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Interpreting ALMA Observations of the ISM During the Epoch of Reionisation
Astrophysics of Galaxies · Submitted 6 Dec 2016
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim If smaller pockets of high metallicity gas exist in the ISM, the emission from these ions may be observable by ALMA while the low metallicity of the galaxy may cause these systems to fall below the local [CII]-SFR relation.
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The abstract, sentence by sentence
We present cosmological, radiation-hydrodynamics simulations of galaxy formation during the epoch of reionization in an effort towards modelling the interstellar medium (ISM) and interpreting ALMA observations. Simulations with and without stellar radiation are compared at large (Mpc), intermediate (tens of kpc), and small (sub kpc) scales. At large scales, the dense regions around galaxies reionize first before UV photons penetrate the voids; however, considerable amounts of neutral gas remain present within the haloes. The spatial distribution of neutral gas is highly dynamic and is anti-correlated with the presence of stars older than a few Myrs. For our specific feedback implementation, most of the metals remain inside the virial radii of haloes and they are proportionally distributed over the ionized and neutral medium by mass. For our most massive galaxy with ${\rm M_h}\sim10^{11}$M$_{\odot}$, the majority of the CII and OI mass are associated with cold neutral clumps. NII is more diffuse and arises in warmer gas while OIII arises in hotter gas with a higher ionization parameter, produced by photo-heating and supernovae. If smaller pockets of high metallicity gas exist in the ISM, the emission from these ions may be observable by ALMA while the low metallicity of the galaxy may cause these systems to fall below the local [CII]-SFR relation. The presence of dust can cause spatial offsets between UV/Ly$\alpha$ and [CII] emission as suggested by the recent observations of Maiolino et al. [OIII] may be spatially offset from both of these components since it arises from a different part of density-temperature phase-space.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present cosmological, radiation-hydrodynamics simulations of galaxy formation during the epoch of reionization in an effort towards modelling the interstellar medium (ISM) and interpreting ALMA observations. | contribution 0.98 | 0.95 | 0.06 | asserted 0.89 |
| s1 | Simulations with and without stellar radiation are compared at large (Mpc), intermediate (tens of kpc), and small (sub kpc) scales. | method 0.96 | 0.89 | 0.03 | asserted 0.88 |
| s2 | At large scales, the dense regions around galaxies reionize first before UV photons penetrate the voids; however, considerable amounts of neutral gas remain present within the haloes. | result 1.00 | 0.88 | 0.12 | asserted 1.00 |
| s3 | The spatial distribution of neutral gas is highly dynamic and is anti-correlated with the presence of stars older than a few Myrs. | result 1.00 | 0.89 | 0.09 | asserted 1.00 |
| s4 | For our specific feedback implementation, most of the metals remain inside the virial radii of haloes and they are proportionally distributed over the ionized and neutral medium by mass. | result 0.99 | 0.92 | 0.08 | asserted 1.00 |
| s5 | For our most massive galaxy with ${\rm M_h}\sim10^{11}$M$_{\odot}$, the majority of the CII and OI mass are associated with cold neutral clumps. | result 1.00 | 0.93 | 0.10 | asserted 1.00 |
| s6 | NII is more diffuse and arises in warmer gas while OIII arises in hotter gas with a higher ionization parameter, produced by photo-heating and supernovae. | result 0.91 | 0.85 | 0.06 | asserted 1.00 |
| s7 | If smaller pockets of high metallicity gas exist in the ISM, the emission from these ions may be observable by ALMA while the low metallicity of the galaxy may cause these systems to fall below the local [CII]-SFR relation. | interpretation 0.99 | 0.45 | 0.16 | hedged possibility 0.98 |
| s8 | The presence of dust can cause spatial offsets between UV/Ly$\alpha$ and [CII] emission as suggested by the recent observations of Maiolino et al. [OIII] may be spatially offset from both of these components since it arises from a different part of density-temperature phase-space. | interpretation 0.89 | 0.19 | 0.07 | hedged possibility 0.97 |
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The paper
Original abstract
We present cosmological, radiation-hydrodynamics simulations of galaxy formation during the epoch of reionization in an effort towards modelling the interstellar medium (ISM) and interpreting ALMA observations. Simulations with and without stellar radiation are compared at large (Mpc), intermediate (tens of kpc), and small (sub kpc) scales. At large scales, the dense regions around galaxies reionize first before UV photons penetrate the voids; however, considerable amounts of neutral gas remain present within the haloes. The spatial distribution of neutral gas is highly dynamic and is anti-correlated with the presence of stars older than a few Myrs. For our specific feedback implementation, most of the metals remain inside the virial radii of haloes and they are proportionally distributed over the ionized and neutral medium by mass. For our most massive galaxy with ${\rm M_h}\sim10^{11}$M$_{\odot}$, the majority of the CII and OI mass are associated with cold neutral clumps. NII is more diffuse and arises in warmer gas while OIII arises in hotter gas with a higher ionization parameter, produced by photo-heating and supernovae. If smaller pockets of high metallicity gas exist in the ISM, the emission from these ions may be observable by ALMA while the low metallicity of the galaxy may cause these systems to fall below the local [CII]-SFR relation. The presence of dust can cause spatial offsets between UV/Ly$\alpha$ and [CII] emission as suggested by the recent observations of Maiolino et al. [OIII] may be spatially offset from both of these components since it arises from a different part of density-temperature phase-space.
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References
How later papers used it
79 later papers cite it
7 papers by the same authors are listed below: 1 built on it and 7 used its method or tool. 1 of them appears under more than one label.
Builds on it 1 paper · 1 by the same authors
By the same authors
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Followed on from the simulations described in this paper.
A Census of the LyC Photons that Form the UV Background During Reionization (2018) (same authors) · 0.93 · paraphrased: the licence does not allow quoting
Uses its method or tool 7 of 27 papers with this label · 7 by the same authors
By the same authors
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Used the variable speed of light approximation described in this paper to speed up its M1 radiative transfer calculation.
LyC escape from SPHINX galaxies in the Epoch of Reionization (2022) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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Employed exactly the same resolution and refinement strategy as presented for this paper's L14-RT model.
A Census of the LyC Photons that Form the UV Background During Reionization (2018) (same authors) · 0.92 · paraphrased: the licence does not allow quoting
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Employed the variable speed of light approximation of this paper to capture the motion of ionization fronts through the ISM and IGM.
Two Modes of LyC Escape From Bursty Star Formation: Implications for [C II] Deficits and the Sources of Reionization (2022) (same authors) · 0.93 · paraphrased: the licence does not allow quoting
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Computed the ionization and dissociation fractions of seven species as described in another work and this paper.
On the origin of low escape fractions of ionizing radiation from massive star-forming galaxies at high redshift (2020) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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Exploited the variable speed of light approximation presented in this paper, using an AMR level dependent speed of light.
Tracing the Sources of Reionization in Cosmological Radiation Hydrodynamics Simulations (2018) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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Followed the evolution of molecular hydrogen and primordial species by solving the non-equilibrium photo-chemistry described in this paper and another work.
Impact of Lyman alpha pressure on metal-poor dwarf galaxies (2018) (same authors) · 0.95 · paraphrased: the licence does not allow quoting
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Accounted for the non-equilibrium H2 abundance and cooling as in this paper.
RAMSES-RTZ: Non-Equilibrium Metal Chemistry and Cooling Coupled to On-The-Fly Radiation Hydrodynamics (2022) (same authors) · 0.80 · paraphrased: the licence does not allow quoting
How the literature uses it
10 arXiv papers cite this in 11 sentences
Papers citing it · 6 sentences without a confident label
Uses its method or tool 2 papers
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Our simulations include non-equilibrium chemistry of hydrogen and helium (including H$_2$) and solve for the local cooling/heating processes coupled to radiative transfer [ref] .
From short-lived to long-lived clouds: impact of star formation models on giant molecular cloud evolution in simulations of an NGC 300-like galaxy · Radiation-hydrodynamics · 0.97
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We consider eight energy bins, ranging from 0.75 to 1000 eV, to cover the characteristic energies for H$^-$ photodetachment, H$_2$ and H$_2^+$ dissociation, and the different hydrogen and helium ionisation states, following a similar approach to [ref] .
The natural emergence of the correlation between H2 and star formation rate surface densities in galaxy simulations · Chemistry and radiative cooling · 0.99
Compares with it 1 paper
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Our geometry is also akin to that found in [ref] (their Figure 20), in that we have a `filament' of gas falling into a galaxy, with spatially separated and UV/Ly$α$ emission.
Galaxy Formation Through Filamentary Accretion at z=6.1 · Discussion · 0.97
Cites it as background 2 papers
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This is an area in which intensive work is ongoing in terms of faster numerical schemes [ref] , or improved physical modelling [ref] .
The impact of chemistry on the structure of high-z galaxies · Introduction · 0.83
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More details of the photo-chemistry will be presented in [ref] in terms of the prediction of molecular hydrogen in high-z galaxies.
Feedback-regulated star formation and escape of LyC photons from mini-haloes during reionisation · Non-equilibrium photo-chemistry and radiative cooling · 0.80
What it cites · 6 sentences without a confident label
Contests 1 paper
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The [ref] simulations, however, do not include on-the-fly radiative transfer (RT) and therefore do not properly model the enhancement of the local Lyman-Werner background above the mean metagalactic background, inside of the galaxy.
Zooming on the internal structure of $z\simeq6$ galaxies · Introduction · contest 0.73
Uses data or values from 1 paper
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Cosmological parameters reported by the Planck Collaboration are assumed ($h=0.6731$, $Ω_m=0.315$, $Ω_Λ=0.685$, $Ω_Λ=0.049$, $σ_8=0.829$, and $n_s=0.9655$, [ref] ).
Planck 2015 results. XIII. Cosmological parameters · Initial Conditions · 0.99
Compares with 1 paper
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[ref] (hereafter P16) performed a similar exercise using a zoom-in simulation and attempted to model the [CII] emission from a single high-redshift $z=6$ galaxy of similar mass to our work and [ref] .
Zooming on the internal structure of $z\simeq6$ galaxies · Comparison with Previous Simulations · 0.83
Cites as background 5 papers
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Various works have attempted to do this [ref] ; however modelling this emission is complicated.
Molecular clouds photoevaporation and FIR line emission · The Spatial Distribution of CII, NII, OI, and OIII · 0.93
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Various observations targeting the [CII] emission line during the epoch of reionization have been successful [ref] .
Tracing the reionization epoch with ALMA: [CII] emission in z~7 galaxies · Interpreting ALMA Observations · 0.82
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Many theoretical studies have attempted to model the far infrared emission which may emanate from star-forming galaxies, both with a semi-analytic approach [ref] and with numerical simulations [ref] .
Zooming on the internal structure of $z\simeq6$ galaxies · Introduction · 1.00
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