matter power spectrum, ๐œŽ8, to 6% across all redshift bins, the hydrostatic mass bias, 1 - bH to ~ 18 %, the bias-weighted average electron pressure, โŸจ๐‘๐‘ƒ๐‘’โŸฉ, to ~12%, the thermal energy density, ฮฉthย  to ~ 10%, as well as TAGN, a single parameter quantifying the intensive thermodynamic properties of haloes. We perform multiple robustness checks to verify the stability of our models, and we report broad agreement with previous results in the literature.

This work builds on the use of secondary CMB anisotropies as a probe of non-linear physics, and of the interplay between dark matter and baryonic matter in haloes. We incorporate novel methods for combining tSZ data with other probes, in an attempt to refine models of halo bias and constrain ๐œŽ8. The inclusion of ๐›ฟ๐‘” ร— K helps to break degeneracies between key parameters of the theoretical framework used. Hence, we highlight the importance of secondary CMB anisotropies as a complementary tool for understanding the large-scale structure, offering new insights into the thermal evolution of the Universe, as well as the growth of structure.

Euclid preparation: VI. Verifying the Performance of Cosmic Shear Experiments

Authors:

Euclid Collaboration, P Paykari, Td Kitching, H Hoekstra, R Azzollini, Vf Cardone, M Cropper, Caj Duncan, A Kannawadi, L Miller, H Aussel, If Conti, N Auricchio, M Baldi, S Bardelli, A Biviano, D Bonino, E Borsato, E Bozzo, E Branchini, S Brau-Nogue, M Brescia, J Brinchmann, C Burigana, S Camera, V Capobianco, C Carbone, J Carretero, Fj Castander, M Castellano, S Cavuoti, Y Charles, R Cledassou, C Colodro-Conde, G Congedo, C Conselice, L Conversi, Y Copin, J Coupon, Hm Courtois, A Da Silva, X Dupac, G Fabbian, S Farrens, Pg Ferreira, P Fosalba, N Fourmanoit, M Frailis, M Fumana, S Galeotta

Abstract:

Our aim is to quantify the impact of systematic effects on the inference of cosmological parameters from cosmic shear. We present an end-to-end approach that introduces sources of bias in a modelled weak lensing survey on a galaxy-by-galaxy level. Residual biases are propagated through a pipeline from galaxy properties (one end) through to cosmic shear power spectra and cosmological parameter estimates (the other end), to quantify how imperfect knowledge of the pipeline changes the maximum likelihood values of dark energy parameters. We quantify the impact of an imperfect correction for charge transfer inefficiency (CTI) and modelling uncertainties of the point spread function (PSF) for Euclid, and find that the biases introduced can be corrected to acceptable levels.

Exploring the origin of thick disks using the NewHorizon and Galactica simulations

Authors:

Minjung J Park, Sukyoung K Yi, Sebastien Peirani, Christophe Pichon, Yohan Dubois, Hoseung Choi, Julien Devriendt, Sugata Kaviraj, Taysun Kimm, Katarina Kraljic, Marta Volonteri

Abstract:

Ever since the thick disk was proposed to explain the vertical distribution of the Milky Way disk stars, its origin has been a recurrent question. We aim to answer this question by inspecting 19 disk galaxies with stellar mass greater than $10^{10}\,\rm M_\odot$ in recent cosmological high-resolution zoom-in simulations: Galactica and NewHorizon. The thin and thick disks are reproduced by the simulations with scale heights and luminosity ratios that are in reasonable agreement with observations. When we spatially classify the disk stars into thin and thick disks by their heights from the galactic plane, the "thick" disk stars are older, less metal-rich, kinematically hotter, and higher in accreted star fraction than the "thin" disk counterparts. However, both disks are dominated by stellar particles formed in situ. We find that approximately half of the in-situ stars in the thick disks are formed even before the galaxies develop their disks, and the other half are formed in spatially and kinematically thinner disks and then thickened with time by heating. We thus conclude from our simulations that the thin and thick disk components are not entirely distinct in terms of formation processes, but rather markers of the evolution of galactic disks. Moreover, as the combined result of the thickening of the existing disk stars and the continued formation of young thin-disk stars, the vertical distribution of stars does not change much after the disks settle, pointing to the modulation of both orbital diffusion and star formation by the same confounding factor: the proximity of galaxies to marginal stability.

First Detection of Spectral Variations of Anomalous Microwave Emission with QUIJOTE and C-BASS

Authors:

R Cepeda-Arroita, S Harper, C Dickinson, Ja Rubiรฑo-Martรญn, Rt Gรฉnova-Santos, Angela C Taylor, Tj Pearson, M Ashdown, A Barr, Rb Barreiro, B Casaponsa, Fj Casas, Hc Chiang, R Fernandez-Cobos, Rdp Grumitt, F Guidi, Hm Heilgendorff, D Herranz, Lrp Jew, Jl Jonas, Michael E Jones, A Lasenby, J Leech, Jp Leahy, E Martรญnez-Gonzรกlez, Mw Peel, F Poidevin, L Piccirillo, Acs Readhead, R Rebolo, B Ruiz-Granados, J Sievers, F Vansyngel, P Vielva, Ra Watson

Abstract:

Anomalous Microwave Emission (AME) is a significant component of Galactic diffuse emission in the frequency range $10$-$60\,$GHz and a new window into the properties of sub-nanometre-sized grains in the interstellar medium. We investigate the morphology of AME in the $\approx10^{\circ}$ diameter $\lambda$ Orionis ring by combining intensity data from the QUIJOTE experiment at $11$, $13$, $17$ and $19\,$GHz and the C-Band All Sky Survey (C-BASS) at $4.76\,$GHz, together with 19 ancillary datasets between $1.42$ and $3000\,$GHz. Maps of physical parameters at $1^{\circ}$ resolution are produced through Markov Chain Monte Carlo (MCMC) fits of spectral energy distributions (SEDs), approximating the AME component with a log-normal distribution. AME is detected in excess of $20\,\sigma$ at degree-scales around the entirety of the ring along photodissociation regions (PDRs), with three primary bright regions containing dark clouds. A radial decrease is observed in the AME peak frequency from $\approx35\,$GHz near the free-free region to $\approx21\,$GHz in the outer regions of the ring, which is the first detection of AME spectral variations across a single region. A strong correlation between AME peak frequency, emission measure and dust temperature is an indication for the dependence of the AME peak frequency on the local radiation field. The AME amplitude normalised by the optical depth is also strongly correlated with the radiation field, giving an overall picture consistent with spinning dust where the local radiation field plays a key role.