218 research outputs found
Dust in the diffuse emission of the galactic plane - The Herschel/Spitzer SED fitting
The first Herschel Hi-Gal images of the galactic plane unveil the
far-infrared diffuse emission of the interstellar medium with an unprecedented
angular resolution and sensitivity. In this paper, we present the first
analysis of these data in combination with that of Spitzer Glimpse & Mipsgal.
We selected a relatively diffuse and low excitation region of the
l~59\,^{\circ} Hi-Gal Science Demonstration Phase field to perform a pixel by
pixel fitting of the 8 to 500 microns SED using the DustEM dust emission model.
We derived maps of the Very Small Grains (VSG) and PAH abundances from the
model. Our analysis allows us to illustrate that the Aromatic Infrared Bands
(AIB) intensity does not trace necessarily the PAH abundance but rather the
product of "abundance x column density x intensity of the exciting radiation
field". We show that the spatial structure of PACS70microns map resembles the
shorter wavelengths (e.g. IRAC8microns) maps, because they trace both the
intensity of exciting radiation field and column density. We also show that the
modeled VSG contribution to PACS70microns (PACS160microns) band intensity can
be up to 50% (7%). The interpretation of diffuse emission spectra at these
wavelengths must take stochastically heated particles into account. Finally,
this preliminary study emphasizes the potential of analyzing the full dust SED
sampled by Herschel and Spitzer data, with a physical dust model (DustEM) to
reach the properties of the dust at simultaneously large and small scales.Comment: accepted for publication in ApJ
Spitzer/IRS investigation of MIPSGAL 24 microns compact bubbles
The MIPSGAL 24 m Galactic Plane Survey has revealed more than 400
compact-extended objects. Less than 15% of these MIPSGAL bubbles (MBs) are
known and identified as evolved stars. We present Spitzer observations of 4 MBs
obtained with the InfraRed Spectrograph to determine the origin of the mid-IR
emission. We model the mid-IR gas lines and the dust emission to infer physical
conditions within the MBs and consequently their nature. Two MBs show a
dust-poor spectrum dominated by highly ionized gas lines of [\ion{O}{4}],
[\ion{Ne}{3}], [\ion{Ne}{5}], [\ion{S}{3}] and [\ion{S}{4}]. We identify them
as planetary nebulae with a density of a few 10 and a central
white dwarf of K. The mid-IR emission of the two other MBs is
dominated by a dust continuum and lower-excitation lines. Both of them show a
central source in the near-IR (2MASS and IRAC) broadband images. The first
dust-rich MB matches a Wolf-Rayet star of K at 7.5 kpc with dust
components of and K. Its mass is about $10^{-3}\
\rm{M_\odot}10^{-6}\ \rm{M_\odot/yr}. The second
dust-rich MB has recently been suggested as a Be/B[e]/LBV candidate. The gas
lines of [\ion{Fe}{2}] as well as hot continuum components (\sim300\sim1250\sim7510^{-3}\ \rm{M_\odot}10^{-5}\ \rm{M_\odot/yr}$.Comment: accepted for publication in Ap
Modeling and budgeting fiber injection efficiency for the Maunakea spectroscopic explorer (MSE)
The Maunakea Spectroscopic Explorer (MSE) will each year obtain millions of
spectra in the optical to near-infrared, at low (R ~ 3,000) to high (R ~
40,000) spectral resolution by observing >4,000 spectra per pointing via a
highly multiplexed fiber-fed system. Key science programs for MSE include black
hole reverberation mapping, stellar population analysis of faint galaxies at
high redshift, and sub-km/s velocity accuracy for stellar astrophysics. One key
metric of the success of MSE will be its survey speed, i.e. how many spectra of
good signal-to-noise ratio will MSE be able to obtain every night and every
year. The survey speed is directly linked to the allocation efficiency - how
many fibers in the focal surface can be allocated to targets - and to the
injection efficiency - what fraction of light from a target can enter the fiber
at the focal surface. In this paper we focus on the injection efficiency and
how to optimize it to increase the signal-to-noise ratio of targets observed in
sky dominated conditions. The injection efficiency depends on the size of the
fiber and requires highly precise, repeatable and stable positioning of the
fiber in the focal surface. We present the allocation budget used for
Conceptual Design Review and the modeling that allows to estimate the injection
efficiency, which is just one part necessary to meet the science requirements
on sensitivities.Comment: Proceedings of SPIE Astronomical Telescopes + Instrumentation 2018;
Modeling, Systems Engineering, and Project Management for Astronomy VII
Proper Motions of Young Stellar Outflows in the Mid-Infrared with Spitzer. II. HH 377/Cep E
We have used multiple mid-infrared observations at 4.5 micron obtained with
the Infrared Array Camera, of the compact (~1.4 arcmin) young stellar bipolar
outflow Cep E to measure the proper motion of its brightest condensations. The
images span a period of ~6 yr and have been reprocessed to achieve a higher
angular resolution (~0.8 arcsec) than their normal beam (2 arcsec).
We found that for a distance of 730 pc, the tangential velocities of the
North and South outflow lobes are 62+/-29 and 94+/-6 km/s respectively, and
moving away from the central source roughly along the major axis of the flow. A
simple 3D hydrodynamical simulation of the H2 gas in a precessing outflow
supports this idea. Observations and model confirm that the molecular Hydrogen
gas, traced by the pure rotational transitions, moves at highly supersonic
velocities without being dissociated. This suggests either a very efficient
mechanism to reform H2 molecules along these shocks or the presence of some
other mechanism (e.g. strong magnetic field) that shields the H2 gas.Comment: Accepted for publication in New Journal of Physics (Special Issue
article
Herschel Survey of the Palomar-Green QSOs at Low Redshift
We investigate the global cold dust properties of 85 nearby (z < 0.5) QSOs,
chosen from the Palomar-Green sample of optically luminous quasars. We
determine their infrared spectral energy distributions and estimate their
rest-frame luminosities by combining Herschel data from 70 to 500 microns with
near-infrared and mid-infrared measurements from the Two Micron All Sky Survey
(2MASS) and the Wide-Field Infrared Survey Explorer (WISE). In most sources the
far-infrared (FIR) emission can be attributed to thermally heated dust. Single
temperature modified black body fits to the FIR photometry give an average dust
temperature for the sample of 33~K, with a standard deviation of 8~K, and an
average dust mass of 7E6 Solar Masses with a standard deviation of 9E6 Solar
Masses. Estimates of star-formation that are based on the FIR continuum
emission correlate with those based on the 11.3 microns PAH feature, however,
the star-formation rates estimated from the FIR continuum are higher than those
estimated from the 11.3 microns PAH emission. We attribute this result to a
variety of factors including the possible destruction of the PAHs and that, in
some sources, a fraction of the FIR originates from dust heated by the active
galactic nucleus and by old stars.Comment: accepted for publication in ApJ
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