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Theoretical models of the planetary nebula populations in galaxies: The ISM oxygen abundance when star formation stops

M. G. Richer tex2html_wrap_inline334 , M. L. McCall tex2html_wrap_inline336 and N. Arimoto tex2html_wrap_inline338

tex2html_wrap_inline334 DAEC, Observatoire de Meudon, 5 Place Jules Janssen, F-92195 Meudon Cedex, France

tex2html_wrap_inline336 Dept. of Physics and Astronomy, York University, 4700 Keele Street, North York, Ontario, Canada M3J 1P3

tex2html_wrap_inline338 Institute of Astronomy, University of Tokyo, Mitaka, Tokyo 181, Japan

Using theoretical models of the planetary nebula populations in galaxies, we investigate whether the current oxygen abundances in bright planetary nebulae can be used to predict the oxygen abundance in the interstellar medium when star formation stopped. These models successfully reproduce a constant planetary nebula luminosity function (PNLF) peak luminosity, the PNLF shape in galaxies with and without star formation, and the mean densities and oxygen abundances observed in bright planetary nebulae in the Magellanic Clouds. To accomplish this, we had to couple the evolution of the nebular shell and the central star, and impose a mass-dependent nebular covering factor. In all galaxies, these models predict that a gap develops between the abundances observed in bright planetary nebulae and those in the interstellar medium when star formation stopped. This abundance gap depends primarily upon the oxygen abundance achieved in the interstellar medium when star formation stopped, though it also has some sensitivity to the history of star formation. The abundance gap is always less than 0.35 dex in these models. For the Milky Way, the predicted abundance gap, 0.14 dex, is identical to that observed.

Accepted by Astronomy & Astrophysics Supplements
Preprints can be obtained by contacting richer@mesunb.obspm.fr
or via anonnymous ftp on ftp://ftp.obspm.fr/transit/richer/compact5.ps.Z

NaI/KI scattering observations in circumstellar envelopes: contraints on ionization and mass-loss rates

Ch. Guilain tex2html_wrap_inline334 , N. Mauron tex2html_wrap_inline336

tex2html_wrap_inline334 Centre d'Etudes Spatiales des Rayonnements, CNRS/UPS, BP 4346, 31029 Toulouse Cedex, France

tex2html_wrap_inline336 GRAAL, CNRS/ Université de Montpellier II, CC072, Place Eugène Bataillon, 34095 Montpellier Cedex 05, France

We investigate KI or NaI fluorescent emission in circumstellar shells to study their ionization and mass-loss rates. First-time KI detections around the mira-type stars W Hya and R Hya are presented. Together with the previously analysed cases of tex2html_wrap_inline358  Ori, tex2html_wrap_inline358 Her and o Cet (Mauron and Caux 1992) and other observations, this gives an extended sample of 10 envelopes which includes tex2html_wrap_inline362 Cep, CE Tau, tex2html_wrap_inline364 Peg, tex2html_wrap_inline366 Per and g Her. A few non-detections are also considered.

In order to compare observed with expected values of KI intensities, the ionization model of Glassgold and Huggins (1986) is used, and the relevant parameters such as distance d, mass-loss rate tex2html_wrap_inline370 , gas temperature, fractional electron abundance tex2html_wrap_inline372 and stellar photoionizing rates tex2html_wrap_inline374 have to be known. Using data found in the literature, we estimate these parameters in detail for each case. The values of tex2html_wrap_inline372 are obtained with a hypothesized simple rule based on the circumstellar abundance of molecules and grains which could lock electron donors, giving either tex2html_wrap_inline372 tex2html_wrap_inline380 3 10 tex2html_wrap_inline382 or tex2html_wrap_inline380 2 10 tex2html_wrap_inline386 . The tex2html_wrap_inline374 values depend on the rare ultraviolet spectrophotometric data available for red giants. The kinetic temperature was assumed to be 30 K at the probed impact parameters tex2html_wrap_inline390 tex2html_wrap_inline380 0.5 to 5 10 tex2html_wrap_inline394  cm.

Despite real uncertainties, the predicted KI intensities with our best estimates of the parameters are in very reasonable agreement with observations in 8 cases in 10. The largest discrepancy concerns the red supergiant tex2html_wrap_inline362 Cep (M2Ia): our KI data suggest that, similar to tex2html_wrap_inline358  Ori, CO and dust are incompletely formed; for this object we favour tex2html_wrap_inline370 =5 10 tex2html_wrap_inline402   M tex2html_wrap_inline404 yr tex2html_wrap_inline406 . The wind of tex2html_wrap_inline364 Peg is the second case for which a larger mass-loss and/or a larger tex2html_wrap_inline372 than primarily believed is suggested, but confirming observations are needed. Finally there is no indication that K or Na might be depleted in silicate grains.

Accepted for publication in Astronomy and Astrophysics
For preprints, contact: mauron@merlin.graal.univ-montp2.fr

A survey of CN in circumstellar envelopes

R. Bachiller tex2html_wrap_inline334 , A. Fuente tex2html_wrap_inline334 , V. Bujarrabal tex2html_wrap_inline334 , F. Colomer tex2html_wrap_inline334 , C. Loup tex2html_wrap_inline336 , A. Omont tex2html_wrap_inline336 , and T. de Jong tex2html_wrap_inline338

tex2html_wrap_inline334 Observatorio Astronómico Nacional (IGN), Apartado 1143, E-28800 Alcalá de Henares, Madrid, Spain tex2html_wrap_inline336 Institut d'Astrophysique de Paris (CNRS), 98 bis Bd. Arago, F-75014 Paris, France tex2html_wrap_inline338 SRON, Space Research Groningen, P.O. Box 800, NL-9700 AV Groningen, The Netherlands

We have conducted a survey of CN N=2-1 and N=1-0 line emission in the envelopes of evolved stars. The sample consists of 42 objects, including C-rich and O-rich envelopes, S-stars, detached envelopes, and proto-planetary nebulae. Confident detections have been achieved in 30 objects. Both CN lines are bright in C-rich envelopes, and the 2-1 line has been detected in 5 O-rich objects (previously, CN had been detected in only one O-rich envelope). The excitation temperature tex2html_wrap_inline436 , evaluated from the 2-1/1-0 intensity ratio, is tex2html_wrap_inline380 3-6 K in most carbon stars, and tex2html_wrap_inline440 10-20 K in O-rich envelopes.

We find that the CN spectra display anomalies in the rotational, fine, and hyperfine line ratios. Anomalies in the rotational excitation appear in W Ori and UU Aur, two stars which are known to present HCN v=0 J=1-0 masers. The excitation of the CN 2-1 line is unusually high in both objects, and UU Aur may present a weak maser effect in this line. Anomalies are also observed in the intensity ratios of the fine and hyperfine components. If such anomalies were due to the envelope thickness, the required line opacities would be excessively high, in particular for low mass-loss rate objects. We thus suggest that the observed anomalies are the result of an anomalous excitation. Pumping through the optical and near-IR bands seems to play a dominant role in the CN excitation.

A comparison with previously published HCN data shows that the CN/HCN ratio of the total numbers of molecules in C-rich stars tends to be larger in the objects with lower mass-loss rate, supporting the idea that CN is mainly formed from the photodissociation of HCN. The average peak abundance of CN is tex2html_wrap_inline380 1.910 tex2html_wrap_inline386 in C-rich objects, and is about 300 times smaller ( tex2html_wrap_inline380 6.610 tex2html_wrap_inline452 ) in O-rich envelopes. The CN/HCN peak abundance ratio is tex2html_wrap_inline380 0.45 in C-rich stars, in agreement with photodissociation chemical models, and tex2html_wrap_inline380 0.04 in O-rich objects. This last value is about two orders of magnitude smaller than the predictions of standard chemical models, and suggest that CN is destroyed by additional mechanisms than photodissociation in O-rich envelopes.

Accepted for publication in Astronomy and Astrophysics
Preprints can be obtained by contacting Rafael Bachiller (bachiller@oan.es)
or via WWW on http://www.oan.es/preprints/lista.html
or via anonymous ftp on suncc.ll.iac.es then cd /pub/A3058

CS chemistry in the bipolar nebula CRL 2688

T. Kasuga tex2html_wrap_inline334 , I. Yamamura tex2html_wrap_inline336 and S. Deguchi tex2html_wrap_inline338

tex2html_wrap_inline334 Department of Instrument and Control Engineering, Hosei University, Kajino 3-7-2, Koganei, Tokyo 184, Japan

tex2html_wrap_inline336 Department of Astronomy, School of Science, University of Tokyo, Bunkyo, Tokyo 113, Japan

tex2html_wrap_inline338 Nobeyama Radio Observatory, National Astronomical Observatory, Minamimaki, Minamisaku, Nagano 384-13 , Japan

High spatial-resolution observations of the protoplanetary nebula CRL2688 were made by the CS J=1-0 and J=2-1 lines with the Nobeyama Millimeter Array with angular resolutions of 6'' tex2html_wrap_inline474 6'' and 3'' tex2html_wrap_inline474 3'' , respectively. The mapping observations reveal that strong CS peaks in the J=2-1 line are located symmetrically at both sides of the optical dark lane at the center, though the CS J=1-0 distribution is rather round. These CS peaks seem to be slightly misaligned from the optical bipolar axis. A modeling of the CRL 2688 envelope results that the density distribution is nearly spherically symmetric but the abundance of CS is enhanced near the polar regions. The increase of the CS abundance near the poles can be explained by the chemistry of sulfur containing molecules in the postshocked region in the high-velocity flow.

Accepted by Astronomy and Astrophysics on Sept. 17, 1996

Preprints can be obtained by contacting Shuji Deguchi (deguchi@nro.nao.ac.jp)

Superwind in evolved OH/IR stars

X.Delfosse tex2html_wrap_inline334 , C.Kahane tex2html_wrap_inline334 and T.Forveille tex2html_wrap_inline334

tex2html_wrap_inline334 Observatoire de Grenoble - B.P. 53 - F-38041 Grenoble Cedex 9 - France

We report observations of tex2html_wrap_inline492 CO (J=1-0) and (J=2-1) emission towards 5 evolved OH/IR envelopes. Four of them are known to have very weak CO emission compared to their infrared flux, and an anomalously high (J=2-1)/(J=1-0) intensity ratio. Modeling of their tex2html_wrap_inline494 CO and tex2html_wrap_inline492 CO lines is used to test several possible explanations of this behaviour. We conclude that it is most likely due to the recent onset of a superwind phase. Another interesting result of the modeling is the very low tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C isotopic ratios we derive in these envelopes, of the order of 3.5 and close to the equilibrium value of the CNO cycle. We interpret this as the signature of massive stars at the end of their AGB phase. The sixth envelope, which shows a much lower (J=2-1)/(J=1-0) intensity ratio, also has a low, marginally larger, tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C isotopic ratio. We conclude that it also is a massive object, but in a slightly less evolved stage, just before the superwind phase.

Accepted by Astronomy and Astrophysics
Preprints can be obtained by contacting delfosse@gag.observ-gr.fr

Measurement of the tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C ratio in Planetary Nebulae

R. E. S. Clegg tex2html_wrap_inline510 , P. J. Storey tex2html_wrap_inline338 , J. R. Walsh tex2html_wrap_inline514 & L. Neale tex2html_wrap_inline338

tex2html_wrap_inline334 Royal Greenwich Observatory, Madingley Rd., Cambridge CB3 0EZ, UK
tex2html_wrap_inline336 Present address: Particle Physics and Astronomy Research Council, Polaris House, North Star Avenue, Swindon, SN2 1SZ, UK
tex2html_wrap_inline338 Department of Physics & Astronomy, University College London, Gower St., London WC1E 6BT, UK
tex2html_wrap_inline514 ST-ECF, European Southern Observatory, Karl-Schwarzchild Str. 2, D-85748 Garching bei München, Germany.

The tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C isotope ratio in the ionized gas in three planetary nebulae has been measured using a new method based on transitions caused by hyperfine effects. The C III] multiplet near 1908Å has an F= tex2html_wrap_inline530 - tex2html_wrap_inline530 transition at 1909.6Å completely forbidden in tex2html_wrap_inline494 C, but allowed as a result of the non-zero nuclear spin of tex2html_wrap_inline492 C. The transition probability for the tex2html_wrap_inline492 C tex2html_wrap_inline540 P tex2html_wrap_inline542 - tex2html_wrap_inline544 S tex2html_wrap_inline546 transition was calculated in a multi-configuration basis and found to be tex2html_wrap_inline548 s tex2html_wrap_inline550 . The Goddard High Resolution Spectrograph aboard the Hubble Space Telescope was used to observe this transition in three nebulae. The tex2html_wrap_inline492 C line was detected in two C rich nebulae: NGC 3918 and SMC N2. The wavelength of the tex2html_wrap_inline492 C tex2html_wrap_inline540 P tex2html_wrap_inline542 - tex2html_wrap_inline544 S tex2html_wrap_inline546 transition in NGC 3918 was found to be displaced by tex2html_wrap_inline564 km s tex2html_wrap_inline550 from that determined from the experimental energies of the tex2html_wrap_inline494 C tex2html_wrap_inline338 P tex2html_wrap_inline542 and tex2html_wrap_inline334 S tex2html_wrap_inline546 states; this displacement is attributed to an isotope shift. The tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C abundance ratio was determined to be tex2html_wrap_inline582 in NGC 3918 and 21 tex2html_wrap_inline584 11 in SMC N2. In the Type I nebula LMC N122, which was found to have C III] tex2html_wrap_inline338 P tex2html_wrap_inline588 - tex2html_wrap_inline334 S velocity components over a range of 230 kms tex2html_wrap_inline550 , a tentative detection of tex2html_wrap_inline492 C was made, indicating a low value of the tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C ratio. The tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C ratio in these nebulae is lower than the typical range of values in carbon stars, excepting the very tex2html_wrap_inline492 C-rich stars. The implications of these new tex2html_wrap_inline494 C/ tex2html_wrap_inline492 C determinations for models of AGB evolution and dredge-up are discussed.

Accepted by MNRAS
Preprints can be obtained by contacting jrw@eso.org

The evolution of ultraviolet emission lines
from circumstellar material surrounding SN 1987A

George Sonneborn tex2html_wrap_inline510 , Claes Fransson tex2html_wrap_inline338 , Peter Lundqvist tex2html_wrap_inline338 , Angelo Cassatella tex2html_wrap_inline514 , Roberto Gilmozzi tex2html_wrap_inline618 ,
Robert P. Kirshner tex2html_wrap_inline620 , Nino Panagia tex2html_wrap_inline622 , and Willem Wamsteker tex2html_wrap_inline624

tex2html_wrap_inline334 Laboratory for Astronomy and Solar Physics, Code 681, NASA/Goddard Space Flight Center, Greenbelt, MD 20771
tex2html_wrap_inline336 Institut d'Astrophysique de Paris, 98bis boulevard Arago, 75014 Paris, France
tex2html_wrap_inline338 Stockholm Observatory, S-133 36 Saltsjöbaden, Sweden
tex2html_wrap_inline514 Istituto di Astrofisica Spaziale, CNR, CP 67, I-00044, Frascati, Italy
tex2html_wrap_inline618 European Southern Observatory, Karl-Schwarzschild Str. 2, 85748 Garching bei München, Germany
tex2html_wrap_inline620 Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138
tex2html_wrap_inline638 Space Telescope Science Institute, 3700 San Martin Dr., Baltimore, MD 21218
tex2html_wrap_inline640 Affiliated with the Astrophysics Division, Space Sciences Department of ESA
tex2html_wrap_inline624 IUE Observatory, ESA-VILSPA, Casilla 50727, E-28080 Madrid, Spain

The presence of narrow high-temperature emission lines from nitrogen-rich gas close to SN 1987A has been a principal observational constraint on the evolutionary status of the supernova's progenitor. A new analysis of the complete five-year set of low and high resolution IUE ultraviolet spectra of SN 1987A (1987.2-1992.3) provide fluxes for the N V 1240, N IV] 1486, He II 1640, O III] 1665, N III] 1751, and C III] 1908 lines with significantly reduced random and systematic errors and reveals significant short-term fluctuations in the light curves. The N V, N IV], and N III] lines turn on sequentially over 15 to 20 days and show a progression from high to low ionization potential, implying an ionization gradient in the emitting region. The line emission turns on suddenly at tex2html_wrap_inline644 days after the explosion, as defined by N IV]. The N III] line reaches peak luminosity at tex2html_wrap_inline646 days. A ring radius of tex2html_wrap_inline648 and inclination of tex2html_wrap_inline650 degrees is derived from these times, assuming a circular ring. The probable role of resonant scattering in the N V light curve introduces systematic errors that leads us to exclude this line from the timing analysis. A new nebular analysis yields improved CNO abundance ratios of N/C tex2html_wrap_inline652 and N/O tex2html_wrap_inline654 , confirming the nitrogen enrichment found in our previous paper. From the late-time behavior of the light curves we find that the emission originates from progressively lower density gas and that the emitting region has a multi-component density structure. We estimate the emitting mass near maximum tex2html_wrap_inline656 days) to be tex2html_wrap_inline658 solar masses, assuming a filling factor of unity and an electron density of tex2html_wrap_inline660 . These results are discussed in the context of current models for the emission and hydrodynamics of the ring.

Accepted by The Astrophysical Journal.
For preprints, contact sonneborn@fornax.gsfc.nasa.gov

The ISO LWS grating spectrum of NGC7027

X.-W. Liu plus 41 co-authors

Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, UK

We present a high signal-to-noise ISO Long Wavelength Spectrometer (LWS) grating spectrum of the planetary nebula NGC7027 from 43-194 tex2html_wrap_inline362 m. In total 40 emission lines have been detected, with 30 identified. From the ionized region, we observe fine-structure lines from [N II], [N III] and [O III]. The [O I] and [C II] fine-structure lines from the photodissociation region are the strongest features observed in this spectral region. Amongst the molecular lines, 11 pure rotation CO lines from J=14-13 up to J=24-23 have been detected. The most striking result, however, is the detection in this carbon-rich nebula of the o-H tex2html_wrap_inline664 O 179.53 tex2html_wrap_inline362 m and the OH 119.3 tex2html_wrap_inline362 m fundamental lines. Astrophysical implications are briefly discussed.

Accepted by A&A
For preprints, contact xwl@star.ucl.ac.uk

Wind fluctuations observed for the [WC9] nucleus of the planetary nebula BD+30 tex2html_wrap_inline670 3639

A. Acker tex2html_wrap_inline334 , Y. Grosdidier tex2html_wrap_inline510 and S. Durand tex2html_wrap_inline334

tex2html_wrap_inline334 URA 1280, Equipe évolution galactique, Observatoire de Strasbourg, 11 rue de l'Université, F-67000 Strasbourg, France

tex2html_wrap_inline336 Département de Physique, Université de Montréal, CP 6128, Montréal, Québec, H3C3J7, Canada

The CIII and CIV lines in the [WC9] spectrum of BD+30 tex2html_wrap_inline670 3639 show variable features, interpreted in terms of radiative acceleration of "blobs" forming in the wind. The variations are like those observed for the WC9 massive stars, and the blobs accceleration appears smaller than for the [WC8] nucleus of NGC 40.

Accepted by A&A Lett.
Preprints can be obtained by contacting acker@cdsxb6.u-strasbg.fr

Variability and nature of the binary in the Red Rectangle Nebula

C. Waelkens tex2html_wrap_inline334 , H. Van Winckel tex2html_wrap_inline334 , L.B.F.M. Waters tex2html_wrap_inline688 , E.J. Bakker tex2html_wrap_inline690

tex2html_wrap_inline334 Instituut voor Sterrenkunde, Celestijnenlaan 200B, 3001 Heverlee
tex2html_wrap_inline336 Astronomisch Instituut, Universiteit van Amsterdam, Kruislaan 403, 1098 SJ Amsterdam, The Netherlands
tex2html_wrap_inline338 SRON Groningen, P.O. Box 800, 9700 AV Groningen, The Netherlands
tex2html_wrap_inline514 SRON Utrecht, Sorbonnelaan 2, 3584 CA Utrecht, The Netherlands
tex2html_wrap_inline618 Astronomical Institute, University of Utrecht, P.O. Box 80000, 3508 TA Utrecht, The Netherlands

We present new observations of the central binary inside the Red Rectangle nebula. The detection of zinc in the optical spectrum confirms that the peculiar photospheric abundances are due to accretion of circumstellar gas. Grey brightness variations with the orbital period are observed. They are interpreted as being due to the variation of the scattering angle with orbital phase. The small orbital separation of the system is not compatible with previous normal evolution of the primary on the AGB. We point out the similarity of the orbital history of this and other similar systems with those of some close Barium stars and suggest that the nonzero eccentricity of the orbit is the result of tidal interaction with the circumbinary disk.

Accepted by Astronomy and Astrophysics Letters

Preprints can be obtained by contacting hans@ster.kuleuven.ac.be

A detached dust shell surrounding the J-type carbon star
Y Canum Venaticorum

H. Izumiura tex2html_wrap_inline334 , O. Hashimoto tex2html_wrap_inline336 , K. Kawara tex2html_wrap_inline706 , I. Yamamura tex2html_wrap_inline708 , and L.B.F.M. Waters tex2html_wrap_inline710

tex2html_wrap_inline334 Okayama Astrophysical Observatory, National Astronomical Observatory, Kamogata, Asakuchi, Okayama 719-02, Japan

tex2html_wrap_inline336 Department of Applied Physics, Seikei University, 3 Kichijojikita, Musashino, Tokyo 180, Japan

tex2html_wrap_inline338 Institute of Space and Astronautical Science, 3-1-1 Yoshinodai, Sagamihara, Kanagawa 229, Japan

tex2html_wrap_inline514 ISO Science Operations Centre, Astrophysics Division of ESA, Villafranca, 28080 Madrid, Spain

tex2html_wrap_inline618 Institute of Astronomy, Faculty of Science, The University of Tokyo, 2-21-1 Osawa, Mitaka, Tokyo 181, Japan

tex2html_wrap_inline620 SRON Laboratory for Space Research Groningen, P.O. Box 800, NL-9700 AV Groningen, The Netherlands

tex2html_wrap_inline638 Astronomical Institute `Anton Pannekoek', University of Amsterdam, Kruislaan 403, NL-1098 SJ Amsterdam, The Netherlands

This paper reports the first clear detection of a detached dust shell surrounding the prototypical J-type carbon star Y CVn in 90 tex2html_wrap_inline362 m and 160 tex2html_wrap_inline362 m maps taken with the ISO/ISOPHOT tex2html_wrap_inline730 The projected inner radius of the shell is 180''-190'', corresponding to (6.4-7.1)10 tex2html_wrap_inline738  cm at a distance of 250 pc. The shell thickness is obtained to be (2-5)10 tex2html_wrap_inline738  cm. The mass-loss rate at the formation of the shell is estimated to be in the range (7-20)10 tex2html_wrap_inline402 M tex2html_wrap_inline404  yr tex2html_wrap_inline550 , about two orders of magnitude higher than the present-day mass-loss rate derived from CO gas observations. The obtained mass in the shell is (4-14)10 tex2html_wrap_inline754 M tex2html_wrap_inline404 . It is concluded that the mass-loss rate decreased by two orders of magnitude on a short time scale 1.410 tex2html_wrap_inline514 years ago assuming an average shell expansion velocity of 15 km s tex2html_wrap_inline550 , and that Y CVn has been staying at the low mass-loss state. The duration of the previous higher mass-loss phase would be at most 210 tex2html_wrap_inline514  years even if the asymmetry in the shell geometry is taken into account. The evolutionary status of Y CVn is also discussed.

tex2html_wrap_inline730 Based on observations with ISO, an ESA project with instruments funded by ESA Member States (especially the PI countries: France, Germany, the Netherlands and the United Kingdom) and with the participation of ISAS and NASA.

Accepted by Astronomy and Astrophysics, ISO special issue
Preprints can be obtained by contacting izumiura@oao.nao.ac.jp
or via WWW on http://isowww.estec.esa.nl:80/ISO/AandA/

Detection of a new linear carbon chain radical: C tex2html_wrap_inline770 H

M. Guélin tex2html_wrap_inline334 , J. Cernicharo tex2html_wrap_inline336 , M.J. Travers tex2html_wrap_inline338 , M.C. McCarthy tex2html_wrap_inline338 , C.A. Gottlieb tex2html_wrap_inline338 , P. Thaddeus tex2html_wrap_inline338 , M. Ohishi tex2html_wrap_inline514 , S. Saito tex2html_wrap_inline618 , S. Yamamoto tex2html_wrap_inline620

tex2html_wrap_inline334 IRAM, 300 Rue de la piscine, F-38406 S tex2html_wrap_inline792 Martin d'Hères, France

tex2html_wrap_inline336 Observatorio Astronomico Nacional, apartado 1143, E-28800 Alcalá de Henares, Spain

tex2html_wrap_inline338 Division of Applied Sciences, Harvard University, Cambridge, MA 02138, USA

tex2html_wrap_inline514 N. R. O., Minamimaki, Minamisaku, Nagano 384-13, Japan

tex2html_wrap_inline618 Institute for Molecular Science, Myodaiji, Okazaki 444, Japan

Following our discovery of C tex2html_wrap_inline802 H in IRC+10216 (Cernicharo & Guelin 1996), we report the detection in this circumstellar envelope of another linear carbon chain radical, C tex2html_wrap_inline770 H. The microwave spectrum of C tex2html_wrap_inline770 H has been recently observed in the laboratory and its rotational line frequencies are precisely known.

With this new detection, the family of acetylenic chain radicals (C tex2html_wrap_inline808 H) observed in space is complete up to n= 8. The members with even numbers of carbon atoms are consistently more abundant than the odd number members; C tex2html_wrap_inline770 H is found to be a factor of 4 less abundant than C tex2html_wrap_inline802 H and a factor of 20 less abundant than C tex2html_wrap_inline816 H.

Accepted by Astron. Astrophys. (Letters)
Preprints can be obtained by contacting guelin@iram.fr

The rich far-infrared water vapour spectrum of W Hya

M. J. Barlow tex2html_wrap_inline334 and 42 co-authors

tex2html_wrap_inline334 Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT

We present an ISO Long Wavelength Spectrometer (LWS) grating spectrum of the oxygen-rich AGB star W Hya from 43-197 tex2html_wrap_inline362 m. The spectrum is dominated by a forest of water vapour emission lines, confirming that H tex2html_wrap_inline664 O molecules are the dominant coolants of the winds of these stars. We have constructed an outflow model for the H tex2html_wrap_inline664 O spectrum of W Hya, which successfully matches the fluxes of most of the observed H tex2html_wrap_inline664 O lines, using an adopted wind temperature profile. These fits are sensitive to the mass loss rate, to the H tex2html_wrap_inline664 O abundance and to the inner radius of the H tex2html_wrap_inline664 O emitting region. The best fit parameters correspond to a mass loss rate of 6 tex2html_wrap_inline834  M tex2html_wrap_inline404  yr tex2html_wrap_inline550 , inner and outer radii for the emitting region of tex2html_wrap_inline840 and tex2html_wrap_inline842 cm, and a H tex2html_wrap_inline664 O/H tex2html_wrap_inline664 abundance of tex2html_wrap_inline848 for tex2html_wrap_inline850 cm and tex2html_wrap_inline852 at large radii. A decrease of the H tex2html_wrap_inline664 O/H tex2html_wrap_inline664 abundance in the outer envelope is consistent with the predictions of photochemical models. The availability for the first time of observations of the line fluxes from the dominant coolant species should enable improved models of the wind temperature distribution to be produced.

Accepted by Astronomy and Astrophysics
Preprints can be obtained by contacting mjb@star.ucl.ac.uk



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