2004MNRAS.353..813M


Query : 2004MNRAS.353..813M

2004MNRAS.353..813M - Mon. Not. R. Astron. Soc., 353, 813-824 (2004/September-3)

On the excitation of the infrared knots in the HH99 outflow.

McCOEY C., GIANNINI T., FLOWER D.R. and CARATTI O GARATTI A.

Abstract (from CDS):

We present near-infrared (IR) spectra (0.98-2.5 µm) from the group of Herbig-Haro (HH) objects comprising HH99: a series of knots forming a bow, HH99B, and a separate knot, HH99A. Observations of H2, [Feii] and [Ci] are used to constrain shock-model parameters and determine the origin of the emission. Previous work has shown that it is likely that the atomic and ionic emission arises in regions of higher ionization than the molecular emission. On the basis of observations, it has often been suggested that the [Feii] and [Ci] emission could arise, for example, at the apex of a bow shock, with the H2emission produced in the wings. Accordingly, we have combined models of C-component and J-type shocks in order to reproduce the observed H2, [Feii] and [Ci] line spectra. We can account for the H2 emission towards the HH99B complex by means of J-type shocks with magnetic precursors. We derive shock velocities of about 30 km/s and ages of order 100 yr; the pre-shock gas has a density nH~ 104/cm3 and the magnetic field B~ 100µG. The J-type shocks required to reproduce the intensities of the observed [Feii] and [Ci] lines have velocities of 50 km/s. It is necessary to assume that Fe has been previously eroded from grains, probably by the earlier passage of a C-type shock wave. Thus, our analysis supports the view that molecular outflows are episodic phenomena whose observed emission arises in shock waves.

Abstract Copyright: 2004 RAS

Journal keyword(s): shock waves - circumstellar matter - ISM: Herbig-Haro objects - ISM: jets and outflows - infrared: ISM

Simbad objects: 10

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Number of rows : 10
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 HD 175529 * 18 57 34.3957961784 -39 49 23.501805888   6.480 6.284     A5IV/V 31 0
2 [B92b] 30 Y*O 19 01 52.63 -36 57 00.2           ~ 31 0
3 V* R CrA Ae* 19 01 53.6764322232 -36 57 08.299341828 12.781 12.651 11.917 11.242 10.412 B5IIIpe 499 2
4 HH 99 HH 19 02 05.407 -36 54 39.85           ~ 29 0
5 HH 99A HH 19 02 05.41 -36 54 39.6           ~ 19 0
6 HH 99B HH 19 02 05.61 -36 54 35.0           ~ 21 0
7 HH 99B1 HH ~ ~           ~ 3 0
8 HH 99B0 HH ~ ~           ~ 3 0
9 HH 99B3 HH ~ ~           ~ 3 0
10 HH 99B2 HH ~ ~           ~ 3 0

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