A&A 456, 189-204 (2006)
DOI: 10.1051/0004-6361:20054156
Recipes for stellar jets: results of combined
optical/infrared diagnostics
L. Podio1, F. Bacciotti2, B. Nisini3, J. Eislöffel4, F. Massi2, T. Giannini3 and T. P. Ray5 1
Dipartimento di Astronomia e Scienza dello Spazio,
Universitá degli Studi di Firenze, Largo E. Fermi 2, 50125 Firenze, Italy
e-mail: lindapod@arcetri.astro.it
2
INAF-Osservatorio Astrofisico di Arcetri,
Largo E. Fermi 5, 50125 Florence, Italy
3
INAF-Osservatorio Astronomico di Roma,
via di Frascati 33, 00040 Monte Porzio Catone, Italy
4
Thüringer Landessternwarte Tautenburg,
Sternwarte 5, 07778 Tautenburg, Germany
5
School of Cosmic Physics, Dublin Institute for Advanced Studies,
5 Merrion Square, Dublin 2, Ireland
(Received 5 September 2005 / Accepted 26 May 2006)
Abstract
We examine the conditions of the plasma along
a sample of "classical" Herbig-Haro (HH) jets located in the Orion and Vela
star forming regions, through combined
optical-infrared spectral diagnostics.
Our sample includes HH 111, HH 34, HH 83, HH 73, HH 24 C/E, HH 24 J,
observed quasi-simultaneously and in the same manner
at moderate spatial/spectral resolution.
Once inter-calibrated, the obtained spectra cover
a wide wavelength range from 0.6-2.5
m, including
many transitions from regions of different excitation conditions.
This allows us to probe the density and temperature stratification which
characterises the cooling zones behind the shock fronts along the jet.
From the line ratios we derive the variation of
the visual extinction along the flow,
the electron density and temperature (
and
), the
hydrogen ionisation fraction
, and
the total density
in the emission region of different lines.
The knowledge of such parameters is essential for testing existing jet
models and for planning follow-up high-angular resolution observations.
From the diagnostics of optical forbidden lines
we find, on average, that in the examined jets, in the region
of optical emission,

varies between 50 cm
-3 and

cm
-3,

ranges between 0.03 and 0.6,
and the electron temperature

is ~

K in the HH 111 and HH 34
jets, while it appears to be higher (

K on average) in the
other examined jets.
The electron density and temperature derived from [

] lines,
turn out to be, respectively, higher and lower in comparison to
those determined from optical lines,
in agreement with the fact that the [

] lines arise in the more
compressed gas located further from the shock front.
An even denser component in the jets,
with values of

up to 10
6 cm
-3 is detected using the ratio of
calcium lines.
The derived physical parameters are used to estimate the depletion onto
dust grains of calcium and iron with respect to solar abundances. This
turns out to be quite substantial, being between 70% and 0% for Ca and ~90% for Fe.
This leads us to suggest that the weak shocks present in the beams
are not capable of completely destroying the ambient dust grains,
confirming previous theoretical studies.
We then derive the mass flux rates,

, in the flows
using two independent methods.
Taking into account the filling factor of the emitting gas,

is on average

yr
-1.
The associated linear momentum fluxes
(

)
are higher than, or of the same order as, those measured in the
coaxial molecular flows, where present, suggesting
that the flows are jet driven.
Finally, we discuss differences between jets in our sample.
In general, we find that higher ionisation and electron temperatures
are associated with less dense jets.
The comparison suggests that the shock mechanism
exciting the knots along the flows has the same efficiency in
all the examined objects, and the observed differences are consistent
with the different densities, and hence cooling rates, found
in the various flows.
Key words: stars: circumstellar matter
-- infrared: ISM
--
ISM: Herbig-Haro objects
-- ISM: jets and outflows
© ESO 2006
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