Articles
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02/28/2006--
02/28/2006
Properties of dust and detection of Halpha emission in LDN 1780
We present ISOPHOT observations between 60 and 200 microns and a
near-infrared extinction map of LDN 1780. We have used the ISOPHOT data
together with the 25, 60 and 100 microns IRIS maps to disentangle the warm and
cold components of large dust grains that are observed in translucent and dense
clouds. The warm and cold components in LDN 1780 have different properties and
spatial distributions, with the warm component surrounding the cold component.
The cold component is associated with molecular gas at densities of ~1000
cm^-3. The warm component has a uniform colour temperature of 25 K, and the
colour temperature of the cold component slightly varies between 15.8 and 17.3
K (beta=2, Delta(T)=0.5 K). The ratio between the 200 microns emission of the
cold component and Av is Ic(200)/Av=12.1 MJy/sr/mag and the average ratio
tau(200)/Av=2.0x10^-4 mag^-1. The far-infrared emissivity of the warm component
is significantly lower than that of the cold component. The Halpha emission and
Av correlate very well; a ratio I(Halpha)/Av=2.2 Rayleigh/mag is observed. This
correlation indicates the presence of a source of ionisation that can penetrate
deeply into the cloud. Using the ratio I(Halpha)/Av we have estimated a
ionisation rate for LDN 1780 that results to be ~10^-16 photons/s. We interpret
this relatively high value as due to an enhanced cosmic ray flux of ~10 times
the standard value. The origin of the cosmic rays could be from supernovae in
the Scorpio-Centaurus OB association and/or the runaway zeta Ophiuchus.
C. del Burgo
L. Cambresy
01/05/2011--
01/05/2011
Variation of the extinction law in the Trifid nebula
In the past few years, the extinction law has been measured in the infrared
wavelengths for various molecular clouds and different laws have been obtained.
In this paper we seek variations of the extinction law within the Trifid nebula
region. Such variations would demonstrate a local dust evolution linked to
variation of the environment parameters such as the density or the interstellar
radiation field. The extinction values, A_lambda/A_V, are obtained using the
2MASS, UKIDSS and Spitzer/GLIMPSE surveys. The technique is to inter-calibrate
color-excess maps from different wavelengths to derive the extinction law and
to map the extinction in the Trifid region. We measured the extinction law at
3.6, 4.5, and 5.8 um and we found a transition at A_V ~ 20 mag. Below this
threshold the extinction law is as expected from models for R_V=5.5 whereas
above 20 mag of visual extinction, it is flatter. Using these results the
color-excess maps are converted into a composite extinction map of the Trifid
nebula at a spatial resolution of 1 arcmin. A tridimensional analysis along the
line-of-sight allowed us to estimate a distance of 2.7 kpc for the Trifid. The
comparison of the extinction with the 1.25 mm emission suggests the millimeter
emissivity is enhanced in the dense condensations of the cloud. Our results
suggest a dust transition at large extinction which has not been reported so
far and dust emissivity variations.
L. Cambrésy
J. Rho
D. J. Marshall
W. T. Reach
10/03/2013--
10/03/2013
Present status of two-dimensional ESTER models: Application to Be stars
ESTER two-dimensional models solve the steady state structure of fast
rotating early-type stars including the large scale flows associated with the
baroclinicity of the radiative zones. Models are compared successfully to the
fundamental parameters of the two main components of the triple system $\delta$
Velorum that have been derived from interferometric and orbit measurements.
Testing the models on the Be star Achernar ($\alpha$ Eri), we cannot reproduce
the data and conclude that this star has left the main sequence and is likely
crossing the Herzsprung gap. Computing main sequence evolution of fast rotating
stars at constant angular momentum shows that their criticality increases with
time suggesting that the Be phenomenon and the ensuing mass ejections is the
result of evolution.
M. Rieutord
F. Espinosa Lara
05/14/2010--
05/14/2010
A Herschel study of the properties of starless cores in the Polaris Flare dark cloud region using PACS and SPIRE
The Polaris Flare cloud region contains a great deal of extended emission. It
is at high declination and high Galactic latitude. It was previously seen
strongly in IRAS Cirrus emission at 100 microns. We have detected it with both
PACS and SPIRE on Herschel. We see filamentary and low-level structure. We
identify the five densest cores within this structure. We present the results
of a temperature, mass and density analysis of these cores. We compare their
observed masses to their virial masses, and see that in all cases the observed
masses lie close to the lower end of the range of estimated virial masses.
Therefore, we cannot say whether they are gravitationally bound prestellar
cores. Nevertheless, these are the best candidates to be potentialprestellar
cores in the Polaris cloud region.
D. Ward-Thompson
J. M. Kirk
P. André
P. Saraceno
P. Didelon
V. Könyves
N. Schneider
A. Abergel
J. -P. Baluteau
J. -Ph. Bernard
S. Bontemps
L. Cambrésy
P. Cox
J. Di Francesco
A. M. Di Giorgio
M. Griffin
P. Hargrave
M. Huang
J. Z. Li
P. Martin
A. Men'shchikov
V. Minier
S. Molinari
F. Motte
G. Olofsson
S. Pezzuto
D. Russeil
M. Sauvage
B. Sibthorpe
L. Spinoglio
L. Testi
G. White
C. Wilson
A. Woodcraft
A. Zavagno
05/17/2010--
05/17/2010
The Aquila prestellar core population revealed by Herschel
The origin and possible universality of the stellar initial mass function
(IMF) is a major issue in astrophysics. One of the main objectives of the
Herschel Gould Belt Survey is to clarify the link between the prestellar core
mass function (CMF) and the IMF. We present and discuss the core mass function
derived from Herschel data for the large population of prestellar cores
discovered with SPIRE and PACS in the Aquila Rift cloud complex at d ~ 260 pc.
We detect a total of 541 starless cores in the entire ~11 deg^2 area of the
field imaged at 70-500 micron with SPIRE/PACS. Most of these cores appear to be
gravitationally bound, and thus prestellar in nature. Our Herschel results
confirm that the shape of the prestellar CMF resembles the stellar IMF, with
much higher quality statistics than earlier submillimeter continuum
ground-based surveys.
V. Könyves
Ph. André
A. Men'shchikov
N. Schneider
D. Arzoumanian
S. Bontemps
M. Attard
F. Motte
P. Didelon
A. Maury
A. Abergel
B. Ali
J. -P. Baluteau
J. -Ph. Bernard
L. Cambrésy
P. Cox
J. Di Francesco
A. M. di Giorgio
M. J. Griffin
P. Hargrave
M. Huang
J. Kirk
J. Z. Li
P. Martin
V. Minier
S. Molinari
G. Olofsson
S. Pezzuto
D. Russeil
H. Roussel
P. Saraceno
M. Sauvage
B. Sibthorpe
L. Spinoglio
L. Testi
D. Ward-Thompson
G. White
C. D. Wilson
A. Woodcraft
A. Zavagno
07/22/2013--
07/17/2013
Young stellar clusters in the Rosette molecular cloud. Arguments against triggered star formation
The Rosette complex is a well studied region of the galactic plane which
presents the apparent characteristics of a triggered star forming region. This
is however still debated as no strong evidence corroborates this statement. We
focus on characterizing the young stellar population in the Rosette complex to
improve our understanding of the processes that regulate the star formation in
this region. We propose an original method that relies on the joint analysis of
the star color and density in the near-infrared. It leads to mapping the
molecular cloud spatial distribution and detecting the embedded clusters with
their characterization in terms of member number and age estimation. We have
identified 13 clusters, 2 of which are new discoveries, and we estimate that
the total number of young stellar objects in the Rosette ranges between 4000
and 8000 members. We find that the age distribution of the young clusters is
not consistent with a general triggered scenario for the star formation in this
molecular cloud. This study proves that the Rosette complex evolution is not
governed by the influence of its OB star population. It suggests that the
simple morphological appearance of an active region is not sufficient to
conclude much about the triggering role in the star formation process. Our
method of constraining the cluster properties using UKIDSS and WISE data has
proven efficient, and studies of other regions of the galactic plane would
definitely benefit from this approach.
L. Cambrésy
G. Marton
O. Feher
L. V. Tóth
N. Schneider
05/04/2004--
05/04/2004
Multi-wavelength analysis of the dust emission in the Small Magellanic Cloud
We present an analysis of dust grain emission in the diffuse interstellar
medium of the Small Magellanic Cloud (SMC). This study is motivated by the
availability of 170 microns ISOPHOT data covering a large part of the SMC, with
a resolution enabling to disentangle the diffuse medium from the star forming
regions. After data reduction and subtraction of Galactic foreground emission,
we used the ISOPHOT data together with HiRes IRAS data and ATCA/Parkes combined
HI column density maps to determine dust properties for the diffuse medium. We
found a far infrared emissivity per hydrogen atom 30 times lower than the Solar
Neighborhood value. The modeling of the spectral energy distribution of the
dust, taking into account the enhanced interstellar radiation field, gives a
similar conclusion for the smallest grains (PAHs and very small grains)
emitting at shorter wavelength. Assuming Galactic dust composition in the SMC,
this result implies a difference in the gas-to-dust ratio (GDR) 3 times larger
than the difference in metallicity. This low depletion of heavy elements in
dust could be specific of the diffuse ISM and not apply for the whole SMC dust
if it results from efficient destruction of dust by supernovae explosions.
C. Bot
F. Boulanger
G. Lagache
L. Cambresy
D. Egret
10/13/2005--
10/11/2005
Luminous AGB stars in nearby galaxies. A study using Virtual Observatory tools
Aims. This study focuses on very luminous Mbol<-6.0 mag AGB stars with
J-Ks>1.5 mag and H-Ks>0.4 mag in the LMC, SMC, M31, and M33 from 2MASS data.
Methods.The data were taken from the 2MASS All-Sky Point Source catalogue
archive. We used Virtual Observatory tools and took advantage of its
capabilities at various stages in the analysis.
Results. It is well known that stars with the colors we selected correspond
mainly to carbon stars. Although the most luminous AGBs detected here contain a
large number of carbon stars,they are not included in existing catalogues
produced from data in the optical domain, where they are not visible since they
are dust-enshrouded. A comparison of the AGB stars detected with combined near
and mid-infrared data from MSX and 2MASS in the LMC shows that 10% of the
bright AGB stars are bright carbon stars never detected before and that the
other 50% are OH/IR oxygen rich stars, whereas the 40% that remain were not
cross-matched.
Conclusions. The catalogues of the most luminous AGB stars compiled here are
an important complement to existing data. In the LMC, these bright AGB stars
are centrally located, whereas they are concentrated in an active
star-formation ring in M31. In the SMC and M33, there are not enough of them to
draw definite conclusions, although they tend to be centrally located. Their
luminosity functions are similar for the four galaxies we studied.
P. Tsalmantza
E. Kontizas
L. Cambresy
F. Genova
A. Dapergolas
M. Kontizas
07/03/2006--
07/03/2006
Can We Trust the Dust? Evidence of Dust Segregation in Molecular Clouds
Maps of estimated dust column density in molecular clouds are usually assumed
to reliably trace the total gas column density structure. In this work we
present results showing a clear discrepancy between the dust and the gas
distribution in the Taurus molecular cloud complex. We compute the power
spectrum of a 2MASS extinction map of the Taurus region and find it is much
shallower than the power spectrum of a 13CO map of the same region previously
analyzed. This discrepancy may be explained as the effect of grain growth on
the grain extinction efficiency. However, this would require a wide range of
maximum grain sizes, which is ruled out based on constraints from the
extinction curve and the available grain models. We show that major effects due
to CO formation and depletion are also ruled out. Our result may therefore
suggest the existence of intrinsic spatial fluctuations of the dust to gas
ratio, with amplitude increasing toward smaller scales. Preliminary results of
numerical simulations of trajectories of inertial particles in turbulent flows
illustrate how the process of clustering of dust grains by the cloud turbulence
may lead to observable effects. However, these results cannot be directly
applied to large scale supersonic and magnetized turbulence at present.
Paolo Padoan
Laurent Cambresy
Mika Juvela
Alexei Kritsuk
William D. Langer
Michael L. Norman
05/25/2010--
05/14/2010
From filamentary clouds to prestellar cores to the stellar IMF: Initial highlights from the Herschel Gould Belt survey
We summarize the first results from the Gould Belt survey, obtained toward
the Aquila Rift and Polaris Flare regions during the 'science demonstration
phase' of Herschel. Our 70-500 micron images taken in parallel mode with the
SPIRE and PACS cameras reveal a wealth of filamentary structure, as well as
numerous dense cores embedded in the filaments. Between ~ 350 and 500
prestellar cores and ~ 45-60 Class 0 protostars can be identified in the Aquila
field, while ~ unbound starless cores and no protostars are observed in the
Polaris field. The prestellar core mass function (CMF) derived for the Aquila
region bears a strong resemblance to the stellar initial mass function (IMF),
already confirming the close connection between the CMF and the IMF with much
better statistics than earlier studies. Comparing and contrasting our Herschel
results in Aquila and Polaris, we propose an observationally-driven scenario
for core formation according to which complex networks of long, thin filaments
form first within molecular clouds, and then the densest filaments fragment
into a number of prestellar cores via gravitational instability.
Ph. André
A. Men'shchikov
S. Bontemps
V. Könyves
F. Motte
N. Schneider
P. Didelon
V. Minier
P. Saraceno
D. Ward-Thompson
J. Di Francesco
G. White
S. Molinari
L. Testi
A. Abergel
M. Griffin
Th. Henning
P. Royer
B. Merín
R. Vavrek
M. Attard
D. Arzoumanian
C. D. Wilson
P. Ade
H. Aussel
J. -P. Baluteau
M. Benedettini
J. -Ph. Bernard
J. A. D. L. Blommaert
L. Cambrésy
P. Cox
A. Di Giorgio
P. Hargrave
M. Hennemann
M. Huang
J. Kirk
O. Krause
R. Launhardt
S. Leeks
J. Le Pennec
J. Z. Li
P. Martin
A. Maury
G. Olofsson
A. Omont
N. Peretto
S. Pezzuto
T. Prusti
H. Roussel
D. Russeil
M. Sauvage
B. Sibthorpe
A. Sicilia-Aguilar
L. Spinoglio
C. Waelkens
A. Woodcraft
A. Zavagno
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