REVIEW
350 Micron Dust Emission from High Redshift Quasars
Astrophysics · Submitted 6 Mar 2006 · 45 references
Pith's verdict: Solid new 350 micron detections double the high-z quasar sample, but the paper's abstract overstates the temperature range and the beta-fixed individual fits carry a systematic caveat that needs airing.
T0 · AI review
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Referee report
The paper
The paper claims
High-redshift quasars share a warm dust component at 47 K, six new 350-micron detections show.
The reading
What carries the argument
The load-bearing model is a single-temperature, optically thin modified blackbody (greybody), with flux density proportional to ν^(3+β)/(exp(hν/kT)-1). Because temperature and emissivity index are degenerate when only two photometric points are available, the authors fix β = 1.6 from a combined fit to all quasars with two or more far-infrared measurements, then derive individual temperatures from the degeneracy equation (Eq. 3). The 350-micron band is the key observable: for z ≈ 2–6 it samples the rest-frame peak of the warm dust emission, anchoring each object's SED and luminosity estimate. The far-infrared/radio ratio q, defined following Condon (1992), is used to compare the quasars with local star-forming galaxies.
Extended reading notes
Core claim
The central discovery is that the warm dust component of high-redshift quasars is uniform: the mean rest-frame far-infrared SED of 14 quasars, built from photometry that now includes the six new 350-micron measurements, is best fit by a single-temperature modified blackbody with T = 47 ± 3 K and β = 1.6 ± 0.1. Individual sources have derived temperatures between 40 and 60 K and far-infrared luminosities of 0.6 to 2.2 × $10^{13}$ L_sun, with the new 350-micron points sampling near the peak of the redshifted emission. The paper further shows that these quasars obey the same far-infrared/radio correlation as local star-forming galaxies (median q = 2.2 ± 0.4), and that the derived warm dust temperatures are not strongly affected by a hotter AGN-heated component, supporting the conclusion that the far-infrared light is powered by star formation.
Load-bearing premise
For four of the six sources, the dust temperature is derived from only two far-infrared photometric points with the emissivity index fixed to β = 1.6, a value obtained from a combined fit to a sample that includes these same objects; if the true emissivity index differs, the derived temperatures, luminosities, and q values shift accordingly.
Editorial extensions
If this is right
- At z ≈ 2–6, 350-micron photometry sits near the rest-frame peak of warm dust emission, so these measurements sharply reduce uncertainties in far-infrared luminosities and implied star formation rates.
- The mean SED with T = 47 K and β = 1.6 can serve as a fixed template for estimating luminosities of high-redshift quasars from just one or two submillimeter flux measurements.
- Because the quasars follow the local far-infrared/radio correlation, radio observations can be used as a relatively inexpensive star-formation indicator for radio-quiet high-redshift quasars.
- Observations at 2–3 mm (rest-frame Rayleigh-Jeans tail) would constrain β independently and test for the presence of a cold dust component that the current single-temperature model cannot exclude.
Reading between the lines
- If the roughly 47 K dust temperature is universal among luminous high-z quasars, then photometric redshift estimates from far-infrared/submillimeter colors are conceivable, though the β–T degeneracy will limit their precision.
- A direct test of the starburst-heating picture would be to resolve the spatial extent of the 350-micron emission in these quasars; compact AGN-heated dust would be unresolved, while kpc-scale emission would match the molecular gas reservoirs already mapped in CO.
- The paper's individual temperature estimates for four sources rest on a β fixed from a sample that includes those very sources; an independent determination of β for any one object would check the circularity.
Original abstract
We report detections of six high-redshift (1.8 < z < 6.4), optically luminous, radio-quiet quasars at 350 micron, using the SHARC II bolometer camera at the Caltech Submillimeter Observatory. Our observations double the number of high-redshift quasars for which 350 micron photometry is available. By combining the 350 micron measurements with observations at other submillimeter/millimeter wavelengths, for each source we have determined the temperature of the emitting dust (ranging from 40 to 60 K) and the far-infrared luminosity (0.6 to 2.2 x 10(13) Lo). The combined mean spectral energy distribution (SED) of all high-redshift quasars with two or more rest frame far-infrared photometric measurements is best fit with a greybody with temperature of 47 +- 3 K and a dust emissivity power-law spectral index of beta = 1.6 +- 0.1. This warm dust component is a good tracer of the starburst activity of the quasar host galaxy. The ratio of the far-infrared to radio luminosities of infrared luminous, radio-quiet high-redshift quasars is consistent with that found for local star-forming galaxies.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
We report detections of six high-redshift (1.8 < z < 6.4), optically luminous, radio-quiet quasars at 350 micron, using the SHARC II bolometer camera at the Caltech Submillimeter Observatory. Our observations double the number of high-redshift quasars for which 350 micron photometry is available. By combining the 350 micron measurements with observations at other submillimeter/millimeter wavelengths, for each source we have determined the temperature of the emitting dust (ranging from 40 to 60 K) and the far-infrared luminosity (0.6 to 2.2 x 10(13) Lo). The combined mean spectral energy distribution (SED) of all high-redshift quasars with two or more rest frame far-infrared photometric measurements is best fit with a greybody with temperature of 47 +- 3 K and a dust emissivity power-law spectral index of beta = 1.6 +- 0.1. This warm dust component is a good tracer of the starburst activity of the quasar host galaxy. The ratio of the far-infrared to radio luminosities of infrared luminous, radio-quiet high-redshift quasars is consistent with that found for local star-forming galaxies.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We report detections of six high-redshift (1.8 < z < 6.4), optically luminous, radio-quiet quasars at 350 micron, using the SHARC II bolometer camera at the Caltech Submillimeter Observatory. | contribution 0.75 | 0.97 | 0.12 | asserted 1.00 |
| s1 | Our observations double the number of high-redshift quasars for which 350 micron photometry is available. | result 0.50 | 0.84 | 0.11 | asserted 1.00 |
| s2 | By combining the 350 micron measurements with observations at other submillimeter/millimeter wavelengths, for each source we have determined the temperature of the emitting dust (ranging from 40 to 60 K) and the far-infrared luminosity (0.6 to 2.2 x 10(13) Lo). | result 0.89 | 0.97 | 0.14 | asserted 1.00 |
| s3 | The combined mean spectral energy distribution (SED) of all high-redshift quasars with two or more rest frame far-infrared photometric measurements is best fit with a greybody with temperature of 47 +- 3 K and a dust emissivity power-law spectral index of beta = 1.6 +- 0.1. | result 1.00 | 0.90 | 0.34 | asserted 1.00 |
| s4 | This warm dust component is a good tracer of the starburst activity of the quasar host galaxy. | interpretation 1.00 | 0.43 | 0.25 | asserted 0.97 |
| s5 | The ratio of the far-infrared to radio luminosities of infrared luminous, radio-quiet high-redshift quasars is consistent with that found for local star-forming galaxies. | result 0.71 | 0.81 | 0.21 | hedged possibility 0.89 |
What was examined, and what was not
- arXiv listing abstract v1
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
Figures
Figures reproduced from arXiv:astro-ph/0603121 by the authors.
References
How later papers used it
51 later papers cite it
5 later papers by other authors are listed below: 2 used its method or tool, 1 used its data or values and 2 compared their own results with it. 2 more papers by the same authors are listed: 1 used its method or tool and 1 cited it as support.
Uses its method or tool 3 of 7 papers with this label · 1 by the same authors
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Estimated its far-infrared luminosities from observed 870 micron and 1200 micron flux densities using equations 1 and 4 of this paper.
The nature of sub-millimetre galaxies II: an ALMA comparison of SMG dust heating mechanisms (2021) · 1.00 · paraphrased: the licence does not allow quoting
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Following [ref] and [ref] , the FIR flux density is expressed as:
A Quasar--Companion System Without AGN Outflow at $z \sim 6$: The Case of PSO J083+11 (2026) · FIR Emission Fitting · 1.00
By the same authors
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Assumed optically thin dust emission at wavelengths above 40 microns as in this paper and used a modified black body model for the dust emission.
Physical constraints on the extended interstellar medium of the z=6.42 quasar J1148+5251: [CII] 158um, [NII] 205um and [OI] 146um observations (2022) (same authors) · 1.00 · paraphrased: the licence does not allow quoting
Uses its data or values 1 of 7 papers with this label
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Here, we consider values for dust temperature and $β$ typically used in the literature, i.e. $T_dust = 47 K$ and $β= 1.6$ (e.g. [ref] , [ref] , [ref] ).
The host galaxies of radio-loud quasars at z>5 with ALMA (2024) · IR and luminosities, Star Formation Rates and Dust Masses · 0.86
Compares with it 2 of 6 papers with this label
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In the previous section, we demonstrated that the dust temperature shows a steep increase up to $∼$ 57K, which is much higher than the typical dust temperature assumed for quasar hosts [ref] and is presumably due to the heated dust by the central AGN.
Spatially resolved dust properties and quasar-galaxy decomposition of a HyLIRG at z = 4.4 (2023) · Image decomposition of Band 7 and Band 9 continuum images · 0.83
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Found its own effective temperatures with statistical uncertainties lie within the range of 350 micron-derived dust temperatures for high redshift radio quiet quasars from this paper.
Quantifying the Thermal Sunyaev-Zel'dovich Effect and Excess Millimeter Emission in Quasar Environments (2019) · 0.98 · paraphrased: the licence does not allow quoting
Cites it as support 1 paper · 1 by the same authors
By the same authors
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Said its conditions are physically motivated based on previous results of this paper and another work.
Constraining the Active Galactic Nucleus and Starburst Properties of the IR-luminous Quasar Host Galaxy APM 08279+5255 at Redshift 4 with SOFIA (2019) (same authors) · 0.97 · paraphrased: the licence does not allow quoting
How the literature uses it
4 arXiv papers cite this in 5 sentences
Papers citing it · 4 sentences without a confident label
Uses its data or values 1 paper
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In the following we estimate whether the derived dust productivities may be sufficient to account for the 2–7 $×$ 10$^8$ $$ of dust inferred in QSOs at $z ≥6$ [ref] .
Production of dust by massive stars at high redshift · An example · 0.97
Discussion
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