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Cécile Gry and Olivier Dupin
Laboratoire d'Astronomie Spatiale, B.P.8, F-13376 Marseille cedex 12,
France
Many observations report that the Sun is embedded in a small interstellar
cloud, with T=7000 K and n of the order of 0.1 cm,
itself located in a region of low density (n
5
) and high
temperature (T
K) called the Local Bubble. This one extends in
all directions to at least 50 pc and reaches the stars
CMa and
CMa respectively 188 and 206 pc away (Gry et al. 1985, Welsh et al. 1995).
We have obtained spectra of both CMa and
CMa with the HST
GHRS.
The analysis of the interstellar medium towards
CMa has been
presented in Gry et al. (1995), as well as the data processing and line profile
analysis methods used for both stars.
We present here a new study of the
CMa line of sight and its
comparison to the
CMa direction.
Three main components, numbered 1 to 3, have been detected without ambiguity
in the CMa FeII and MgII lines (see Gry et al.
1995). The first one has been identified to the Local Interstellar Cloud (LIC),
in which the Sun is
embedded, and the second one is identical to the second component seen in
the line of sight to
CMa, that lies only 3 pc away from the Sun
(Lallement et al. 1994). Table 1 summarizes
the temperatures and turbulent velocities of these three clouds derived
from both FeII and MgII b-values.
The electron densities shown in Table 1 have been obtained from the
observed MgII/MgI ratio. Despite of the high uncertainty on
these values, it is clear that the ionization is important in these clouds.
For the LIC, the ionization fraction ranges from 5 to 75% with a
preferred value of 47% if T=7000 K and n(HI)=0.1 are adopted.
The LIC and the component 3 have been detected in highly ionized species
(CIV and SiIII). The most plausible
interpretation is a collisional ionization in a high temperature gas
( K) linked to these components. This gas could be the thermal
conduction interface between the clouds and the very hot coronal gas
(
K) which fills the Local Bubble and is responsible of the soft
X-ray background.
Cassinelli
et al. (1995a) and Vallerga et al. (1995) have established a total HI
column density of 9 cm
from the lyman continuum in the
EUVE spectrum. We find an upper limit of 5
cm
from the
NI lines.
The total H column density is slightly higher, indicating that about
half of the gas is ionized : N(H
) has been estimated to
1.5
cm
for FeII and 1.4
cm
for MgII using the
warm cloud abundances determined by Jenkins et al. (1986).
The contribution
of the clouds 1 and 2 to the total column density is located within the 3 first
parsecs. Therefore, in the other 185 pc, the mean gas density is less than 4.5
cm
. This makes the
CMa line of sight the most
devoid region of neutral gas known in the solar neighborhood.
Table 1: Physical conditions in the clouds:
The line of sight towards CMa had already been studied by
Gry et al. (1985) at lower resolution
with Copernicus UV data.
They reported an HI column density of 1--2
cm
and
a total H column density (derived from SII and SIII)
of about 1.6
cm
.
The study of the EUV spectrum of
CMa by Cassinelli et al. (1995b) has
yield to a total column density of 2.0
0.2 10
cm
for
HI and at least 1.4 10
cm
for HeI that implies
a total H column density of at least 1.4 10
cm
, both results
in agreement with the previous Copernicus results.
Our Ech-B GHRS data allow us for the first time to separate the
interstellar absorption in
at least 4 clouds labeled A, B, C and D (figure 1). All four are
visible in both the FeII and MgII lines, but only the
strongest C and D components in the MgI and SiIII lines.
Physical parameters of the clouds are shown in Table 1.
The projection of the Local Cloud (LIC) velocity vector
(v=26
towards the direction
,
(Lallement & Bertin 1992) on the
CMa line of sight give us an
heliocentric velocity of 20.3
for its absorption feature. So, the component due to
the LIC is hidden in the blue wing of the component C; but we take it into
account in our model adopting the column densities and b-values found in
the
CMa direction.
Given its velocity position, the cloud B can be identified to the
component 2 of CMa. However, its location close to the component
C has made the determination of both its column densities and b-values very
uncertain.
Using the warm cloud abundances of Jenkins et al. (1986) and our column
densities, we derived N(H)=1.5
0.2 10
cm
and
N(H
)=1.7
0.3 10
cm
from, respectively, FeII and MgII, that is in good agreement with the Copernicus and
EUVE values. We, thus, confirm that at least 90% of the matter in the line
of sight is ionized. The strength
of our data is to show that the ionized gas is distributed in two distinct
interstellar components (C and D) for which we measure the electron densities
from the MgII/MgI ratio (the results are shown in table 1).
This shows altogether that the ionized gas is not uniformly
distributed in the line of sight and that it
does not constitute either a usual
HII region around the star
CMa.
We have measured N(SiIII) for clouds C and D, but we failed in
detecting CIV unlike in the CMa case. This lack
of detection could induce inhomogeneities of the boundary layer.
Figure: GHRS Ech-B spectrum (R85000) of MgII, MgI
and FeII lines.
The solid points are the observations, the dashed line is the stellar
continuum and the solid line the fit to the interstellar absorption profile.
Despite of their proximity and their similarities in HI content,
the lines of sight of CMa and
CMa are radically different. The
CMa sigh-line intercepts
mostly local gas
and thereby allows the study of the physical conditions in local clouds.
Its two main clouds have been detected in the
CMa line of sight (3
pc away) and so, it is essentially empty after the 3 first parsecs.
The CMa line of sight is dominated by two ionized components,
located after the 3 first parsecs (not detected in the
CMa
direction), where at least 90% of the gas responsible for the FeII
and MgII absorption is not in an HI region. This ionization
could be due to the strong EUV radiation fields produced by both
CMa and
CMa which are known to be the strongest EUV
sources in the sky. Note that a
collisional ionization induced by the particular location of the clouds in
the void tunnel is also possible. The study of the ionization processes
constitute the next step of our work.
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