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S. M. X. Claude(1),(2), L. W. Avery(1) and H. E.
Matthews(1),(3)
(1)National Research Council of Canada, Herzberg Institute of
Astrophysics, 5071 West Saanich Road, Victoria, BC V8X 4M6, Canada,
(2)Institut de Radio Astronomie Millimétrique (IRAM), 300 Rue de
la Piscine, Domaine Universitaire, F-38406 Saint Martin D'Hères,
France,
(3)Joint Astronomy Centre, 660 North A'ohoku Place, University
Park, Hilo, HI 96720, United States
Abstract:
In the nebula OH 231.8+4.2 we have observed SO and SO2millimeter-wave emission lines having a wide range of excitation
energy. The extent of the SO emission was also mapped. Rotation
diagrams were derived from these observations, and we deduced the
rotation temperatures and relative abundances of SO and SO2 for three
different velocity ranges corresponding to the spherical mass-loss
envelope and the blue and red lobes of the bipolar outflow.
The rotation temperatures for SO and SO2 are higher in the expanding
envelope than in the outflow lobes. Subject to modeling uncertainties,
the relative abundances of both molecules in the lobes are slightly
enhanced by factors 25 times relative to the values in the envelope.
Appeared in ApJ 545, 379
A. Navarrini(1), B. Lazareff(1)
(1)Institut de Radio Astronomie Millimétrique, 300 rue de la Piscine,
38406 St Martin d'Hères, France
Abstract:
We discuss the design and optimisation of two full height waveguide SIS
mixers for astronomical applications both covering the 275-370 GHz
frequency band: a Double Side Band (DSB) and a Single Side Band (SSB)
mixer. The expected SSB receiver noise temperature referred to the mixer
input are in the range 23-35 K for the DSB and 25-38 K for the SSB
mixer. A >30 % operating bandwidth can be achieved in the DSB case by
using an "end-loaded" tuning stub to tune out the junction capacitance
of 75 fF (junction size 1
)
followed by two quarter-wave
transformer sections. A similar operating bandwidth is obtained in the
SSB mixer by using a parallel tuning inductor with a radial microstrip
stub. Single junctions are mounted on a 80 mm thick quartz which
stretches only part way across the waveguide. In the SSB mixer the
image rejection is obtained using a mechanically rugged non-contacting
backshort with a circular cross-section which can be moved inside a
circular waveguide. Both mixers have a 4 GHz IF passband and a central
IF frequency of 6 GHz. A stability criterion for intrinsically DSB and
SSB mixers under typical operating conditions has been derived. We have
shown that when an inductive series matching structure is used to
compensate the junction capacitance, the SSB mixer cannot be operated
over a wide frequency range in a stable way. An inductive parallel
matching structure allows us to fulfil the necessary conditions of
stability.
Receiver performance has been optimised for both mixers in
order to guarantee a low mixer noise temperature while maintaining
adequate gain and stable operations over the whole frequency band of
interest.
Appeared in: ALMA Memo 351, March 2001
R. Bachiller(1), M. Pérez Gutiérrez(1),
M.S.N. Kumar(1) & M. Tafalla(1)
(1)IGN Observatorio Astronómico Nacional, Apartado 1143,
E-28800 Alcalá de Henares, Spain
Abstract:
We present millimeter-wave maps of the L1157 bipolar outflow in
several molecular emission lines (Fig. 4). The CO emission
traces the bulk of the outflowing gas in the red and blue shifted
lobes displaying a remarkable S-shaped symmetry indicating the
presence of a precessing jet. We determine the physical
characteristics of the CO flow and show evidence for 3 or 4
independent episodes of mass ejection from the source. Molecules such
as C3H2, N2H+ and DCO+ are seen to be abundant only in
the quiescent medium, and result to be the best tracers of the
high-density core surrounding the driving source of the outflow.
Other molecules (SiO, CH3OH,H2CO, HCN, CN, SO, SO2) are
abundant in the outflow lobes, but exhibit strong emission
gradients. Multi-line observations of some species indicate that these
gradients are not simply due to excitation effects, but are caused by
an actual stratification in the chemical composition of the shocked
molecular gas. Shock tracers such as SiO, CH3OH, and
sulphur-bearing molecules result to be the most promising candidates
as potential chemical clocks to study the evolution of outflows. The
characteristics of the L1157 outflow, when compared to those of
other outflows from Class0 sources, indicate that L1157 is the
prototype of a category of bipolar outflows around Class0 protostars
which we denominate ``chemically active outflows''.
To appear in A&A. Preprints are available from:
bachiller@oan.es
Figure 4:
Maps of the molecular emission towards the
southern lobe of L1157. First contour and step are 0.07 K km/s for
C3H2, 0.3 for DCO+, 0.8 for N2H+, 1.3 for HCO+ and
SO, 0.7 for CN, 2 for H2CO, CS and SiO, 6 for CH3OH, and 0.5 K
km/s for SO2. The star symbol marks the position of the Class 0
protostar L1157-mm, and the squares mark - for orientation- two
positions where an initial molecular survey was carried out. Note the
striking differences in the line emission distribution which
correspond to a strong chemical segregation created by the outflow
propagation.
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A. Navarrini(1), D. Billon-Pierron(1),
K.F. Schuster(1) and B. Lazareff(1),
(1)Institut de Radio Astronomie Millimétrique, 300 rue de la Piscine,
38406 St Martin d'Hères, France
Abstract:
We discuss the design and optimisation of a SIS Single Side Band (SSB)
mixer covering the 275-370 GHz frequency band for astronomical
applications. The junction is probe-coupled to the full height
waveguide. An adjustable circular non-contacting backshort allows SSB
tuning in either USB or LSB in the whole RF band. A >30 % operating
bandwidth can be achieved by using parallel inductive tuning of the
junction capacitance. The calculated SSB receiver noise temperature
referred to the mixer input is in the range 25-38 K. A stability
criterion for an SSB mixer with distinct signal and image termination
impedances under typical operating conditions is derived. We show that
when an inductive series matching structure with a two-stage impedance
transformer is used to compensate the junction capacitance, the mixer
cannot be operated over a wide frequency range in a stable way. An
inductive parallel matching structure with a single-stage transformer
allows us to fulfill the necessary conditions of stability.
To appear in: Proceedings of the 12th. International Symposium
on Space Terahertz Technology, San Diego, California, USA,
14/02/2001 - 16/02/2001
Natta, A. (1); Prusti, T. (2); Neri, R. (3); Wooden
D. (4); Grinin, V.P. (5),(6); Mannings, V. (7)
(1)OAA, Largo Enrico Fermi 5, 50125 Firenze, Italy,
(2)ISO Data Centre, Astrophysics Division, Villafranca del
Castillo, 28020 Madrid, Spain,
(3)IRAM, 300 rue de la Piscine, Domaine Universitaire, 38406 St
Martin d'Hères Cedex, France,
(4)NASA-Ames Research Center, Moffett Field, CA 94035, USA,
(5)Crimean Astrophysical Observatory, Crimea, 334413 Nauchny, Ukraine,
(6)St.Petersburgh University, St.Petersburg, 198904, Russia,
(7)SIRTF Science Center, Caltech, MS 314-6, Pasadena, CA 91125, USA
Abstract:
This paper presents state-of-the-art spectral energy distributions
(SEDs) of four Herbig Ae stars, based in part on new data in the mid
and far-infrared and at millimeter wavelengths. The SEDs are discussed
in the context of circumstellar disk models. We show that models of
irradiated disks provide a good fit to the observations over the whole
range of wavelengths. We offer a possible solution to the
long-standing puzzle caused by the excess emission of Herbig Ae stars,
where a large fraction of the stellar luminosity is re-radiated
between
and 7m, with a peak at about 3m. We
suggest that this general behaviour can be caused by dust evaporation
in disks where the gas component is optically thin to the stellar
radiation, as expected if the accretion rate in very low. The creation
of a puffed-up inner wall of optically thick dust at the dust
sublimation radius can account for the near-infrared characteristics
of the SEDs. It can also naturally explain the H and K band
interferometric observations of AB Aur (Millan-Gabet et al. 2001),
which reveal a ring of emission of radius AU. Finally,
irradiated disk models can easily explain the observed intensity of
the 10m silicate features and their variation from star to star.
Accepted for publication in A&A
Fuente, A. (1); Neri, R. (2); Martin-Pintado, J. (1);
Bachiller, R. (1); Rodriguez-Franco,
A. (1),(3),(4); Palla, F. (5)
(1)OAN (IGN), Campus Universitario, Apdo. 1143, 28800 Alcala de
Henares (Madrid), Spain,
(2)IRAM, 300 rue de la Piscine, Domaine Universitaire, 38406 St
Martin d'Hères Cedex, France,
(3)Universidad Complutense de Madrid, Av. Arcos de Jalon s/n,
28037 Madrid, Spain,
(4)NRO, Nobeyama, Minamimaki, Minamisaku, Nagano, 384-1305, Japan,
(5)OAA, Largo Enrico Fermi 5, 50125 Firenze, Italy
Abstract:
In order to study the existence and evolution of circumstellar disks
around intermediate-mass stars (M
), we have
obtained single-dish and interferometric continuum images at 2.6 mm
and 1.3 mm of the intermediate-mass protostar NGC7129FIRS2 and
of the Herbig Be stars LkH234 and HD200775. These objects
are representative of the different stages of the pre-main sequence
evolution with ages ranging from a few 103 to years.
Figure 5:
Molecular emission, dust and outflows in NGC 7129
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Single-dish and interferometric observations of the outflows
associated with these sources are also presented (Fig. 5). In
NGC7129FIRS2, two millimeter sources are required to fit the
interferometric 1.3 mm continuum emission. Only the most intense of
these millimeter objects, FIRS2-MM1, seems to be associated with
the CO outflow. The second and weaker source, FIRS2-MM2, does
not present any sign of stellar activity. The single-dish map of the
CO outflow presents an unusual morphology with the blue and red lobes
separated by an angle of 82.
The CO (J=1-0) interferometric
image shows that this unusual morphology is the result of the
superposition of two outflows, one of them associated with
FIRS2-MM1 (the blue lobe in the single-dish map) and the other
(the red lobe) with a new infrared source (FIRS2-IR) which is
not detected in the millimeter continuum images. The interferometric
1.3 mm continuum image of NGC7129FIRS1 reveals that
LkH234 is a member of a cluster of embedded objects. Two
millimeter clumps are detected in this far-infrared source. The
strongest is spatially coincident with the mid-infrared companion of
LkH234, IRS6. A new millimeter clump, FIRS1-MM1, is
detected at an offset (
-3.23'', 3.0'') from LkH234. We have
not detected any compact source towards LkH234 with a limit
for the mass of a circumstellar disk,
.
The comparison of the interferometric CO (J=1-0) and continuum images
reveals that IRS 6 very likely drives the energetic molecular outflow
detected towards NGC7129FIRS1 and the [SII] jet. The extremely
young object FIRS1-MM1 (it has not been detected in the near-and
mid-infrared) turns out to be the driving source of the H2 jet. There
is no evidence for the existence of a bipolar outflow associated with
LkH234. We have not detected 1.3 mm continuum emission towards
HD200775. Our observations imply a
upper limit of
for the mass of a circumstellar disk. This is the lowest
upper limit obtained so far in a Herbig Be star. Thus our observations
provide new important information on three protostars (IRS 6,
FIRS1-MM1 and FIRS2-MM1), one infrared star
(FIRS2-IR) and two Herbig Be stars.
The luminosities of the
protostars are consistent with being intermediate-mass objects
(
). They are surrounded by thick
envelopes with masses ranging between
and drive
energetic outflows. Circumstellar disks and bipolar outflows are not
detected toward the Herbig Be stars. We have obtained an upper limit
for the disk/stellar mass ratio,
,
of < 0.02 in
LkH234 and of < 0.0002 in HD200775. Our limit in
HD200775 implies that in evolved Herbig Be stars the
ratio is more than two orders of magnitude lower than in T Tauri and
Herbig Ae stars. We propose that in massive stars (
)
both the dispersal of the outer disk and the energetic
mass-loss, occur early in the stellar evolution before the star
becomes visible. Some mechanisms for the dispersal of the outer disk
are discussed.
Appeared in A&A 2001, 366, 873
Dominique Bockelée-Morvan(1), Nicolas Biver(1),
Raphaël Moreno(2), Pierre Colom(1),
Jacques Crovisier(1), Éric Gérard(1),
Florence Henry(1), Dariusz C. Lis(3),
Henry Matthews(4), H. A. Weaver(5),
Maria Womack(6), Michel C. Festou(7)
(1)Observatoire de Paris-Meudon, F-92195, Meudon, France,
(2)Institut de Radioastronomie Millimétrique, 300
rue de la Piscine, Domaine Universitaire, F-38406,
St Martin d'Hères Cedex, France,
(3)Department of Physics, California Institute of Technology,
MS 320-47, Pasadena, CA 91125, USA,
(4)Joint Astronomy Centre, 660 North A`ohoku Place, Hilo,
HI96720, USA,
(5)Johns Hopkins University, 3400 North Charles Street,
Baltimore, MD 21218-2686, USA,
(6)St. Cloud State University, 720 Fourth Ave. S, MS 324,
St. Cloud, MN 56301-4498, USA,
(7)Observatoire Midi-Pyrénées, 14 avenue Édouard Belin,
F-31400, Toulouse, France
Abstract:
Comet C/1999 S4 (LINEAR), which was discovered in September 1999,
passed perihelion on 26 July 2000 at 0.765 AU from the Sun. Around
that time, visual observations, confirmed by HST and VLT
high-resolution images, showed that the comet nucleus broke up into
many fragments that rapidly fizzled out. In mid-August, the comet no
longer existed. Thus this object belongs to this class of comets
which are disrupted for no apparent reason. Such events can inform us
on the internal structure and composition of the comet nuclei, but,
being unpredictable, they are difficult to observe.
We observed comet C/LINEAR at several radio telescopes (NRAO 12-m, CSO,
JCMT, IRAM 30-m and Nançay) as part of our continuing efforts to
expand our data sample used for comparative studies of cometary
composition. We had the chance to observe the comet at IRAM at the
very moment it underwent its major disruption, and to monitor its gas
production rate (using the HCN lines) during this event
(see Fig. 6).
A surge of gas was observed on 23 July followed by a rapid decrease.
An analysis of the observations indicates that a runaway fragmentation
of the nucleus may have begun around 18 July 2000 and proceeded until
23 July. The mass in small icy debris (
30 cm radius) was
comparable to the mass in the large fragments seen in optical images.
The mass budget after breakup suggests a small nucleus
(100-300 m radius), that had been losing debris for weeks.
The HNC, H2CO, H2S and CS abundances relative to H2O
measured during breakup are consistent with those obtained in other
comets, showing that freshly exposed ices from the inner nucleus have
a composition similar to the ices of the outer layers of the nucleus.
However, a deficiency in CH3OH and CO is observed.
Published in Science Magazine 292, 1339-1343
Figure 6:
The evolution of the HCN J(3-2) line at
265.9 GHz in comet C/1999 S4 (LINEAR), observed with the
IRAM 30-m telescope from July 18 to 26, 2000.
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