2011
DOI: 10.1051/0004-6361/201014260
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Interstellar H2toward HD 37903

Abstract: We present an analysis of interstellar H 2 toward HD 37903, which is a hot B 1.5 V star located in the NGC 2023 reflection nebula. Meyer et al. (2001, ApJ, 553, L59) used a rich spectrum of vibrationally excited H 2 observed by the HST to calculate a model of the interstellar cloud toward HD 37903. We extend their analysis by including the ν = 0 vibrational level observed by the FUSE satellite. The temperature calculated from the two lowest rotational levels (J = 0, 1) of the H 2 molecule should not be interpr… Show more

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Cited by 17 publications
(28 citation statements)
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“…Gerin et al (2015) have used the 158 µm [C ii] absorption spectra observed by HIFI towards a few se- lected Galactic objects to derive the thermal pressure in the diffuse ISM. In the solar neighborhood (∼1 kpc) measurements of the thermal gas pressure have been made with C i UV absorption spectra towards a sample of about 89 selected target stars (Jenkins et al 1983;Jenkins & Tripp 2001, 2011 and CO UV absorption towards 76 stars (Goldsmith 2013).…”
mentioning
confidence: 99%
“…Gerin et al (2015) have used the 158 µm [C ii] absorption spectra observed by HIFI towards a few se- lected Galactic objects to derive the thermal pressure in the diffuse ISM. In the solar neighborhood (∼1 kpc) measurements of the thermal gas pressure have been made with C i UV absorption spectra towards a sample of about 89 selected target stars (Jenkins et al 1983;Jenkins & Tripp 2001, 2011 and CO UV absorption towards 76 stars (Goldsmith 2013).…”
mentioning
confidence: 99%
“…The excellent agreement with the Boltzmann distribution confirms the correctness of the H 2 column densities. For the sightline towards HD 37903, the rotational temperatures fall with increased vibrational number ν (Gnaciński 2011). This behavior is not observed towards HD 147888.…”
Section: Ortho To Para H 2 and Temperaturesmentioning
confidence: 97%
“…The H 2 in the cloud towards HD 147888 does not satisfy this equation because 1.13 √ 0.15 = 0.39. Also the cloud toward HD 37903 (see Gnaciński 2011 for O/P H 2 values) does not satisfy the (O/P)* = √ (O/P) J=1 equation. One of the reasons for the discrepancy is that the bulk of H 2 * and H 2 (J = 0,1) are located in different parts of the cloud, so the column densities ratio of H 2 * and H 2 (J = 0,1) are not equal to the local density ratio.…”
Section: Ortho To Para H 2 and Temperaturesmentioning
confidence: 99%
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“…(1) are appropriate for diatomic systems, but can be generalized for polyatomic ones. All the above processes drive the particle densities in fusion plasmas close to the walls and in the divertor region [5][6][7][8], in various media of astrophysical interest [9][10][11][12], in the hypersonic entry plasmas [13], and in many other environments of fundamental or technological relevance.…”
Section: Introductionmentioning
confidence: 99%