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The Molecular Interstellar Medium in Ultraluminous Infrared Galaxies
Astrophysics · Submitted 21 Oct 1996
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A collision involving a molecular gas rich spiral could lead to an ultraluminous galaxy powered by central starbursts triggered by the compression of infalling preexisting GMC's.
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The abstract, sentence by sentence
We present CO observations of a large sample of ultraluminous IR galaxies out to z = 0.3. Most of the galaxies are interacting, but not completed mergers. All but one have high CO(1-0) luminosities, log(Lco [K-km/s-pc^2]) = 9.92 +/- 0.12. The dispersion in Lco is only 30%, less than that in the FIR luminosity. The integrated CO intensity correlates Strongly with the 100 micron flux density, as expected for a black body model in which the mid and far IR radiation are optically thick. We use this model to derive sizes of the FIR and CO emitting regions and the enclosed dynamical masses. Both the IR and CO emission originate in regions a few hundred parsecs in radius. The median value of Lfir/Lco = 160 Lsun/(K-km/s-pc^2), within a factor of two of the black body limit for the observed FIR temperatures. The entire ISM is a scaled up version of a normal galactic disk with densities a factor of 100 higher, making even the intercloud medium a molecular region. Using three different techniques of H2 mass estimation, we conclude that the ratio of gas mass to Lco is about a factor of four lower than for Galactic molecular clouds, but that the gas mass is a large fraction of the dynamical mass. Our analysis of CO emission reduces the H2 mass from previous estimates of 2-5e10 Msun to 0.4-1.5e10 Msun, which is in the range found for molecular gas rich spiral galaxies. A collision involving a molecular gas rich spiral could lead to an ultraluminous galaxy powered by central starbursts triggered by the compression of infalling preexisting GMC's.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We present CO observations of a large sample of ultraluminous IR galaxies out to z = 0.3. | contribution 0.95 | 0.96 | 0.03 | asserted 0.99 |
| s1 | Most of the galaxies are interacting, but not completed mergers. | result 0.78 | 0.74 | 0.03 | asserted 1.00 |
| s2 | All but one have high CO(1-0) luminosities, log(Lco [K-km/s-pc^2]) = 9.92 +/- 0.12. | result 1.00 | 0.94 | 0.09 | asserted 1.00 |
| s3 | The dispersion in Lco is only 30%, less than that in the FIR luminosity. | result 1.00 | 0.92 | 0.06 | asserted 1.00 |
| s4 | The integrated CO intensity correlates Strongly with the 100 micron flux density, as expected for a black body model in which the mid and far IR radiation are optically thick. | result 0.88 | 0.86 | 0.11 | asserted 0.98 |
| s5 | We use this model to derive sizes of the FIR and CO emitting regions and the enclosed dynamical masses. | method 0.98 | 0.95 | 0.05 | asserted 0.97 |
| s6 | Both the IR and CO emission originate in regions a few hundred parsecs in radius. | result 1.00 | 0.93 | 0.09 | asserted 1.00 |
| s7 | The median value of Lfir/Lco = 160 Lsun/(K-km/s-pc^2), within a factor of two of the black body limit for the observed FIR temperatures. | result 0.98 | 0.93 | 0.13 | asserted 1.00 |
| s8 | The entire ISM is a scaled up version of a normal galactic disk with densities a factor of 100 higher, making even the intercloud medium a molecular region. | interpretation 0.87 | 0.77 | 0.27 | asserted 1.00 |
| s9 | Using three different techniques of H2 mass estimation, we conclude that the ratio of gas mass to Lco is about a factor of four lower than for Galactic molecular clouds, but that the gas mass is a large fraction of the dynamical mass. | result 0.99 | 0.95 | 0.25 | asserted 0.99 |
| s10 | Our analysis of CO emission reduces the H2 mass from previous estimates of 2-5e10 Msun to 0.4-1.5e10 Msun, which is in the range found for molecular gas rich spiral galaxies. | result 0.99 | 0.91 | 0.26 | asserted 1.00 |
| s11 | A collision involving a molecular gas rich spiral could lead to an ultraluminous galaxy powered by central starbursts triggered by the compression of infalling preexisting GMC's. | interpretation 1.00 | 0.29 | 0.31 | hedged possibility 1.00 |
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The paper
Original abstract
We present CO observations of a large sample of ultraluminous IR galaxies out to z = 0.3. Most of the galaxies are interacting, but not completed mergers. All but one have high CO(1-0) luminosities, log(Lco [K-km/s-pc^2]) = 9.92 +/- 0.12. The dispersion in Lco is only 30%, less than that in the FIR luminosity. The integrated CO intensity correlates Strongly with the 100 micron flux density, as expected for a black body model in which the mid and far IR radiation are optically thick. We use this model to derive sizes of the FIR and CO emitting regions and the enclosed dynamical masses. Both the IR and CO emission originate in regions a few hundred parsecs in radius. The median value of Lfir/Lco = 160 Lsun/(K-km/s-pc^2), within a factor of two of the black body limit for the observed FIR temperatures. The entire ISM is a scaled up version of a normal galactic disk with densities a factor of 100 higher, making even the intercloud medium a molecular region. Using three different techniques of H2 mass estimation, we conclude that the ratio of gas mass to Lco is about a factor of four lower than for Galactic molecular clouds, but that the gas mass is a large fraction of the dynamical mass. Our analysis of CO emission reduces the H2 mass from previous estimates of 2-5e10 Msun to 0.4-1.5e10 Msun, which is in the range found for molecular gas rich spiral galaxies. A collision involving a molecular gas rich spiral could lead to an ultraluminous galaxy powered by central starbursts triggered by the compression of infalling preexisting GMC's.
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References
How later papers used it
79 later papers cite it
25 later papers by other authors are listed below: 24 used its method or tool and 1 used its data or values.
Uses its method or tool 24 of 44 papers with this label
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Following [ref] , we estimate the CO line luminosity, $L'_CO$ (in K km s$^-1$ pc$^2$), from the Gaussian fitting results using: [equation] where $S_CO,tot$ is the total CO line flux (in Jy km s$^-1$).
From Starburst to Quenching: Physical Properties of Extremely Compact Starbursts at z$\sim$0.1 (2026) · Data Reduction · 1.00
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Calculated the CO(1-0) line luminosity using this paper's equation 3.
Total Molecular Gas Masses of Planck - Herschel Selected Strongly Lensed Hyper Luminous Infrared Galaxies (2017) · 1.00 · paraphrased: the licence does not allow quoting
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Converted CO line measurements into CO luminosities following this paper's methodology.
The Molecular-Gas Main Sequence and Schmidt-Kennicutt relation are fundamental, the Star-Forming Main Sequence is a (useful) byproduct (2022) · 1.00 · paraphrased: the licence does not allow quoting
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From the line intensity ($I_CO$ in $K km/s pc^2$)[$I_CO$ and $L^'_CO$ are computed assuming the main-beam temperature $T_mb = 1.33T_A^*$ on <https://www.iram.fr/IRAMFR/ARN/jan95/node46.html>.] we calculate the CO line luminosity $L^'_CO$ (in $K km/s pc^2$) following [ref] [equation] where $z$ is the redshift from [ref] and $D_L$ is the corresponding luminosity distance in Mpc. $Ω_s*b$ is the solid angle of the source convolved with the beam: [equation] where $θ_s$ and $θ_b$ are the half-power beam widths of the source and beam, respectively.
Measuring the ISM Content of Nearby, Luminous, Type 1 and Type 2 QSOs through CO and [C II] (2024) · IRAM CO Observations and Data Reduction · 0.96
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Estimated molecular gas masses from integrated CO fluxes using this paper's standard luminosity relation.
Cold molecular gas distribution and kinematics in the low-metallicity dusty starburst of Mrk 996 resolved with ALMA (2026) · 1.00 · paraphrased: the licence does not allow quoting
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Evaluated line luminosities using this paper's standard relation.
[NII] fine-structure emission at 122 and 205um in a galaxy at z=2.6: a globally dense star-forming interstellar medium (2020) · 1.00 · paraphrased: the licence does not allow quoting
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Defined its brightness temperature luminosity using the same L' as defined in this paper.
A Molecular gas rich GRB host galaxy at the peak of cosmic star formation (2017) · 0.99 · paraphrased: the licence does not allow quoting
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Converted the line strength into units of L'_CO(3-2) using this paper's equation.
The SCUBA-2 Web Survey: I. Observations of CO(3-2) in hyper-luminous QSO fields (2018) · 0.98 · paraphrased: the licence does not allow quoting
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Used this paper's equation to calculate CO(1-0) luminosity from the measured CO flux.
Dust and Cold Gas Properties of Starburst HyLIRG-Quasars at $z \sim 2.5$ (2024) · 1.00 · paraphrased: the licence does not allow quoting
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For our sample, as well as for the data from other works, we estimated the luminosity using the same prescription – equation 3 in [ref] .
Main Sequence to Starburst Transitioning Galaxies: Gamma-ray Burst Hosts at $z\sim2$ (2023) · Flux, Luminosity and Mass Measurements · 1.00
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We derived the line luminosities $L^'_dense$ for each position following [ref] : [equation] where $SΔv$ is the velocity-integrated flux density, $ν_obs$ is the observed line frequency, and $D_L$ is the luminosity distance.
Sub-kiloparsec scaling relations between hot gas, dense gas and star formation rate in five nearby star-forming galaxies (2024) · JCMT HCN (4$-$3) and HCO$^+$(4$-$3) Data · 1.00
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Translated the total flux into a luminosity using this paper's relation.
Cold molecular gas outflow encasing the ionised one in the Seyfert galaxy NGC 3281 (2023) · 0.92 · paraphrased: the licence does not allow quoting
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Calculated CO luminosities for each source using this paper's equation.
High molecular gas content and star formation rates in local galaxies that host quasars, outflows and jets (2020) · 0.99 · paraphrased: the licence does not allow quoting
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Applied all the standard factors from this paper's prescription when stacking in gas fraction units.
Molecular and atomic gas along and across the main sequence of star-forming galaxies (2016) · 1.00 · paraphrased: the licence does not allow quoting
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Estimated the total CO line luminosity using equation 3 of this paper.
Searching for signs of jet-driven negative feedback in the nearby radio galaxy UGC 05771 (2019) · 1.00 · paraphrased: the licence does not allow quoting
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We then convert the total fluxes to luminosities ($L'$; K km s$^-1$ pc$^2$) using equation 3 in [ref] .
CO Excitation in High-z Main Sequence Analogues: Resolved CO(4-3)/CO(3-2) Line Ratios in DYNAMO Galaxies (2023) · Relating High$-$J CO to CO(1$-$0) · 0.97
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Derived the luminosity from the integrated flux of the emission line using the same method as this paper.
Cold Molecular Gas and Free-Free Emission from Hot, Dust-Obscured Galaxies at $z$~3 (2020) · 1.00 · paraphrased: the licence does not allow quoting
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Derived line luminosities using equations given in another work and this paper.
An ALMA multi-line survey of the interstellar medium of the redshift 7.5 quasar host galaxy J1342+0928 (2019) · 1.00 · paraphrased: the licence does not allow quoting
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Converted CO(3-2) flux density to integrated line luminosity using this paper's equation.
Unveiling the Main Sequence to Starburst Transition Region with a Sample of Intermediate Redshift Luminous Infrared Galaxies (2022) · 1.00 · paraphrased: the licence does not allow quoting
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We can then follow the procedure in [ref] to obtain a CO line luminosity (in units of brightness temperature) using
ALMA-JELLY I: High Resolution CO(2-1) Observations of Ongoing Ram Pressure Stripping in NGC 4858 Reveal Asymmetrical Gas Tail Formation and Fallback (2025) · ALMA CO(2-1) · 1.00
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Converted its CO(3-2) line luminosity into line intensity using equation 2 from this paper.
JINGLE, a JCMT legacy survey of dust and gas for galaxy evolution studies: II. SCUBA-2 850 {\mu}m data reduction and dust flux density catalogues (2019) · 1.00 · paraphrased: the licence does not allow quoting
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Calculated line luminosities from velocity integrated line flux densities using this paper's equation.
Molecular Line Observations in Two Dusty Star-Forming Galaxies at z = 6.9 (2021) · 1.00 · paraphrased: the licence does not allow quoting
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Converted the CO flux into a CO luminosity following this paper's process to determine molecular gas mass.
The ALMaQUEST Survey IX: The nature of the resolved star forming main sequence (2022) · 1.00 · paraphrased: the licence does not allow quoting
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Followed this paper to calculate the line luminosity in each voxel.
COMAP Early Science: VIII. A Joint Stacking Analysis with eBOSS Quasars (2023) · 1.00 · paraphrased: the licence does not allow quoting
Uses its data or values 1 of 8 papers with this label
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Compiled CO data for 56 local LIRGs and ULIRGs from another work, this paper and another work.
The EGNoG Survey: Molecular Gas in Intermediate-Redshift Star-Forming Galaxies (2013) · 1.00 · paraphrased: the licence does not allow quoting
How the literature uses it
5 arXiv papers cite this in 6 sentences
Papers citing it
Uses its method or tool 5 papers
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The molecular gas mass ($M_mol$) is derived from the CO luminosity $L'_CO(1-0)$ [ref] : [equation] where the factor 1.36 accounts for helium.
From Starburst to Quenching: Physical Properties of Extremely Compact Starbursts at z$\sim$0.1 · Data Reduction · 0.97
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We estimated molecular gas masses from the integrated CO fluxes using the standard luminosity relation from [ref] , [equation] in K km s$^-1$ pc$^2$, where $S_lineΔv$ is the integrated flux in Jy km s$^-1$, $D_L$ the luminosity distance (Mpc), and $ν_obs$ the observed frequency (GHz).
Cold molecular gas distribution and kinematics in the low-metallicity dusty starburst of Mrk 996 resolved with ALMA · Molecular gas estimations · 1.00
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In order to compute the molecular mass from the integrated CO flux density, we adopted equation (3) of [ref] : [equation] with the line luminosity $L^'_CO$ expressed in K km s$^-1$ pc$^-2$, $S_CO ΔV$ being the velocity-integrated line flux in Jy km s$^-1$, $D_L$ the luminosity distance in Mpc, $ν_obs$ the redshifted frequency in GHz and $z$ the redshift.
Resolved molecular gas and star-formation in massive unquenched spirals : I. UGC 8179 · Mapped molecular gas mass · 1.00
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