Context. We present an analysis of the kinematics and physical properties of the Class I driven jet HH46-47 based on IR medium and low resolution spectroscopy obtained with ISAAC on VLT. Aims. Our aim is to study the gas physics as a function of the velocity and distance from the source and to compare the results with similar studies performed on other Class I and classical T Tauri jets as well as with existing models for the jet formation and excitation. have been used to derive physical parameters such as electron density, H 2 temperature, iron gas-phase abundance and mass flux.
Methods[Fe ii] 1.644 μm and H 2 2.122 μm position velocity diagrams (PVDs) have been additionally constructed to study the kinematics of both the atomic and molecular gas. Results. Within 1000-2000 AU from the source the atomic gas presents a wide range of radial velocities, from ∼-230 km s −1 to ∼100 km s −1 . Only the gas component at the highest velocity (high velocity component, HVC) survives at large distances. The H 2 shows only a single velocity component at almost zero velocity close to the source while it reaches higer velocities (up to ∼95 km s −1 ) further downstream. Electron densities (n e ) and mass ejection fluxes (Ṁ jet ) have been separately measured for the HVC and for the component at lower velocity (LVC) from the [Fe ii] lines. n e increases with decreasing velocities with an average value of ∼ 6000 cm −3 for the LVC and ∼4000 cm −3 for the HVC, while the opposite occurs forṀ jet which is ∼0.5−2 × 10 −7 M yr −1 and ∼0.5−3.6 × 10 −8 M yr −1 for the HVC and LVC, respectively. The mass flux carried out by the molecular component, measured from the H 2 lines flux, is ∼4 × 10 −9 M yr −1 . We have estimated that the Fe gas phase abundance is significantly lower than the solar value, with ∼88% of iron still depleted onto dust grains in the internal jet region. This fraction decreases to ∼58%, in the external knots. Conclusions. Many of the derived properties of the HH46-47 jet are common to jets from young stellar objects (YSOs) in different evolutionary states. The derived densities and mass flux values are typical of Class I objects or very active T Tauri stars. However, the spatial extent of the LVC and the velocity dependence of the electron density have been so far observed only in another Class I jet, the HH34 jet, and are not explained by the current models of jet launching.