Burnham's nebula (HH 255), a peculiar Herbig-Haro object.

Details Burnham's nebula (HH 255), a peculiar Herbig-Haro object. Burnham's nebula (HH 255), a peculiar Herbig-Haro object.

Feb 1997

adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1997a%26a...318..565b&link_type=abstract

Astronomy and Astrophysics, v.318, p.565-570

Astronomy and Astrophysics

Astrophysics

9

Stars: Individual: T Tau, Stars: Pre-Main Sequence, Ism: Individual: Burnham Nebula, Ism: Jets And Outflows, Ism: Kinematics And Dynamics

Scientific paper

Burnham's nebula (HH 255) has been consistently identified as a Herbig-Haro object, i.e. a radiating shock wave. Spectrophotometry shows that at least a considerable part of this shock wave must have a velocity of ~90km/s or more. Recently, position-velocity diagrams have shown that the centroid radial velocity and the radial velocity dispersion are unusually small in HH 255 causing problems in the detailed shock wave interpretation. A bow shock like structure is excluded. In order to get some insight into the physics of this enigmatic HH object we have studied the degree of ionization, the kinematic state and the electron density as a function of position near the main axis of HH 255. We find that the ionization (visible in a steep increase in O^++^, N^+^ ions and in a decrease in C^o^ and Ca^+^) occurs in a very narrow (1.0"-1.5" wide) region which is centered at ~3" S of T Tau. In the same narrow region the centroid radial velocity drops rapidly to zero and the radial velocity dispersion has a maximum and then drops rapidly to 25 km.s^-1^ (FWHM). Beyond 4."5 S of T Tau HH 255 looks qualitatively like a pure recombination zone. The [OIII] lines and then the [NII] lines become gradually weak in comparison to neutral and low-ionization lines. However, this interesting region, which forms the bulk of HH 255, is about 100 times wider than the theoretical prediction for the recombination region of a plane shock with the same post-shock density and the same shock velocity as HH 255. Consequently an interpretation of the zero radial velocity region as a plane shock seen edge-on is also excluded.

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