scholarly journals Photometric properties of reionization-epoch galaxies in the Simba simulations

Author(s):  
Xiaohan Wu ◽  
Romeel Davé ◽  
Sandro Tacchella ◽  
Jennifer Lotz

Abstract We study the photometric properties and sizes of the reionization-epoch galaxies in high-resolution Simba cosmological hydrodynamical simulations with box sizes of [25, 50]h−1Mpc. Assuming various attenuation laws, we compute photometry by extincting each star particle’s spectrum using the line-of-sight gas metal column density. The predicted ultraviolet luminosity function (UVLF) generally agrees with observations at z = 6, owing to a partial cancellation between the high metallicities of the simulated galaxies and lower dust-to-metal ratios. The simulated z = 8 UVLF is low compared to observations, likely owing to excessive dust extinction. Simba predicts UV continuum slopes (β) in agreement with the z = 6 observations, with the best agreement obtained using a Calzetti extinction law. Interestingly, the gas-phase mass-metallicity relation in Simba is higher at z ∼ 6 than at z ∼ 2, suggesting that rapid early enrichment (and dust growth) might be necessary to match the observed β. We find that β is more sensitive to the dust extinction law than the UVLF. By generating mock James Webb Space Telescope (JWST) images and analysing in a manner similar to observations, we show that Simba’s galaxy size–luminosity relation well reproduces the current z = 6 Hubble observations. Unlike observations at lower redshifts, Simba predicts similar rest-UV and rest-optical sizes of z = 6 galaxies, owing to weak age gradients and dust extinction in star-forming regions counteract each other to weaken the color gradients within galaxies. These predictions will be testable with JWST.

2020 ◽  
Vol 500 (1) ◽  
pp. 118-137
Author(s):  
A Zanella ◽  
A Pallottini ◽  
A Ferrara ◽  
S Gallerani ◽  
S Carniani ◽  
...  

ABSTRACT We investigate the spatially resolved morphology of galaxies in the early Universe. We consider a typical redshift z = 6 Lyman break galaxy, ‘Althæa’, from the SERRA hydrodynamical simulations. We create mock rest-frame ultraviolet (UV), optical, and far-infrared observations, and perform a two-dimensional morphological analysis to deblend the galaxy disc from substructures (merging satellites or star-forming regions). We find that the [C ii]158 μm emitting region has an effective radius 1.5–2.5 times larger than the optical one, consistent with recent observations. This [C ii] halo in our simulated galaxy arises as the joint effect of stellar outflows and carbon photoionization by the galaxy UV field, rather than from the emission of unresolved nearby satellites. At the typical angular resolution of current observations (≳ 0.15 arcsec) only merging satellites can be detected; detection of star-forming regions requires resolutions of ≲ 0.05 arcsec. The [C ii]-detected satellite has a 2.5-kpc projected distance from the galaxy disc, whereas the star-forming regions are embedded in the disc itself (distance ≲ 1 kpc). This suggests that multicomponent systems reported in the literature, which have separations ≳ 2 kpc, are merging satellites, rather than galactic substructures. Finally, the star-forming regions found in our mock maps follow the local L[C ii]–SFRUV relation of galaxy discs, although sampling the low-luminosity, low-SFR tail of the distribution. We show that future James Webb Space Telescope observations, bridging UV and [C ii] data sets, will be exceptionally suited to characterize galaxy substructures, thanks to their exquisite spatial resolution and sensitivity to both low-metallicity and dust-obscured regions that are bright at infrared wavelengths.


2018 ◽  
Vol 609 ◽  
pp. A66 ◽  
Author(s):  
R. E. G. Machado ◽  
P. B. Tissera ◽  
G. B. Lima Neto ◽  
L. Sodré

Context. Galaxies are surrounded by extended gaseous halos that store significant fractions of chemical elements. These are syntethized by the stellar populations and later ejected into the circumgalactic medium (CGM) by different mechanism, of which supernova feedback is considered one of the most relevant. Aims. We aim to explore the properties of this metal reservoir surrounding star-forming galaxies in a cosmological context aiming to investigate the chemical loop between galaxies and their CGM, and the ability of the subgrid models to reproduce observational results. Methods. Using cosmological hydrodynamical simulations, we have analysed the gas-phase chemical contents of galaxies with stellar masses in the range 109−1011 M⊙. We estimated the fractions of metals stored in the different CGM phases, and the predicted O vi and Si iii column densities within the virial radius. Results. We find roughly 107 M⊙ of oxygen in the CGM of simulated galaxies having M⋆ ~ 1010 M⊙, in fair agreement with the lower limits imposed by observations. The Moxy is found to correlate with M⋆, at odds with current observational trends but in agreement with other numerical results. The estimated profiles of O vi column density reveal a substantial shortage of that ion, whereas Si iii, which probes the cool phase, is overpredicted. Nevertheless, the radial dependences of both ions follow the respective observed profiles. The analysis of the relative contributions of both ions from the hot, warm and cool phases suggests that the warm gas (105 K < T < 106 K) should be more abundant in order to bridge the mismatch with the observations, or alternatively, that more metals should be stored in this gas-phase. These discrepancies provide important information to improve the subgrid physics models. Our findings show clearly the importance of tracking more than one chemical element and the difficulty of simultaneously satisfying the observables that trace the circumgalactic gas at different physical conditions. Additionally, we find that the X-ray coronae around the simulated galaxies have luminosities and temperatures in decent agreement with the available observational estimates.


2004 ◽  
Vol 194 ◽  
pp. 3-6
Author(s):  
Andrea H. Prestwich

AbstractChandra and XMM-Newton are revolutionizing our understanding of compact binaries in external galaxies, allowing us to study sources in detail in Local Group Galaxies and study populations in more distant systems. In M31 the X-ray luminosity function depends on the local stellar population in the sense that areas with active star formation have more high luminosity sources, and a higher overall source density (Kong. Di Stefano. Garcia, & Greiner 2003). This result is also true in galaxies outside the Local Group; starburst galaxies have flatter X-ray luminosity functions than do spiral galaxies which are in turn flatter than elliptical galaxies. These observational results suggest that the high end of the luminosity function in star forming regions is dominated by short-lived high mass X-ray binaries.In Chandra Cycle 2 we started a Large Project to survey a sample of 11 nearby (< 10Mpc) face-on spiral galaxies. We find that sources can be approximately classified on the basis of their X-ray color into low mass X-ray binaries, high mass X-ray binaries and supersoft sources. There is an especially interesting class of source that has X-ray colors softer (“redder”) than a typical low mass X-ray binary source, but not so extreme as supersoft sources. Most of these are probably X-ray bright supernova remnants, but some may be a new type of black hole accretor. Finally, when we construct a luminosity function of sources selecting only sources with low mass X-ray binary colors (removing soft sources) we find that there is a dip or break probably associated with the Eddington luminosity for a neutron star.


1997 ◽  
Vol 178 ◽  
pp. 45-60 ◽  
Author(s):  
A.G.G.M. Tielens ◽  
D.C.B. Whittet

IR spectra of sources associated with molecular cloud material show a variety of absorption features attributed to simple molecules, such as H2O, CO, CH3OH, CO2, CH4, and OCS in icy grain mantles. These identifications are reviewed. These molecules are formed through accretion and reaction of gas phase species on grain surfaces. The high abundance of CH3OH and CO2 point towards the importance of hydrogenation and oxidation reactions in this process. Observations also show that thermal outgassing is of great importance for the composition of interstellar ice mantles. Both these processes are discussed in some detail.


2019 ◽  
Vol 631 ◽  
pp. A137 ◽  
Author(s):  
H. Calcutt ◽  
E. R. Willis ◽  
J. K. Jørgensen ◽  
P. Bjerkeli ◽  
N. F. W. Ligterink ◽  
...  

Context. Propyne (CH3CCH), also known as methyl acetylene, has been detected in a variety of environments, from Galactic star-forming regions to extragalactic sources. These molecules are excellent tracers of the physical conditions in star-forming regions, allowing the temperature and density conditions surrounding a forming star to be determined. Aims. This study explores the emission of CH3CCH in the low-mass protostellar binary, IRAS 16293–2422, and examines the spatial scales traced by this molecule, as well as its formation and destruction pathways. Methods. Atacama Large Millimeter/submillimeter Array (ALMA) observations from the Protostellar Interferometric Line Survey (PILS) were used to determine the abundances and excitation temperatures of CH3CCH towards both protostars. This data allows us to explore spatial scales from 70 to 2400 au. This data is also compared with the three-phase chemical kinetics model MAGICKAL, to explore the chemical reactions of this molecule. Results. CH3CCH is detected towards both IRAS 16293A and IRAS 16293B, and is found the hot corino components, one around each source, in the PILS dataset. Eighteen transitions above 3σ are detected, enabling robust excitation temperatures and column densities to be determined in each source. In IRAS 16293A, an excitation temperature of 90 K and a column density of 7.8 × 1015 cm−2 best fits the spectra. In IRAS 16293B, an excitation temperature of 100 K and 6.8 × 1015 cm−2 best fits the spectra. The chemical modelling finds that in order to reproduce the observed abundances, both gas-phase and grain-surface reactions are needed. The gas-phase reactions are particularly sensitive to the temperature at which CH4 desorbs from the grains. Conclusions. CH3CCH is a molecule whose brightness and abundance in many different regions can be utilised to provide a benchmark of molecular variation with the physical properties of star-forming regions. It is essential when making such comparisons, that the abundances are determined with a good understanding of the spatial scale of the emitting region, to ensure that accurate abundances are derived.


Author(s):  
Shinji Fujita ◽  
Daichi Tsutsumi ◽  
Akio Ohama ◽  
Asao Habe ◽  
Nirmit Sakre ◽  
...  

Abstract Using the NANTEN2 Observatory, we carried out a molecular-line study of high-mass star forming regions with reflection nebulae, NGC 2068 and NGC 2071, in Orion in the $^{13}$CO($J = 2$–1) transition. The $^{13}$CO distribution shows that there are two velocity components at ${9.0}$ and ${10.5}\:$km$\:$s$^{-1}$. The blue-shifted component is in the northeast associated with NGC 2071, whereas the red-shifted component is in the southwest associated with NGC 2068. The total intensity distribution of the two clouds shows a gap of $\sim\!\! 1\:$pc, suggesting that they are detached at present. A detailed spatial comparison indicates that the two show complementary distributions. The blue-shifted component lies toward an intensity depression to the northwest of the red-shifted component, where we find that a displacement of ${0.8}\:$pc makes the two clouds fit well with each other. Furthermore, a new simulation of non-frontal collisions shows that observations from $60^\circ$ off the collisional axis agreed well with the velocity structure in this region. On the basis of these results, we hypothesize that the two components collided with each other at a projected relative velocity of ${3.0}\:$km$\:$s$^{-1}$. The timescale of the collision is estimated to be ${0.3}\:$Myr for an assumed axis of the relative motion $60^\circ$ off the line of sight. We assume that the two most massive early B-type stars in the cloud, illuminating stars of the two reflection nebulae, were formed by collisional triggering at the interfaces between the two clouds. Given the other young high-mass star-forming regions, namely, M 42, M 43, and NGC 2024 (Fukui et al. 2018a, ApJ, 859, 166; Ohama et al. 2017, arXiv:1706.05652), it seems possible that collisional triggering has been independently working to form O-type and early B-type stars in Orion in the last Myr over a projected distance of ∼80 pc.


2014 ◽  
Vol 10 (S309) ◽  
pp. 247-250
Author(s):  
Tucker Jones

AbstractSpatially resolved spectroscopy is even more powerful when combined with magnification by gravitational lensing. I discuss observations of lensed galaxies at z≃2 with spatial resolution reaching 100 parsecs. Near-IR integral field spectroscopy reveals the kinematics, distribution and physical properties of star forming regions, and gas-phase metallicity gradients. Roughly two thirds of observed galaxies are isolated systems with coherent velocity fields, large velocity dispersion, multiple giant star-forming regions, and negative gas-phase metallicity gradients, suggestive of inside-out growth in gravitationally unstable disks. The remainder are undergoing mergers and have shallower metallicity gradients, indicating mixing of the interstellar gas via gravitational interaction. The metallicity gradients in isolated galaxies are consistent with simulations using standard feedback prescriptions, whereas simulations with enhanced feedback predict shallower gradients. These measurements therefore constrain the growth of galaxies from mergers and star formation as well as the regulatory feedback.


2018 ◽  
Vol 14 (S345) ◽  
pp. 355-357
Author(s):  
Ya-Ping Li

AbstractIn this work, we carry out two-fluid (gas+dust) hydrodynamical simulations on a large family of models in order to study the dust coagulation and the dust-gas dynamical processes in protoplanetary disks. Our theoretical effort is guided by the observational results of disks in nearby star forming regions at sub-millimeter and millimeter (mm) wavelengths. By a systematic comparison with the continuum emission at several mm bands from ALMA observations, we find that ringed structures are predicated in the unresolved faint disks for those with mm spectral indexes as low as about 2.0. Our parameter exploration can also be used to constrain the fragmentation velocity, one key parameter of the dust coagulation model, and some other disk parameters.


2018 ◽  
Author(s):  
◽  
Bradley W. Mills

"[ACCESS RESTRICTED TO THE UNIVERSITY OF MISSOURI AT AUTHOR'S REQUEST.] It is now well recognized that the interstellar medium acts as an efficient polarizer of electromagnetic radiation, resulting in the partial plane polarization of starlight by dichroic absorption by aligned, non-spherical dust grains on the line of sight. The discovery of the linear polarization of starlight provided a valuable mechanism for constraining the physical properties of interstellar dust, requiring the need for a grain population which both departs from spherical symmetry and efficiently aligns with the galactic magnetic field. Observations of light from distant stars have shown the degree of polarization to scale with reddening, suggesting that the grains which are responsible for effectively absorbing and scattering electromagnetic radiation are also responsible for the partial plane polarization of the transmitted light. The exact chemical and physical nature of interstellar dust remains a point of contention, being generally recognized to consist of both amorphous silicate and carbonaceous material. Grain models consisting of bare and separated silicate and carbon, silicates covered with a mantle of carbonaceous dust and porous composites of small silicates and carbonaceous particles have been invoked to explain the main observational constraints, most notably being the observed wavelength dependent extinction, polarization and far infrared emission. While each dust model appears to be consistent in explaining such constraints, each makes unique assumptions regarding the physical relationship of the main dust forming components, with no further methods of differentiating between such models being discussed. Spectropolarimetric observations across solid state absorption features have recently provided a means in which to distinguish between dust models. The core-mantle model of interstellar dust postulates a grain morphology consisting of an amorphous silicate core coated by (i.e., being physically associated with) a mantle of water ice, or carbonaceous material, being dependent on the environment in which the grain resides. For spectral features whose carrier resides in the mantle atop an elongated silicate core, a correlation between the polarization profiles of such features is expected with that of the silicate. Two studies are proposed: (i) Spectroscopic observations of dense, star forming regions from 2 to 13 µm have been carried out for several young, high luminosity infrared sources, protostars. The 3.1 µm feature, attributed to absorption by amorphous H2O ice, and 9.7 µm feature, attributed to absorption by amorphous silicates, appear concurrently in all sources with molecular clouds intervening along the line of sight, indicative of both ice and silicates as important grain constitutes in dense phases of the interstellar medium. Freeze out of gas phase elements onto refractory grain cores result in a silicate core-ice mantle grain morphology. Spectropolarimetric observations of the Becklin-Neugebauer (BN) object have shown the 3.1 µm and 9.7 µm features to be polarized, highly suggestive of an aligned silicate core-ice mantle grain morphology present on the line of sight. Subsequent observations of a source similar in nature to BN, the embedded protostar AFGL 2591, have raised a challenge to this model, with excess polarization detected in the 9.7 µm absorption band, combined with a 3.1 µm ice band feature being devoid of polarization. A model which physically associates the carrier material of the ice feature with that of an aligned silicate component requires a polarization signature across the 3.1 µm feature commensurate with that of the silicate feature. We seek to alleviate this challenge on the coreâ€""mantle model by computing the degree of polarization across both the 3.1 µm ice and 9.7 µm silicate features for spheroidal silicate core-spherical ice core-mantle grains; on the basis that grains with spherical mantles, being much less elongated in nature, should reduce the degree of polarization across the ice feature. By considering variations in specific grain parameters, including variations in core elongation and mantle thickness, we seek to reduce the degree of 3.1 µm polarization while simultaneously reproducing 9.7 µm spectropolarimetric observations. Such constraints provide a valuable test of the physical relationship of silicate and ice components in star forming regions. (ii)Spectroscopic observations from 2 to 13 µm have been carried out on multi- ple lines of sight which sample the diffuse interstellar medium. Absorption features at 3.4 µm, attributed to carbonaceous material, and 9.7 µm, attributed to amorphous silicates are indicative of both carbon and silicates materials as important grain constitutes. Spectropolarimetric observations have shown the 9.7 µm feature to be polarized, suggesting highly aligned silicate grains present on the line of sight. Subsequent observations of the 3.4 µm feature on the same Galactic sightlines have shown a carbonaceous dust feature to be devoid of polarization. A model which physically associates the carrier material of the carbonaceous feature with that of an aligned silicate component requires a polarization signature across the 3.4 µm feature commensurate with that of the silicate feature. No such excess rise is currently detected, indicative of a carbonaceous component being devoid of polarization. We seek to alleviate this challenge on the core-mantle model by computing the degree of polarization across both the 3.4 µm carbonaceous and 9.7 µm silicate features for spheroidal silicate core -'equal-thickness' carbonaceous core-mantle grains; on the basis that grains with equal thickness mantles should reduce the degree of polarization associated with the carbonaceous feature, a result of equal attenuation of light along both the grains semi-major and semi-minor axis. By considering variations in specific grain parameters, including variations in core elongation and mantle thickness, we seek to reduce the degree of 3.4 µm polarization while simultaneously reproducing both 9.7 µm and optical (0.55µm) spectropolarimetric observations. Such constraints provide a valuable test of the physical relationship of silicate and carbonaceous dust components in diffuse regions of the interstellar medium."


2007 ◽  
Vol 3 (S248) ◽  
pp. 186-189 ◽  
Author(s):  
L. Loinard ◽  
R. M. Torres ◽  
A. J. Mioduszewski ◽  
L. F. Rodríguez

AbstractUsing phase-referenced multi-epoch Very Long Baseline Array observations, we have measured the trigonometric parallax of several young stars in the Taurus and Ophiuchus star-forming regions with unprecedented accuracy. The mean distance to the Taurus complex was found to be about 140 pc, and its depth around 20 pc, comparable to the linear extent of Taurus on the sky. In Ophiuchus, 4 sources have been observed so far. Two of them were found to be at about 160 pc (the distance traditionally attributed to Ophiuchus), while the other 2 are at about 120 pc. Since the entire Ophiuchus complex is only a few parsecs across, this difference is unlikely to reflect the depth of the region. Instead, we argue that two physically unrelated sites of star-formation are located along the line of sight toward Ophiuchus.


Sign in / Sign up

Export Citation Format

Share Document