Spectroscopic observations using the Infrared Space Observatory are reporte
d towards the two well known infrared sources and young stellar objects L15
51 IRS 5 and L1551 NE, and at a number of locations in the molecular outflo
w. The ISO spectrum contains several weak gas-phase lines of OI, CII, [Fe I
I] and [Si II], along with solid state absorption lines of CO, CO2, H2O, CH
4 and CH3OH. Hubble Space Telescope (HST) images with the NICMOS infrared c
amera reveal a diffuse conical shaped nebulosity, due to scattered light fr
om the central object, with a jet emanating from L1551 IRS 5. The continuum
spectral energy distribution has been modelled using a 2D radiative transf
er model, and fitted for a central source luminosity of 45 L., surrounding
a dense torus extending to a distance of similar to 3 x 10(4) AU, which has
a total mass of similar to 13 M.. The visual extinction along the outflow
is estimated to be approximate to 10 and the mid-plane optical depth to L15
51 IRS 5 to be approximate to 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 w
ith a range of different aperture sizes. On the basis of the above model, t
he extinction curve shows that emission at wavelengths shorter than similar
to 2 mum is due to scattered light from close to L1551 IRS 5, while at wav
elengths greater than or similar to 4 mum, is seen through the full extingu
ishing column towards the central source. Several [FeII] lines were detecte
d 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 bee
n examined where the [Fe II] gas is excited in hot (similar to 4000 K) and
dense (greater than or similar to 10(9) cm(-3)) material located close to t
he root of the outflow. The SWS observations did not detect any emission fr
om rotationally excited Hz. Observations with United Kingdom Infrared Teles
cope (UKIRT) of the vibrationally excited S- and Q-branch lines were howeve
r consistent with the gas having an excitation temperature of similar to 25
00 K. There was no evidence of lower temperature (similar to 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 mum are best lit with gas temperature
s similar to 2500 K, and a column density similar to 6 x 10(20) cm(-2) Ther
e 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 fitti
ng all the data which can explain this.