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Approximations for modelling CO chemistry in GMCs: a comparison of approaches
Astrophysics of Galaxies · Submitted 3 Feb 2011
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Nevertheless, the fact that these chemical differences do not appear to have a strong effect on the density or temperature distributions of the gas suggests that the dynamical behaviour of the molecular clouds on large scales is not particularly sensitive to how accurately the small-scale chemistry is modelled.
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The abstract, sentence by sentence
We examine several different simplified approaches for modelling the chemistry of CO in three-dimensional numerical simulations of turbulent molecular clouds. We compare the different models both by looking at the behaviour of integrated quantities such as the mean CO fraction or the cloud-averaged CO-to-H2 conversion factor, and also by studying the detailed distribution of CO as a function of gas density and visual extinction. In addition, we examine the extent to which the density and temperature distributions depend on our choice of chemical model. We find that all of the models predict the same density PDF and also agree very well on the form of the temperature PDF for temperatures T > 30 K, although at lower temperatures, some differences become apparent. All of the models also predict the same CO-to-H2 conversion factor, to within a factor of a few. However, when we look more closely at the details of the CO distribution, we find larger differences. The more complex models tend to produce less CO and more atomic carbon than the simpler models, suggesting that the C/CO ratio may be a useful observational tool for determining which model best fits the observational data. Nevertheless, the fact that these chemical differences do not appear to have a strong effect on the density or temperature distributions of the gas suggests that the dynamical behaviour of the molecular clouds on large scales is not particularly sensitive to how accurately the small-scale chemistry is modelled.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We examine several different simplified approaches for modelling the chemistry of CO in three-dimensional numerical simulations of turbulent molecular clouds. | contribution 0.96 | 0.91 | 0.02 | asserted 0.81 |
| s1 | We compare the different models both by looking at the behaviour of integrated quantities such as the mean CO fraction or the cloud-averaged CO-to-H2 conversion factor, and also by studying the detailed distribution of CO as a function of gas density and visual extinction. | method 0.92 | 0.93 | 0.03 | asserted 0.88 |
| s2 | In addition, we examine the extent to which the density and temperature distributions depend on our choice of chemical model. | contribution 0.61 | 0.87 | 0.03 | unclear 0.78 |
| s3 | We find that all of the models predict the same density PDF and also agree very well on the form of the temperature PDF for temperatures T > 30 K, although at lower temperatures, some differences become apparent. | result 1.00 | 0.96 | 0.12 | asserted 1.00 |
| s4 | All of the models also predict the same CO-to-H2 conversion factor, to within a factor of a few. | result 1.00 | 0.94 | 0.10 | asserted 1.00 |
| s5 | However, when we look more closely at the details of the CO distribution, we find larger differences. | result 0.98 | 0.96 | 0.07 | asserted 1.00 |
| s6 | The more complex models tend to produce less CO and more atomic carbon than the simpler models, suggesting that the C/CO ratio may be a useful observational tool for determining which model best fits the observational data. | result 0.73 | 0.93 | 0.13 | hedged possibility 0.92 |
| s7 | Nevertheless, the fact that these chemical differences do not appear to have a strong effect on the density or temperature distributions of the gas suggests that the dynamical behaviour of the molecular clouds on large scales is not particularly sensitive to how accurately the small-scale chemistry is modelled. | interpretation 1.00 | 0.88 | 0.75 | hedged possibility 0.86 |
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The paper
Original abstract
We examine several different simplified approaches for modelling the chemistry of CO in three-dimensional numerical simulations of turbulent molecular clouds. We compare the different models both by looking at the behaviour of integrated quantities such as the mean CO fraction or the cloud-averaged CO-to-H2 conversion factor, and also by studying the detailed distribution of CO as a function of gas density and visual extinction. In addition, we examine the extent to which the density and temperature distributions depend on our choice of chemical model. We find that all of the models predict the same density PDF and also agree very well on the form of the temperature PDF for temperatures T > 30 K, although at lower temperatures, some differences become apparent. All of the models also predict the same CO-to-H2 conversion factor, to within a factor of a few. However, when we look more closely at the details of the CO distribution, we find larger differences. The more complex models tend to produce less CO and more atomic carbon than the simpler models, suggesting that the C/CO ratio may be a useful observational tool for determining which model best fits the observational data. Nevertheless, the fact that these chemical differences do not appear to have a strong effect on the density or temperature distributions of the gas suggests that the dynamical behaviour of the molecular clouds on large scales is not particularly sensitive to how accurately the small-scale chemistry is modelled.
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References
How later papers used it
67 later papers cite it
10 later papers by other authors are listed below: 10 used its method or tool. 2 more papers by the same authors are listed: 2 used its method or tool.
Uses its method or tool 12 of 42 papers with this label · 2 by the same authors
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Used a time-dependent chemistry network from another work and this paper.
Metallicity dependence of the H/H$_2$ and C$^+$/C/CO distributions in a resolved self-regulating interstellar medium (2021) · 1.00 · paraphrased: the licence does not allow quoting
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Implemented this paper's network including the effects of dust shielding on the rates of all photochemical reactions.
The art of modeling CO, [CI], and [CII] in cosmological galaxy formation models (2018) · 0.98 · paraphrased: the licence does not allow quoting
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Used an implementation of this paper's network that includes reductions in photochemical reaction rates by dust shielding and in H2 and CO dissociation rates by self-shielding and H2 cross shielding.
A physical model for the [CII]-FIR deficit in luminous galaxies (2016) · 1.00 · paraphrased: the licence does not allow quoting
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Adopted a time-dependent chemistry network developed in another work and this paper.
Co-evolution of Dust and Chemistry in Galaxy Simulations with a Resolved Interstellar Medium (2023) · 1.00 · paraphrased: the licence does not allow quoting
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Chemistry and cooling are based on [ref] and [ref] and include time-dependent treatment of hydrogen chemistry.
The GHOSDT Simulations (Galaxy Hydrodynamical Simulations with Supernova-Driven Turbulence) -- I. Magnetic Support in Gas Rich Disks (2024) · ISM Physics and Star Formation · 0.99
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Included time-dependent cooling and H2 chemistry based on another work and this paper.
Dependence of $X_{\rm CO}$ on metallicity, intensity, and spatial scale in a self-regulated interstellar medium (2022) · 1.00 · paraphrased: the licence does not allow quoting
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Based its CO model on those presented in another work and this paper.
PRISM: A Non-Equilibrium, Multiphase Interstellar Medium Model for Radiation Hydrodynamics Simulations of Galaxies (2022) · 0.99 · paraphrased: the licence does not allow quoting
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Following [ref] the “3D” $A_v^3D$ is given by [equation] where $A_v, i$ is the visual extinction along each direction in each of the principal axes of our numerical grid.
Projection-angle effects when "observing" a turbulent magnetized collapsing molecular cloud. I. Chemistry and line transfer (2025) · Chemical modeling · 1.00
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Assumed solar metallicity for its atomic and molecular cooling functions and followed the models by another work and this paper.
The in situ formation of molecular and warm ionised gas triggered by hot outflows (2021) · 0.92 · paraphrased: the licence does not allow quoting
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Dust temperature is computed by the NL97 chemical network based on the radiative cooling of dust in thermal equilibrium [ref] .
IRIS: Deciphering Spectral-Line Imagery of the Galactic Center by Machine-Learning on Simulations (2026) · Tensor Variables and Gas Temperature · 0.98
By the same authors
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Took the maximum of the X-ray irradiated dust temperature and the radiative equilibrium temperature resulting from FUV irradiation from this paper.
Non-Equilibrium Chemistry and Destruction of CO by X-ray Flares (2018) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
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The thermodynamics of the gas and dust are treated according to [ref] and [ref] ; this represents a largely complete account of all important processes, including radiative heating and cooling, cosmic rays, dust-gas thermal coupling, and the energy liberated by exothermic chemical reactions.
Non-Equilibrium Abundances Treated Holistically (NEATH): the molecular composition of star-forming clouds (2023) (same authors) · Magnetohydrodynamical model · 0.99
How the literature uses it
9 arXiv papers cite this in 18 sentences
Papers citing it · 7 sentences without a confident label
Uses its method or tool 5 papers
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Our modifications include a sink particle algorithm for treating gravitationally collapsing regions that become to small to resolve [ref] , the inclusion into the equation of motion of an optional confining pressure term [ref] , a treatment of gas-phase chemistry (described in more detail below), as well as radiative heating and cooling from a number of atomic and molecular species [ref] , and an approximate treatment of the attenuation of the Galactic interstellar radiation field (ISRF).
Is molecular gas necessary for star formation? · Numerical approach · 1.00
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These are used as inputs for the atomic and molecular heating and cooling function described in [ref] , where a detailed description of the included processes can be found in [ref] , with later modifications made by [ref] and [ref] .
The diffuse gamma-ray sky of a Milky Way analogue: Local diversity and global constraints · Simulation setup · 0.87
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Dust temperature is computed by the NL97 chemical network based on the radiative cooling of dust in thermal equilibrium [ref] .
IRIS: Deciphering Spectral-Line Imagery of the Galactic Center by Machine-Learning on Simulations · Tensor Variables and Gas Temperature · 0.98
Cites it as support 1 paper
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However, we know from previous work [ref] that the behaviour of the gas is not particularly sensitive to whether the dominant coolant is C$^+$ or CO.
Modeling H2 formation in the turbulent ISM: Solenoidal versus compressive turbulent forcing · Chemistry and cooling · 0.97
Cites it as background 1 paper
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For a more detailed treatment, see e.g. [ref] .] [equation] Here $Γ_ext$ is the dust heating rate per unit volume due to absorption of radiation from the ISRF and $Λ_dust$ is the radiative cooling rate of the dust.
TreeCol: a novel approach to estimating column densities in astrophysical simulations · Dust heated by the interstellar radiation field · 0.89
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