An infrared study of the L1551 star formation region

Liseau, R.; White, G. J.; Ceccarelli, C.; Benedettini, M.; Spinoglio, L.; Justtanont, K.; Men'shchikov, A. B.; Caux, E.; Molinari, S.; Lorenzetti, D.; Nisini, B.; Smith, H. A.; Giannini, T.; Saraceno, P.; Tommasi, E.; Kaufman, M.; Correia, J. C.

Sweden, United Kingdom, Italy, France, United States

Abstract

Spectroscopic observations using the Infrared Space Observatory are reported towards the two well known infrared sources and young stellar objects L1551 IRS 5 and L1551 NE, and at a number of locations in the molecular outflow. The ISO spectrum contains several weak gas-phase lines of O I, C II, [Fe II] and [Si II], along with solid state absorption lines of CO, CO_2, H_2O, CH_4 and CH_3OH. Hubble Space Telescope (HST) images with the NICMOS infrared camera reveal a diffuse conical shaped nebulosity, due to scattered light from the central object, with a jet emanating from L1551 IRS 5. The continuum spectral energy distribution has been modelled using a 2D radiative transfer model, and fitted for a central source luminosity of 45 Lsun, surrounding a dense torus extending to a distance of ~ 3x104 AU, which has a total mass of ~ 13 Msun. The visual extinction along the outflow is estimated to be ~ 10 and the mid-plane optical depth to L1551 IRS 5 to be ~ 120. This model provides a good fit to the ISO spectral data, as well as to the spatial structures visible on archival HST/NICMOS data, mid-IR maps and sub-millimetre radio interferometry, and to ground-based photometry obtained with a range of different aperture sizes. On the basis of the above model, the extinction curve shows that emission at wavelengths shorter than ~ 2 mu m is due to scattered light from close to L1551 IRS 5, while at wavelengths >~ 4 mu m, is seen through the full extinguishing column towards the central source. Several [Fe II] lines were detected in the SWS spectrum towards L1551 IRS 5. Although it would seem at first sight that shocks would be the most likely source of excitation for the [Fe II] in a known shocked region such as this, the line intensities do not fit the predictions of simple shock models. An alternative explanation has been examined where the [Fe II] gas is excited in hot ( ~ 4000 K) and dense (>~ 109 cm-3) material located close to the root of the outflow. The SWS observations did not detect any emission from rotationally excited H_2. Observations with United Kingdom Infrared Telescope (UKIRT) of the vibrationally excited S- and Q-branch lines were however consistent with the gas having an excitation temperature of ~ 2500 K. There was no evidence of lower temperature ( ~ 500 K) H_2 gas which might be visible in the rotational lines. Observations with UKIRT of the CO absorption bands close to 2.4 mu m are best fit with gas temperatures ~ 2500 K, and a column density ~ 6x1020 cm-2. There is strong circumstantial evidence for the presence of dense (coronal and higher densities) and hot gas (at least 2500 K up to perhaps 5000 K) close to the protostar. However there is no obvious physical interpretation fitting all the data which can explain this.

2000 Astronomy and Astrophysics
ISO eHST 35