<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
<record>
  <controlfield tag="001">1929</controlfield>
  <controlfield tag="005">20160701171655.0</controlfield>
  <datafield tag="024" ind1="7" ind2=" ">
    <subfield code="a">10.1051/0004-6361:20030724</subfield>
    <subfield code="2">DOI</subfield>
  </datafield>
  <datafield tag="037" ind1=" " ind2=" ">
    <subfield code="a">ASTROimport-86</subfield>
  </datafield>
  <datafield tag="100" ind1=" " ind2=" ">
    <subfield code="a">Van de Steene, G. C.</subfield>
  </datafield>
  <datafield tag="260" ind1=" " ind2=" ">
    <subfield code="c">2003</subfield>
  </datafield>
  <datafield tag="245" ind1=" " ind2=" ">
    <subfield code="a">Shock emission in the bipolar post-AGB star IRAS 16594-4656</subfield>
  </datafield>
  <datafield tag="520" ind1=" " ind2=" ">
    <subfield code="a">In this paper we study the near-infrared emission spectrum of IRAS 16594-4656, a bipolar post-AGB star with spectral type B7 and no observed ionization. Using optical and near-infrared photometry we determined the total extinction towards this object to be AV= 7.5+/-0.4 mag and derived a distance of 2.2+/-0.4 kpc, assuming a luminosity of 104 Lsun. The near-infrared spectrum shows strong H2 emission lines and some typical metastable shock excited lines such as [Fe II] 1.257  1.644 mu m. We determined the rotational and vibrational excitation temperatures, as well as the ortho-to-para ratio of the molecular hydrogen. Based on these we argue that the H2 emission is mainly collisionally excited. Line ratios indicate that the H2 emission originates in a  ~ 25 km s-1 C-type shock. On the other hand, the metastable lines, and especially the [Fe II] emission lines, indicate the presence of a  ~ 75 km s-1 J-type shock. Hence we postulate that the H2 emission originates where the stellar wind (with an observed terminal velocity of  ~ 126 km s-1) is funneled through an equatorial density enhancement, impinging almost tangentially upon the circumstellar material. The [Fe II] emission either occurs along the walls of the bipolar lobes where the transverse shock velocity would be higher, or could originate much closer to the central star in shocks in the post-AGB wind itself, or possibly even an accretion disk. Further high resolution near-infrared spectra are currently being obtained to confirm the proposed geometry and kinematics. Based on observations collected at the European Southern Observatory, Chile (proposal No. 61.C-0567). </subfield>
  </datafield>
  <datafield tag="700" ind1=" " ind2=" ">
    <subfield code="a"> van Hoof, P. A. M.</subfield>
  </datafield>
  <datafield tag="773" ind1=" " ind2=" ">
    <subfield code="p">Astronomy and Astrophysics</subfield>
    <subfield code="v">406</subfield>
    <subfield code="y">2003</subfield>
    <subfield code="c">773-781</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="2">
    <subfield code="a">http://esoads.eso.org/abs/2003A%26A...406..773V</subfield>
  </datafield>
  <datafield tag="905" ind1=" " ind2=" ">
    <subfield code="a">published in</subfield>
  </datafield>
  <datafield tag="980" ind1=" " ind2=" ">
    <subfield code="a">REFERD</subfield>
  </datafield>
</record>
</collection>