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dc.contributor.authorOudmaijer, R.D.
dc.contributor.authorDrew, J.E.
dc.contributor.authorBarlow, M.J.
dc.contributor.authorCrawford, I.A.
dc.contributor.authorProga, D.
dc.date.accessioned2009-12-01T10:46:38Z
dc.date.available2009-12-01T10:46:38Z
dc.date.issued1997
dc.identifier.citationOudmaijer , R D , Drew , J E , Barlow , M J , Crawford , I A & Proga , D 1997 , ' Helium absorption and emission towards Theta^1 ORI C ' , Monthly Notices of the Royal Astronomical Society , vol. 291 , no. 1 , pp. 110-120 .
dc.identifier.issn0035-8711
dc.identifier.otherdspace: 2299/4036
dc.identifier.otherORCID: /0000-0003-1192-7082/work/62750190
dc.identifier.urihttp://hdl.handle.net/2299/4036
dc.descriptionOriginal article can be found at: http://adsabs.harvard.edu/basic_search.html Copyright Royal Astronomical Society [Full text of this article is not available in the UHRA]
dc.description.abstractThe Hei absorption and emission systems towards Theta^1Ori C, the exciting star of the Orion Nebula, are investigated. To this end, high-resolution near-infrared long-slit spectra centred on the Hei 1.083-μm and Brgamma lines and an ultra-high-resolution (R~10^6) spectrum of the optical Hei 3889-Angstroms line have been obtained. These data are supplemented by blue high spectral resolution echelle observations of Theta^1Ori C and the other members of the Trapezium. Even at R~10^6, the Hei absorption profile, associated with foreground gas at a heliocentric velocity of +3km s^-1, is very smooth, suggesting a simple broadening mechanism and homogeneity. The combination of the Hei 2^3S column density, deduced from the 3889-Angstroms line, with the non-detection of Brgamma emission at the same velocities sets an upper limit on the electron density in this medium of 10^10 m^-3. The Hei 1.083-μm long-slit spectrum shows the familiar background nebular emission, while a second blueshifted component is visible off-star at the same velocities as the absorption on-star. Several mechanisms to explain this emission are explored. We conclude that it is most probably emission formed behind, and leaking through, the absorbing gas layer. A clue to the origin of this emission is found in its spatial distribution: unlike the bright background nebular emission, the blueshifted component peaks symmetrically around the position of Theta^1Ori C, suggesting a physical association with the star. A possible model for the blueshifted emission is that it arises in a large-scale, dense shock front, provoked in some way by the wind of ^1Ori C.en
dc.language.isoeng
dc.relation.ispartofMonthly Notices of the Royal Astronomical Society
dc.titleHelium absorption and emission towards Theta^1 ORI Cen
dc.contributor.institutionSchool of Physics, Astronomy and Mathematics
dc.description.statusPeer reviewed
rioxxterms.typeJournal Article/Review
herts.preservation.rarelyaccessedtrue


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