Abstract

The intrinsic alignment of galaxy shapes with the large-scale density field is a contaminant to weak lensing measurements, as well as being an interesting signature of galaxy formation and evolution (albeit one that is difficult to predict theoretically). Here we investigate the shapes and relative orientations of the stars and dark matter of halos and subhalos (central and satellite) extracted from the MassiveBlack-II simulation, a state-of-the-art high resolution hydrodynamical cosmological simulation which includes stellar and AGN feedback in a volume of $(100{h^{-1}\mathrm{Mpc}})^3$. We consider redshift evolution from $z=1$ to $0.06$ and mass evolution within the range of subhalo masses, $10^{10} -6.0 \times 10^{14.0}{h^{-1}M_{\odot}}$. The shapes of the dark matter distributions are generally more round than the shapes defined by stellar matter. The projected root-mean-square (RMS) ellipticity per component for stellar matter is measured to be $e_\text{rms} = 0.28$ at $z=0.3$ for $M_{subhalo}> 10^{12.0}{h^{-1}M_{\odot}}$, which compares favourably with observational measurements. We find that the shapes of stellar and dark matter are more round for less massive subhalos and at lower redshifts. By directly measuring the relative orientation of the stellar matter and dark matter of subgroups, we find that, on average, the misalignment between the two components is larger for less massive subhalos. The mean misalignment angle varies from $\sim 30^{\circ}-10^{\circ}$ for $M \sim 10^{10} - 10^{14} {h^{-1}M_{\odot}}$ and shows a weak dependence on redshift. We also compare the misalignment angles in central and satellite subhalos at fixed subhalo mass, and find that centrals are more misaligned than satellites. We present fitting formulae for the shapes of dark and stellar matter in subhalos and also the probability distributions of misalignment angles.

Highlights

  • Weak gravitational lensing is a useful probe to constrain cosmological parameters since it is sensitive to both luminous and dark matter (Hu 2002; Benabed & van Waerbeke 2004; Ishak et al 2004; Takada & White 2004; Bernstein & Jain 2004; Huterer 2010)

  • We find good agreement with the theoretical prediction given in Tinker et al (2008) based on Spherical Overdensity (SO) approach

  • Our results agree with theirs qualitatvely in that the average axis ratios, q and s, increase as we go to lower redshifts and lower masses for the dark matter component

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Summary

INTRODUCTION

Weak gravitational lensing is a useful probe to constrain cosmological parameters since it is sensitive to both luminous and dark matter (Hu 2002; Benabed & van Waerbeke 2004; Ishak et al 2004; Takada & White 2004; Bernstein & Jain 2004; Huterer 2010). Using a high-resolution hydrodynamic simulation in a large cosmological volume that incorporates the physics of star formation and associated feedback as well as black hole accretion and AGN feedback, we focus on measuring directly the shapes of the stellar components of galaxies and examine the misalignments between stars and dark matter in galaxies (central and satellite). Dubois et al (2014) studied the alignment between the spin of galaxies and their host filament direction using a hydrodynamical cosmological simulation of box size 100h−1Mpc. Studies of misalignment based on SPH simulations of smaller volumes detected misalignments between the baryonic and dark matter component of halos (van den Bosch et al 2003; Sharma & Steinmetz 2005; Hahn et al 2010; Deason et al 2011). The functional forms for our results are provided in the Appendix

MassiveBlack-II Simulation
Determination of 3D and 2D shapes
Convergence tests on axis ratios
SHAPES OF DARK MATTER AND STELLAR MATTER OF SUBGROUPS
Redshift evolution and mass dependence of 3D axis ratios
MISALIGNMENTS BETWEEN STELLAR MATTER AND DARK MATTER SHAPES OF SUBHALOS
Definition of misalignment angle
Mass and redshift dependence of misalignments
CONCLUSIONS

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