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    <title>MPIA Picture of the month</title>
    <link>http://www.mpia-hd.mpg.de/PSF/potm.php</link>
    <description>Picture of the Month of the Max-Planck-Institue for Astronomy in Heidelberg, Germany</description>
    <generator>by hand</generator>
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    <item>
      <title>Massive star formation</title>
      <link>http://www.mpia.de/PSF/potm.php?date=0310</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=0310</guid>
      <pubDate>Fri, 26 Feb 2010 10:30:00 +0100</pubDate>
      <description>
        &lt;p align=&quot;left&quot;&gt;
        &lt;a href=&quot;POTM0310/potm0310.jpg&quot;&gt;&lt;img src=&quot;potm/POTM0310/potm0310_s.jpg&quot; alt=&quot;image&quot; width=&quot;30%&quot;&gt;&lt;/a&gt;
        &lt;/p&gt;
        &lt;b&gt;Legend:&lt;/b&gt;
        &lt;table&gt;
        &lt;tr&gt;&lt;td&gt;Contour lines&lt;/td&gt;&lt;td&gt;=&lt;/td&gt;&lt;td&gt;Gas-density&lt;/td&gt;&lt;/tr&gt;
        &lt;tr&gt;&lt;td&gt;Colors&lt;/td&gt;&lt;td&gt;=&lt;/td&gt;&lt;td&gt;Temperature&lt;/td&gt;&lt;/tr&gt;
        &lt;/table&gt;
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        &lt;b&gt;Description:&lt;/b&gt;&lt;br&gt;
        In the related research project (&lt;a href=&quot;http://www.mpia-hd.mpg.de/~kuiper/research_msf.php&quot;&gt;MSF&lt;/a&gt;), we investigate the role of the radiation pressure onto the formation of massive stars. Potentially, the strong radiation pressure of a massive star inhibits further accretion onto its surface; such an intrinsic process would e.g. give an upper mass limit for stars in general.
        &lt;br&gt;
        The image illustrates a snapshot of a high-resolution radiation hydrodynamics simulation of the collapse of a pre-stellar core of cold gas and dust of 120 solar masses. In the center of the core, a new star is born during the free-fall epoch of the collapsing core. Afterwards the newborn star gains further mass from an accretion disk, which formed due to angular momentum conservation from the initially slowly rotating core.
        &lt;br&gt;
        After some while, the luminosity of the massive star has increased so much, that the resulting radiation pressure drags the in-falling mass from the bipolar direction into outer space. The concentrated opaque density of the accretion disk (the blue region) hampers the radiation pressure in this midplane layer at this point in time.
        &lt;br&gt;
        At the point when the accretion from the envelope region onto the disk has sufficiently decreased, the accretion disk looses its opaqueness and without this shielding effect the radiation pressure of the star starts to clear also the midplane layer.
        &lt;br&gt;
        In the end, the final star has accreted approximately 56.5 solar masses.
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        &lt;b&gt;Authors:&lt;/b&gt;
        &lt;br&gt;
        Rolf Kuiper
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        &lt;b&gt;More information:&lt;/b&gt;
        &lt;br&gt;
        &lt;a href=&quot;http://www.mpia-hd.mpg.de/~kuiper&quot;&gt;Homepage of the author&lt;/a&gt;&lt;br&gt;
        &lt;a href=&quot;http://www.mpia-hd.mpg.de/~kuiper/movies_2D.php&quot;&gt;Scientific background&lt;/a&gt;&lt;br&gt;
        &lt;a href=&quot;http://www.youtube.com/user/RolfKuiper&quot;&gt;YouTube channel&lt;/a&gt;
	  </description>
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    <item>
      <title>Anchoring Magnetic Field in Turbulent Molecular Clouds</title>
      <link>http://www.mpia.de/PSF/potm.php?date=1209</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=1209</guid>
      <pubDate>Wed, 03 Dec 2009 13:12:00 +0100</pubDate>
      <description>
        &lt;p align=&quot;left&quot;&gt;
        &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM1209/potm1209.jpg&quot;&gt;&lt;img src=&quot;http://www.mpia.de/PSF/potm/POTM1209/potm1209_s.jpg&quot; alt=&quot;image&quot; width=&quot;30%&quot;&gt;&lt;/a&gt;
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        The background image shows the far-infrared map in representative color and logarithmic scale. Superposed on it are the magnetic field directions inferred from optical polarimetry data (blue lines) tracing the diffused regions. The average of all the optical data is shown as the thick gray line. Magnetic fields within eight high-density cloud cores (labels A through H on the background map) are mapped using submillimeter polarimetry and the results are shown as insets, using red lines on individual representative-color intensity maps. The average direction of each core is shown as a white line superposed on the core map; these white lines also are plotted on the background map. Even though the core separations exceed the core sizes by as much as a factor of 100, they are for the most part "magnetically connected", i.e. the cores' average field directions are similar. Moreover, these directions are close to the average field direction seen in the diffused regions, as seen in a cloud simulation with sub-Alfvenic turbulence.
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        &lt;b&gt;Authors:&lt;/b&gt;
        &lt;br&gt;
        Hua-bai Li (MPIA); Darren Dowell (JPL/Caltech); Alyssa Goodman (CfA); Roger Hildebrand (U. Chicago); and Giles Novak (Northwestern U.)
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        &lt;b&gt;Reference:&lt;/b&gt;
        &lt;br&gt;
        &lt;a href=&quot;http://adsabs.harvard.edu/abs/2009ApJ...704..891L&quot;&gt;Link to the article&lt;/a&gt;
        &lt;/p&gt;
	  </description>
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    </item>

    <item>
      <title>Clustering in massive star forming regions</title>
      <link>http://www.mpia.de/PSF/potm.php?date=1009</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=1009</guid>
      <pubDate>Mon, 05 Oct 2009 11:05:00 +0100</pubDate>
      <description>
        &lt;p align=&quot;left&quot;&gt;
        &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM1009/potm1009.jpg&quot;&gt;&lt;img src=&quot;http://www.mpia.de/PSF/potm/POTM1009/potm1009_s.jpg&quot; alt=&quot;image&quot; width=&quot;30%&quot;&gt;&lt;/a&gt;
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        Despite their importance, the formation and early evolution of massive mass stars (more massive than 8 times the mass of the Sun) is not well understood. The formation and early evolution of high-mass stars happens in clustered and highly complex environments, where the forming stars and the molecular cloud are mutually interacting.  To properly understand the role of the cluster in the formation of massive stars we need to investigate the complete stellar content of these regions. This figure shows a Spitzer/IRAC image of RCW 34, a massive star-forming region (blue: 3.6 micron, green: 4.5 micron, red: 8 micron) located in the Vela Molecular Cloud.  A large bubble has been detected on the IRAC images in which a cluster of intermediate- and low-mass class II objects is found. Surprisingly, the massive stars are not present in the center of the bubble, but at the northern edge only, where an HII region is located, ionized by 3 massive stars.  North of the HII region, a dense molecular cloud is detected where current star formation is still taking place.  To explain this unusual location of the massive stars we have to conclude that this complex region is not formed in one star formation event, but the large bubble is formed first, and only after that the massive stars are formed. Currently, the stars inside the molecular cloud north of the bubble are still forming.
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        &lt;b&gt;Authors:&lt;/b&gt;
        &lt;br&gt;
        Arjan Bik, Thomas Henning, Tatiana Vasyunina, Henrik Beuther, Hendrik Linz, paper submitted
        &lt;/p&gt;
	  </description>
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    </item>

    <item>
      <title>Large Rotational Structure in a Massive Star Formation Region</title>
      <link>http://www.mpia.de/PSF/potm.php?date=0809</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=0809</guid>
      <pubDate>Fri, 31 Aug 2009 15:52:00 +0100</pubDate>
      <description>
        &lt;p align=&quot;left&quot;&gt;
        &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM0809/potm0809.pdf&quot;&gt;&lt;img src=&quot;http://www.mpia.de/PSF/potm/POTM0809/potm0809_s.jpg&quot; alt=&quot;image&quot; width=&quot;30%&quot;&gt;&lt;/a&gt;
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        These are velocity moment maps of three different higher density molecular tracers.  At each spatial position, a velocity moment map plots the intensity weighted velocity of the respective line from that location. The source, IRDC 18223-3 is at the beginning of the massive star formation process.  We first identified the outflow orientation using 12CO to be in the northwest-southeast direction (indicated on the plots with arrows). All of these molecules exhibit a velocity gradient that is not aligned with that outflow orientation.  We suspect that C18O may be influenced by the outflow, but the other lines show a velocity gradient perpendicular to the outflow orientation.  This is indicative of rotation perpendicular to the outflow likely resulting from a large rotating and infalling envelope (diameter ~28,000 AU) that may harbor a smaller Keplerian disk within.
        &lt;/p&gt;
	  </description>
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    </item>

    <item>
      <title>Open House at MPIA</title>
      <link>http://www.mpia.de/PSF/potm.php?date=0509</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=0509</guid>
      <pubDate>Wed, 28 May 2009 16:13:00 +0100</pubDate>
      <description>
        &lt;p align=&quot;center&quot;&gt;
        &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM0509/potm0509.jpg&quot;&gt;&lt;img src=&quot;http://www.mpia.de/PSF/potm/POTM0509/potm0509_s.jpg&quot; alt=&quot;image&quot; width=&quot;10%&quot;&gt;&lt;/a&gt;
        &lt;/p&gt;
        &lt;p align=&quot;justify&quot;&gt;
        Sunday, March 17 was Open House Day at the Max-Planck-Institute for Astronomy. Around 5000 visitors took the effort of getting up on the hill to look at exhibitions, try out experiments, listen to talks or to talk to the astronomers.&lt;br/&gt;&lt;br/&gt;
        The PSF department has contributed many public talks, a corner with experiments, video presentations and posters and a ''timeline'' of 9 posters describing the various aspects of planet and star formation.&lt;br/&gt;&lt;br/&gt;
        Due to the enormous interest in these posters, we have decided to make them available on this page (click on the images below for hi-res pdf files). You can find also a link to a &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM0509/movie/index.php&quot; alt=&quot;link to TdoT-video website&quot;&gt;video&lt;/a&gt; showing some impressions of the Open House Day 2009.
        &lt;/p&gt;
	  </description>
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    </item>

    <item>
      <title>Vortices as efficient particle traps</title>
      <link>http://www.mpia.de/PSF/potm.php?date=0409</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=0409</guid>
      <pubDate>Wed, 1 Apr 2009 14:25:00 +0100</pubDate>
      <description>
      To date, 344 exoplanets have been found from which 89 are in multiple-planet systems. There are altogether 37 systems with more than 1 detected planet (&lt;a href="http://www.exoplanet.eu"&gt;www.exoplanet.eu&lt;/a&gt;). The question naturally arises whether the formation of a first planet helps to form other planets in the system?&lt;br&gt;
      Would these multiple systems be frequent or rare?&lt;br&gt;
      A giant planet opens up a gap in the disk. Also vortices can form at the outer edges of the gap, if the disk is not too turbulent. These vortices then merge and soon there will be one big vortex at the outer edge of the gap, and a smaller one at the inner edge of the gap. These vortices can trap the dust particles and if the relative velocity between these particles are low enough, they will collide and grow producing planet cores.
      &lt;br&gt;
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm.php?date=0409&quot;&gt;read more&lt;/a&gt;
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM0409/potm0409_s.jpg&quot;&gt;&lt;img
      src=&quot;http://www.mpia.de/PSF/potm/POTM0409/potm0409_s.jpg&quot; style=&quot;float:left; padding-right:10px; padding-bottom:10px; width:100px;&quot;/&gt;&lt;/a&gt;
	  </description>
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    </item>

    <item>
      <title>A possible environment for planet formation</title>
      <link>http://www.mpia.de/PSF/potm.php?date=0309</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=0309</guid>
      <pubDate>Wed, 4 Mar 2009 13:01:00 +0100</pubDate>
      <description>
      Protoplanetary disks are often tought to be turbulent and having a pressure that decreases
      with radius. This scenario leads to inward drift of the particles (due to the pressure gradient)
      and to fragmentation of the particles (due to the turbulence).
      &lt;br&gt;
      &lt;br&gt;
      One possible way to keep particles growing in the disk are so called dead zones. The turbulence is driven
      by magnetic fields which couple to the ionized gas. Reducing the ionization fraction can
      cause the turbulence to stop working. Gas therefore accumulates in dead zones. If this causes a pressure
      bump, particles will stop drifting, once they reach the dead zone.
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm.php?date=0309&quot;&gt;read more&lt;/a&gt;
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM0309/potm0309.jpg&quot;&gt;&lt;img
      src=&quot;http://www.mpia.de/PSF/potm/POTM0309/potm0309_s.jpg&quot; style=&quot;float:left; padding-right:10px; padding-bottom:10px; width:100px;&quot;/&gt;&lt;/a&gt;
	  </description>
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    </item>

    <item>
      <title>[Ne II] emission in T Tau</title>
      <link>http://www.mpia.de/PSF/potm.php?date=0209</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=0209</guid>
      <pubDate>Tue, 10 Feb 2009 12:18:00 +0100</pubDate>
      <description>
      Emission from ionized neon in the 12.81 micrometer [Ne II] line is observed
      towards many young stars. It has been thought to originate in the surface of
      their circumstellar disks, which are irradiated by X-rays from the central star.
      However, an alternative emission mechanism has been proposed: [Ne II] production
      in shocks occuring e.g. in jets.
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm.php?date=0209&quot;&gt;read more&lt;/a&gt;
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM0209/potm0209.jpg&quot;&gt;&lt;img
      src=&quot;http://www.mpia.de/PSF/potm/POTM0209/potm0209_s.jpg&quot; style=&quot;float:left; padding-right:10px; padding-bottom:10px; width:100px;&quot;/&gt;&lt;/a&gt;
	  </description>
      <enclosure url="http://www.mpia.de/PSF/potm/POTM0209/potm0209.jpg" length="95716" type="image/jpg"/>
    </item>

    <item>
      <title>Brown Dwarfs Don't Hang Out With Stars</title>
      <link>http://www.mpia.de/PSF/potm.php?date=0109</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=0109</guid>
      <pubDate>Fri, 09 Jan 2009 16:22:00 +0100</pubDate>
      <description>
		This pair of NASA Hubble Space Telescope images of the binary brown dwarf
		Kelu-1 trace the orbital motion of the two stars over a seven-year span as
		photographed by the Near Infrared Camera and Multi-Object Spectrometer
		(NICMOS) on Hubble.
	    &lt;br&gt;&lt;br&gt;
		In 1998, the &quot;stars&quot; were too close together to be resolved by Hubble. By
		2005, they had moved apart to a separation of 520 million miles. The
		projected maximum separation is 550 million miles.
		&lt;br&gt;&lt;br&gt;
		Binary systems allow astronomers to estimate the mass of companion objects. The
		brown dwarfs are 61 and 50 times the mass of Jupiter. They are therefore too
		small to burn as stars, but too large to have formed as planets. Based on the
		total estimated mass of the system, astronomers suspect there is a third
		brown dwarf member that has not yet been resolved.
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm.php?date=0109&quot;&gt;read more&lt;/a&gt;
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM0109/potm0109.jpg&quot;&gt;&lt;img
      src=&quot;http://www.mpia.de/PSF/potm/POTM0109/potm0109_s.jpg&quot; style=&quot;float:left; padding-right:10px; padding-bottom:10px; width:371px; height:278px;&quot;/&gt;&lt;/a&gt;
	  </description>
      <enclosure url="http://www.mpia.de/PSF/potm/POTM0109/potm0109.jpg" length="95716" type="image/jpg"/>
    </item>

    <item>
      <title>Simulation of the diversity of extrasolar planets</title>
      <link>http://www.mpia.de/PSF/potm.php?date=1208</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=1208</guid>
      <pubDate>Mon, 01 Dec 2008 08:55:00 +0100</pubDate>
      <description>
      According to our current understanding form planets in circumstellar disks of dust and gas, where dust particles first accumulate to form kilometer sized planetesimals, and then continue to grow first to protoplanets and finally to planets with some mass and distance from the parent star.
      &lt;br&gt;
	  These model calculations show which planetary masses are expected at which distances from a solar like star. The numerical formation model contains our current knowledge about dust and gas disks around young stars as well as present-day theories about various planet formation processes.
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm.php?date=1208&quot;&gt;read more&lt;/a&gt;
      &lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM1208/potm1208.pdf&quot;&gt;&lt;img
      src=&quot;http://www.mpia.de/PSF/potm/POTM1208/potm1208_s.jpg&quot; style=&quot;float:left; padding-right:10px; padding-bottom:10px; width:371px; height:278px;&quot;/&gt;&lt;/a&gt;
	  </description>
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    </item>
    
    <item>
      <title>Plasma beta in saturated MRI turbulence</title>
      <link>http://www.mpia.de/PSF/potm.php?date=1108</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=1108</guid>
      <pubDate>Tue, 04 Nov 2008 20:55:00 -0800</pubDate>
      <description>
	  This contour plot presents the logarithmic plasma beta distribution in
	  the saturated MRI turbulence regime. The plasma beta describes the ratio
	  between the gas pressure over the magnetic pressure.&lt;br&gt;
	  There are low plasma beta regions (dark) with strong
	  magnetic fields in the outer part of the disk and a dominating MRI
	  turbulent core with weak magnetic fields (bigger plasma beta).&lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM1108/potm1108.pdf&quot;&gt;&lt;img
      src=&quot;http://www.mpia.de/PSF/potm/POTM1108/potm1108.jpg&quot; style=&quot;float:left; padding-right:10px; padding-bottom:10px; width:371px; height:278px;&quot;/&gt;&lt;/a&gt;
	  </description>
      <enclosure url="http://www.mpia.de/PSF/potm/POTM1108/potm1108.pdf" length="95716" type="image/pdf"/>
    </item>
    
    <item>
      <title>PSF Group Picture</title>
      <link>http://www.mpia.de/PSF/potm.php?date=1008</link>
      <guid>http://www.mpia.de/PSF/potm.php?date=1008</guid>
      <pubDate>Tue, 04 Nov 2008 17:20:07 -0800</pubDate>
      <description>
      Group picture from PSF Workshop 2008 at the monastery of Maulbronn&lt;br&gt;
      &lt;a href=&quot;http://www.mpia.de/PSF/potm/POTM1008/potm1008.jpg&quot;&gt;&lt;img
      src=&quot;http://www.mpia.de/PSF/potm/POTM1008/potm1008_s.jpg&quot; style=&quot;float:left; padding-right:10px; padding-bottom:10px; width:371px; height:278px;&quot;/&gt;&lt;/a&gt;
	  </description>
      <enclosure url="http://www.mpia.de/PSF/potm/POTM1008/potm1008.jpg" length="95716" type="image/pdf"/>
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