2005
DOI: 10.1111/j.1365-2966.2005.09044.x
|View full text |Cite
|
Sign up to set email alerts
|

New insights into the dust properties of the Taurus molecular cloud TMC-2 and its surroundings

Abstract: We present ISOPHOT observations at 120 and 200 μm of a 31 × 57 arcmin2 region, with optical extinction AV ranging between ≈ 0.5 and 11 mag, that encloses the Taurus molecular cloud TMC‐2. The far‐infrared emission is separated into a warm and a cold component using the ISOPHOT data and IRAS measurements at 60 and 100 μm. This separation is based on the very different morphologies of the 60 and 200 μm emission maps. The 60 μm emission is used as a spatial template for the warm component, and the 200 μm emission… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

2
15
0

Year Published

2005
2005
2012
2012

Publication Types

Select...
7
1

Relationship

1
7

Authors

Journals

citations
Cited by 21 publications
(17 citation statements)
references
References 27 publications
2
15
0
Order By: Relevance
“…Variations in dust's optical properties are visible even on a scale of the galactic anticentre hemisphere, anywhere where A V > ∼ 1 mag (Cambresy et al 2005). Del Burgo & Laureijs (2005) used observations of the Taurus molecular cloud TMC-2 between 60 µm and 200 µm to separate the emission into cold and warm components. They found that far-IR emissivity of the cold component is a few times larger than that of the diffuse interstellar medium, and that the change in the properties of the big dust particles takes place at intermediate densities of n(H 2 ) ≈ 10 3 cm −3 .…”
Section: Introductionmentioning
confidence: 99%
“…Variations in dust's optical properties are visible even on a scale of the galactic anticentre hemisphere, anywhere where A V > ∼ 1 mag (Cambresy et al 2005). Del Burgo & Laureijs (2005) used observations of the Taurus molecular cloud TMC-2 between 60 µm and 200 µm to separate the emission into cold and warm components. They found that far-IR emissivity of the cold component is a few times larger than that of the diffuse interstellar medium, and that the change in the properties of the big dust particles takes place at intermediate densities of n(H 2 ) ≈ 10 3 cm −3 .…”
Section: Introductionmentioning
confidence: 99%
“…The diffuse ISM component has a typical temperature of about 17.5 K (Boulanger et al 1996) while the colder condensation component has a typical temperature of about 12.5 K (del Burgo & Laureijs 2005). Observations with ISO, Spitzer, SPM/PRONAOS and IRAS of different regions in the interstellar medium indicate increased dust emissivities in colder regions (Bernard et al 1999;del Burgo et al 2003;Stepnik et al 2003;del Burgo & Laureijs 2005;Kiss et al 2006;Ridderstad et al 2006;Lehtinen et al 2007;Bot et al 2009;Paradis et al 2009). This increase in emissivity observed at wavelengths ≥200 μm is often explained by a change in the properties of the cold dust.…”
Section: Introductionmentioning
confidence: 99%
“…Lagache et al 1998;Bernard et al 1999;Stepnik et al 2003;del Burgo et al 2003;Planck Collaboration 2011b). Additionally, an increase in the dust opacity by a factor between 2 and 4 is observed in these denser regions at long wavelengths, which is inferred from the low dust temperature, and not always by comparison to the gas or A V (Bernard et al 1999;Hotzel et al 2001;Cambrésy et al 2001;Stepnik et al 2003;Bianchi et al 2003;del Burgo et al 2003;del Burgo & Laureijs 2005;Kiss et al 2006;Lehtinen et al 2007;Ridderstad et al 2006;Bot et al 2009;Paradis et al 2009;Planck Collaboration 2011b). Moreover, the abundance of the very small grains (VSGs, 1−15 nm in radius), that are stochastically heated and responsible for the 60 μm emission, decreases by ∼80-100% in the transition from diffuse to dense molecular clouds (Laureijs et al 1991;Abergel et al 1994Abergel et al , 1996Lagache et al 1998;Stepnik et al 2003;Kramer et al 2003).…”
Section: Introductionmentioning
confidence: 99%