
The interstellar carbonaceous aromatic matter as a trap for molecular hydrogen
Author(s) -
Pauzat F.,
Lattelais M.,
Ellinger Y.,
Minot C.
Publication year - 2011
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2010.18106.x
Subject(s) - physisorption , physics , interstellar medium , graphene , astrochemistry , molecule , hydrogen , interstellar cloud , chemical physics , carbon fibers , atomic physics , density functional theory , polycyclic aromatic hydrocarbon , molecular physics , chemistry , galaxy , astrophysics , astrobiology , materials science , composite number , quantum mechanics , adsorption , composite material
We report a theoretical study of the physisorption of molecular hydrogen, H 2 , on a major component of the interstellar dust, namely, the polyaromatic carbonaceous grains. Going beyond the model of the polycyclic aromatic hydrocarbon freeflyers and its theoretical treatment within the super molecule approach, we consider the graphene surface in a Density Functional Theory periodic approach using plane‐wave expansions. The physisorption energy of isolated H 2 on that flat and rigid support is determined to be attractive by ∼0.75 kcal mol −1 and practically independent of the orientation with respect to the infinite surface. Since this energy is also not affected by the position (over a ring centre, a carbon atom or the middle of a carbon–carbon bond), we can conclude that H 2 is able to move freely like a ball rolling on the graphene support. We also investigate the conditions for multiple physisorption. It leads to a monolayer of H 2 molecules where the corresponding interaction energy per H 2 amounts to a potential depth of ∼1 kcal mol −1 , close to the available experimental estimates ranging from 1.1 to 1.2 kcal mol −1 . We show that the most energetically favourable coverage, which corresponds to an arrangement of the H 2 molecules, the closest possible to the dimer configuration, leads to a surface density of ∼ 0.8 × 10 15 molecule cm −2 . Finally, assuming that 15–20 per cent of the interstellar carbon is locked in aromatic systems, one obtains ∼10 −5 of the interstellar hydrogen trapped as H 2 on such types of surfaces.