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  • 1
    Publication Date: 2015-08-20
    Description: We compare the shapes and intrinsic alignments of galaxies in the MassiveBlack-II (MBII) cosmological hydrodynamic simulation to those in an identical dark matter-only (DMO) simulation. Understanding the impact of baryonic physics on galaxy shapes should prove useful for creating mock galaxy catalogues based on DMO simulations that mimic intrinsic alignments in hydrodynamic simulations. The dark matter subhaloes are typically rounder in MBII, and the shapes of stellar matter in low-mass galaxies are more misaligned with the shapes of dark matter of the corresponding subhaloes in the DMO simulation. At z  = 0.06, the fractional difference in the mean misalignment angle between MBII and DMO simulations varies from ~28to12 per cent in the mass range 10 10.8 –6.0  x  10 14 h –1 M . We study the dark matter halo shapes and alignments as a function of radius, and find that while galaxies in MBII are more aligned with the inner parts of their dark matter subhaloes, there is no radial trend in their alignments with the corresponding subhalo in the DMO simulation. This result highlights the importance of baryonic physics in determining galaxy alignments with inner parts of their halo. Finally, we find that the stellar-dark matter misalignment suppresses the ellipticity–direction (ED) correlation of galaxies in comparison to that of dark matter haloes. In the projected shape–density correlation ( w + ), higher mean ellipticities of the stellar component reduce this effect, but differences of the order of 30–40 per cent remain on scales 〉1 Mpc.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 2
    Publication Date: 2015-09-21
    Description: We examine the luminosity function (LF) of [O ii ] emission-line galaxies in the high-resolution cosmological simulation MassiveBlack-II (MBII). From the spectral energy distribution of each galaxy, we select a sub-sample of star-forming galaxies at 0.06 ≤  z  ≤ 3.0 using the [O ii ] emission line luminosity L ([O ii ]). We confirm that the specific star formation rate matches that in the Galaxy And Mass Assembly survey. We show that the [O ii ] LF at z  = 1.0 from the MBII shows good agreement with the LFs from several surveys below L ([O ii ]) = 10 43.0  erg s –1 while the low redshifts ( z  ≤ 0.3) show an excess in the prediction of bright [O ii ] galaxies, but still displaying a good match with observations below L ([O ii ]) = 10 41.6  erg s –1 . Based on the validity in reproducing the properties of [O ii ] galaxies at low redshift ( z  ≤ 1), we forecast the evolution of the [O ii ] LF at high redshift ( z  ≤ 3), which can be tested by upcoming surveys such as the Hobby-Eberly Telescope Dark Energy Experiment and Dark Energy Spectroscopic Instrument. The slopes of the LFs at bright and faint ends range from –3 to –2 showing minima at z  = 2. The slope of the bright end evolves approximately as ( z  + 1) –1 at z  ≤ 2 while the faint end evolves as ~3( z  + 1) –1 at 0.6 ≤  z  ≤ 2. In addition, a similar analysis is applied for the evolution of [O iii ] LFs, which is to be explored in the forthcoming survey Wide-Field InfraRed Survey Telescope -Astrophysics Focused Telescope Assets. Finally, we show that the auto-correlation function of [O ii ] and [O iii ] emitting galaxies shows a rapid evolution from z  = 2 to 1.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 3
    Publication Date: 2016-06-19
    Description: We use the large cosmological hydro-dynamic simulation B lue T ides to predict the photometric properties of galaxies during the epoch of reionization ( z = 8–15). These properties include the rest-frame UV to near-IR broad-band spectral energy distributions, the Lyman continuum (LyC) photon production, the UV star formation rate calibration, and intrinsic UV continuum slope. In particular we focus on exploring the effect of various modelling assumptions, including the assumed choice of stellar population synthesis (SPS) model, initial mass function, and the escape fraction of LyC photons, upon these quantities. We find that these modelling assumptions can have a dramatic effect on photometric properties leading to consequences for the accurate determination of physical properties from observations. For example, at z = 8 we predict that nebular emission can account for up to 50 per cent of the rest-frame R -band luminosity, while the choice of SPS model can change the LyC production rate up to a factor of x 2.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 4
    Publication Date: 2005-07-18
    Print ISSN: 0027-8424
    Electronic ISSN: 1091-6490
    Topics: Biology , Medicine , Natural Sciences in General
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  • 5
    Publication Date: 2016-08-25
    Description: We study the shapes and intrinsic alignments of discs and elliptical galaxies in the MassiveBlack-II (MBII) and Illustris cosmological hydrodynamic simulations, with volumes of (100 h –1 Mpc) 3 and (75 h –1 Mpc) 3 , respectively. We find that simulated disc galaxies are more oblate in shape and more misaligned with the shape of their host dark matter subhalo when compared with ellipticals. The disc major axis is found to be oriented towards the location of nearby elliptical galaxies. We also find that the discs are thinner in MBII and misalignments with dark matter halo orientations are smaller in both discs and ellipticals when compared with Illustris. As a result, the intrinsic alignment correlation functions at fixed mass have a higher amplitude in MBII than in Illustris. Finally, at scales above ~0.1 h –1 Mpc, the intrinsic alignment two-point correlation functions for disc galaxies in both simulations are consistent with a null detection, unlike those for ellipticals. Despite significant differences in the treatments of hydrodynamics and baryonic physics in the simulations, we find that the w + correlation function scales similarly with transverse separation. However, the less massive galaxies show different scale dependence in the ellipticity-direction correlation. This result indicates that, while hydrodynamic simulations are a promising tool to study intrinsic alignments, further study is needed to understand the impact of differences in the implementations of hydrodynamics and baryonic feedback.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 6
    Publication Date: 2015-10-19
    Description: In this paper, we study the filamentary structures and the galaxy alignment along filaments at redshift z  = 0.06 in 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 Mpc  h –1 ) 3 . The filaments are constructed using the subspace constrained mean shift (SCMS; Ozertem & Erdogmus; Chen et al.). First, we show that reconstructed filaments using galaxies and reconstructed filaments using dark matter particles are similar to each other; over 50 per cent of the points on the galaxy filaments have a corresponding point on the dark matter filaments within distance 0.13 Mpc  h –1 (and vice versa) and this distance is even smaller at high-density regions. Second, we observe the alignment of the major principal axis of a galaxy with respect to the orientation of its nearest filament and detect a 2.5 Mpc  h –1 critical radius for filament's influence on the alignment when the subhalo mass of this galaxy is between 10 9 M h –1 and 10 12 M h –1 . Moreover, we find the alignment signal to increase significantly with the subhalo mass. Third, when a galaxy is close to filaments (less than 0.25 Mpc  h –1 ), the galaxy alignment towards the nearest galaxy group is positively correlated with the galaxy subhalo mass. Finally, we find that galaxies close to filaments or groups tend to be rounder than those away from filaments or groups.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 7
    Publication Date: 2016-06-15
    Description: Using deep Hubble and Spitzer observations Oesch et al. have identified a bright ( M UV –22) star-forming galaxy candidate at z 11. The presence of GN- z 11 implies a number density ~10 –6 Mpc –3 , roughly an order of magnitude higher than the expected value based on extrapolations from lower redshift. Using the unprecedented volume and high resolution of the B lue T ides cosmological hydrodynamical simulation, we study the population of luminous rare objects at z 〉 10. The luminosity function in B lue T ides implies an enhanced number of massive galaxies, consistent with the observation of GN- z 11. We find about 30 galaxies at M UV –22 at z = 11 in the B lue T ides volume, including a few objects about 1.5 mag brighter. The probability of observing GN- z 11 in the volume probed by Oesch et al. is ~13 per cent. The predicted properties of the rare bright galaxies at z = 11 in B lue T ides closely match those inferred from the observations of GN- z 11. B lue T ides predicts a negligible contribution from faint AGN in the observed SED. The enormous increase in volume surveyed by WFIRST will provide observations of ~1000 galaxies with M UV 〈 –22 beyond z = 11 out to z = 13.5.
    Print ISSN: 1745-3925
    Electronic ISSN: 1745-3933
    Topics: Physics
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  • 8
    Publication Date: 2015-04-26
    Description: We investigate the properties of haloes, galaxies and black holes to z  = 0 in the high-resolution hydrodynamical simulation MassiveBlack-II (MBII) which evolves a cold dark matter cosmology in a comoving volume V box  = (100 Mpc h –1 ) 3 . MBII is the highest resolution simulation of this size which includes a self-consistent model for star formation, black hole accretion and associated feedback. We provide a simulation browser web application which enables interactive search and tagging of the MBII data set and publicly release our galaxy catalogues. We find that baryons affect strongly the halo mass function (MF), with 20–33 per cent change in the halo abundance below the knee of the MF ( M halo  〈 10 13.2 M h –1 at z  = 0) when compared to dark-matter-only simulations. We provide a fitting function for the halo MF out to redshift z  = 11 and discuss its limitations. We study the halo occupation distribution and clustering of galaxies, in particular the evolution and scale dependence of stochasticity and bias finding reasonable agreement with observational data. The shape of the cosmic spectral energy distribution of galaxies in MBII is consistent with observations, but lower in amplitude. The Galaxy stellar mass function (GSMF) function is broadly consistent with observations at z  ≥ 2. At z  〈 2, the population of passive low-mass ( M *  〈 10 9 M ) galaxies in MBII makes the GSMF too steep compared to observations whereas at the high-mass end ( M *  〉 10 11 M ) galaxies hosting bright AGNs make significant contributions to the GSMF. The quasar bolometric luminosity function is also largely consistent with observations. We note however that more efficient AGN feedback is necessary for the largest, rarest objects/clusters at low redshifts.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 9
    Publication Date: 2015-09-23
    Description: We examine the luminosity function (LF) of [O ii ] emission-line galaxies in the high-resolution cosmological simulation MassiveBlack-II (MBII). From the spectral energy distribution of each galaxy, we select a sub-sample of star-forming galaxies at 0.06 ≤  z  ≤ 3.0 using the [O ii ] emission line luminosity L ([O ii ]). We confirm that the specific star formation rate matches that in the Galaxy And Mass Assembly survey. We show that the [O ii ] LF at z  = 1.0 from the MBII shows good agreement with the LFs from several surveys below L ([O ii ]) = 10 43.0  erg s –1 while the low redshifts ( z  ≤ 0.3) show an excess in the prediction of bright [O ii ] galaxies, but still displaying a good match with observations below L ([O ii ]) = 10 41.6  erg s –1 . Based on the validity in reproducing the properties of [O ii ] galaxies at low redshift ( z  ≤ 1), we forecast the evolution of the [O ii ] LF at high redshift ( z  ≤ 3), which can be tested by upcoming surveys such as the Hobby-Eberly Telescope Dark Energy Experiment and Dark Energy Spectroscopic Instrument. The slopes of the LFs at bright and faint ends range from –3 to –2 showing minima at z  = 2. The slope of the bright end evolves approximately as ( z  + 1) –1 at z  ≤ 2 while the faint end evolves as ~3( z  + 1) –1 at 0.6 ≤  z  ≤ 2. In addition, a similar analysis is applied for the evolution of [O iii ] LFs, which is to be explored in the forthcoming survey Wide-Field InfraRed Survey Telescope -Astrophysics Focused Telescope Assets. Finally, we show that the auto-correlation function of [O ii ] and [O iii ] emitting galaxies shows a rapid evolution from z  = 2 to 1.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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  • 10
    Publication Date: 2015-10-02
    Description: We use the high-resolution simulation MassiveBlackII to examine scaling relations between black hole (BH) mass and host galaxy properties (, total M * and L V ), finding good agreement with recent observational data, especially at the high-mass end. We find Gaussian intrinsic scatter (~half the observed scatter) about all three relations, except among the most massive objects. Below z  ~ 2 the slope of the relations remain roughly z -independent, and only steepen by 50 per cent by z  ~ 4. The normalization of the , L V relations evolve by 0.3, 0.43 dex, while the M * correlation does not evolve out to at least z  ~ 2. Testing for selection biases, we find M BH - or M * -selected samples have steeper slopes than random samples, suggesting a constant-mass selection function can exhibit faster evolution than a random sample. We find a potential bias among high- L BH subsamples due to their more massive hosts, but that bright (active) active galactic nuclei exhibit no intrinsic bias relative to fainter (inactive) BHs in equivalent-mass hosts. Finally, we show that BHs below the local relation tend to grow faster than their host (72 per cent of BHs 〉0.3 dex below the mean relation have an M BH – M * trajectory steeper than the local relation), while those above have shallower trajectories (only 14 per cent are steeper than local). Thus BHs tend to grow faster than their hosts until surpassing the local relation, when their growth is suppressed, bringing them back towards the mean relation.
    Print ISSN: 0035-8711
    Electronic ISSN: 1365-2966
    Topics: Physics
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