Velocity structure in the orion nebula. ii. emission line atlas of partially ionized to fully ionized gas

We present an atlas4 of three-dimensional (position-position-velocity) spectraof the Orion Nebula in optical emission lines from a variety of different ionizationstages: [O I] 6300˚A, [S II] 6716,6731˚A, [N II] 6584˚A, [S III] 6312˚A, Hα 6563˚A,a...

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Bibliographic Details
Authors: T. Doi, Ma. T. García Díaz, W. J. Henney, J. A. López
Format: article
Status:Published version
Publication Date:2008
Country:México
Institution:Universidad Nacional Autónoma de México
Repository:Redalyc-UNAM
OAI Identifier:oai:redalyc.org:57144114
Online Access:https://www.redalyc.org/articulo.oa?id=57144114
Access Level:Open access
Keyword:Física, Astronomía y Matemáticas
H II regions — ISM: Herbig
Haro objects — ISM: individual: Orion nebula — techniques: spectroscopy — turbulence
Description
Summary:We present an atlas4 of three-dimensional (position-position-velocity) spectraof the Orion Nebula in optical emission lines from a variety of different ionizationstages: [O I] 6300˚A, [S II] 6716,6731˚A, [N II] 6584˚A, [S III] 6312˚A, Hα 6563˚A,and [O III] 5007˚A. These transitions provide point to point information aboutthe physical structure and kinematics of the nebula at an effective resolution of3´´ × 2´´ × 10 km s−1, clearly showing the large scale behavior of the ionized gasand the presence of localized phenomena such as Herbig-Haro outflows. As anexample application of the atlas, we present a statistical analysis of the widths ofthe Hα, [OIII], and [N II] lines that permits a determination of the mean electrontemperature in the nebula of (9200 ± 400) K. We also find, in contradiction toprevious claims, that the non-thermal line broadening is not significantly differentbetween recombination lines and collisional lines.