2010
DOI: 10.1051/0004-6361/201014536
|View full text |Cite
|
Sign up to set email alerts
|

Mapping the interstellar medium in galaxies withHerschel/SPIRE

Abstract: The standard method of mapping the interstellar medium in a galaxy, by observing the molecular gas in the CO 1-0 line and the atomic gas in the 21-cm line, is largely limited with current telescopes to galaxies in the nearby universe. In this letter, we use SPIRE observations of the galaxies M 99 and M 100 to explore the alternative approach of mapping the interstellar medium using the continuum emission from the dust. We have compared the methods by measuring the relationship between the star-formation rate a… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
23
0

Year Published

2011
2011
2024
2024

Publication Types

Select...
8

Relationship

4
4

Authors

Journals

citations
Cited by 38 publications
(23 citation statements)
references
References 27 publications
0
23
0
Order By: Relevance
“…A measurement of κ at Herschel wavelengths (but for local normal galaxies) has been attempted by Weibe et al (2009) andEales et al (2010b). Both works, however, suggest a much lower value for κ, which would increase the dust masses estimated here by a factor of ∼3.…”
Section: Final Caveatmentioning
confidence: 93%
See 1 more Smart Citation
“…A measurement of κ at Herschel wavelengths (but for local normal galaxies) has been attempted by Weibe et al (2009) andEales et al (2010b). Both works, however, suggest a much lower value for κ, which would increase the dust masses estimated here by a factor of ∼3.…”
Section: Final Caveatmentioning
confidence: 93%
“…Dust emission is often used as an indicator of the current star formation rate (SFR) in galaxies -although this calibration makes the assumption that young, massive stars are the main source of heating for the dust and that the majority of the UV photons from the young stars are absorbed and re-radiated by dust (Kennicutt 1998;Kennicutt et al 2009;Calzetti et al 2007). Many surveys of dust emission from 24 to 850 μm (Saunders et al 1990;Blain et al 1999;Le Floc'h et al 2005;Dye et al 2010;Eales et al 2010b;Gruppioni et al 2010) have noted the very strong evolution present in these bands and this is usually ascribed to a decrease in the SFR density over the past 8 billion years of cosmic history (z ∼ 1; Madau et al 1995;Hopkins 2004). The interpretation of this evolution is complicated by the fact that the dust luminosity of a galaxy is a function of both the dust content and the temperature of the dust.…”
Section: Introductionmentioning
confidence: 99%
“…The total gas mass (M gas , which incorporates both the molecular and atomic phases) can be inferred from the dust mass through the metallicity dependent gas-to-dust ratio (GDR, e.g. Eales et al 2010;Magdis et al 2012a): M gas = M dust /GDR(Z). For consistency with M gas estimates of SBs in the literature, we adopt GDR ≈ 30, that based on Magdis et al (2012a) corresponds to a CO-to-M gas α co conversion factor of 0.8 M / (K km s −1 pc 2 ), typically used for strong starbursts.…”
Section: Dust and Molecular Gas Massesmentioning
confidence: 99%
“…Luminosity functions based on observations at 250, 350 and 500 μm from the recent Balloon-borne Large Aperture Submillimeter Telescope (BLAST) survey centred on the GOODS-South field have shown a strong increase in the number density of the most luminous galaxies from the present out to z = 1 (Eales et al 2009). Two recent papers have presented luminosity functions using observations at 250 μm from the science demonstration phase of the Herschel Space Telescope: Dye et al (2010) used data from a 14 deg 2 field out to z = 0.5, showing steady evolution out to this redshift and Eales et al (2010) in two smaller but deeper fields to z = 2.0 found strong evolution out to z ∼ 1 but at most weak evolution beyond this redshift.…”
mentioning
confidence: 99%