TY - JOUR
T1 - Cosmological simulation with dust formation and destruction
AU - Aoyama, Shohei
AU - Hou, Kuan Chou
AU - Hirashita, Hiroyuki
AU - Nagamine, Kentaro
AU - Shimizu, Ikkoh
N1 - Funding Information:
We thank the anonymous referee for careful reading and useful comments. We are grateful to Volker Springel for providing us with the original version of the GADGET-3 code. Numerical computations were carried out on the Cray XC30 at the Center for Computational Astrophysics, National Astronomical Observatory of Japan and XL at the Theoretical Institute for Advanced Research in Astrophysics (TIARA) in Academia Sinica. HH thanks the Ministry of Science and Technology for financial support through MOST 105-2112-M-001-027-MY3 and MOST 107-2923-M-001-003-MY3. This work was in part supported by JSPS KAKENHI Grant Number JP17H01111.
Funding Information:
We thank the anonymous referee for careful reading and useful comments. We are grateful to Volker Springel for providing us with the original version of the GADGET-3 code. Numerical computations were carried out on the Cray XC30 at the Center for Computational Astrophysics, National Astronomical Observatory of Japan and XL at the Theoretical Institute for Advanced Research in Astrophysics (TIARA) in Academia Sinica. HHthanks the Ministry of Science and Technology for financial support through MOST 105-2112-M-001-027-MY3 and MOST 107-2923-M-001-003-MY3. This work was in part supported by JSPS KAKENHI Grant Number JP17H01111.
Publisher Copyright:
© 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society.
PY - 2018/8/21
Y1 - 2018/8/21
N2 - To investigate the evolution of dust in a cosmological volume, we perform hydrodynamic simulations, in which the enrichment of metals and dust is treated self-consistently with star formation and stellar feedback. We consider dust evolution driven by dust production in stellar ejecta, dust destruction by sputtering, grain growth by accretion and coagulation, and grain disruption by shattering, and treat small and large grains separately to trace the grain size distribution. After confirming that our model nicely reproduces the observed relation between dust-to-gas ratio and metallicity for nearby galaxies, we concentrate on the dust abundance over the cosmological volume in this paper. The comoving dust mass density has a peak at redshift z ~ 1-2, coincident with the observationally suggested dustiest epoch in the Universe. In the local Universe, roughly 10 per cent of the dust is contained in the intergalactic medium (IGM), where only 1/3-1/4 of the dust survives against dust destruction by sputtering. We also show that the dust mass function is roughly reproduced at ≲ 108 M⊙, while the massive end still has a discrepancy, which indicates the necessity of stronger feedback in massive galaxies. In addition, our model broadly reproduces the observed radial profile of dust surface density in the circum-galactic medium (CGM). While our model satisfies the observational constraints for the dust extinction on cosmological scales, it predicts that the dust in the CGM and IGM is dominated by large (> 0.03μm) grains, which is in tension with the steep reddening curves observed in the CGM.
AB - To investigate the evolution of dust in a cosmological volume, we perform hydrodynamic simulations, in which the enrichment of metals and dust is treated self-consistently with star formation and stellar feedback. We consider dust evolution driven by dust production in stellar ejecta, dust destruction by sputtering, grain growth by accretion and coagulation, and grain disruption by shattering, and treat small and large grains separately to trace the grain size distribution. After confirming that our model nicely reproduces the observed relation between dust-to-gas ratio and metallicity for nearby galaxies, we concentrate on the dust abundance over the cosmological volume in this paper. The comoving dust mass density has a peak at redshift z ~ 1-2, coincident with the observationally suggested dustiest epoch in the Universe. In the local Universe, roughly 10 per cent of the dust is contained in the intergalactic medium (IGM), where only 1/3-1/4 of the dust survives against dust destruction by sputtering. We also show that the dust mass function is roughly reproduced at ≲ 108 M⊙, while the massive end still has a discrepancy, which indicates the necessity of stronger feedback in massive galaxies. In addition, our model broadly reproduces the observed radial profile of dust surface density in the circum-galactic medium (CGM). While our model satisfies the observational constraints for the dust extinction on cosmological scales, it predicts that the dust in the CGM and IGM is dominated by large (> 0.03μm) grains, which is in tension with the steep reddening curves observed in the CGM.
KW - Dust
KW - Extinction
KW - Galaxies: ISM
KW - Galaxies: evolution
KW - Galaxies: formation
KW - ISM: dust
KW - Methods: numerical
UR - http://www.scopus.com/inward/record.url?scp=85050790749&partnerID=8YFLogxK
U2 - 10.1093/mnras/sty1431
DO - 10.1093/mnras/sty1431
M3 - Article
AN - SCOPUS:85050790749
SN - 0035-8711
VL - 478
SP - 4905
EP - 4921
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 4
ER -