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            <SubmissionLog>----- Submission 1 (Fri May 13 01:56:13 GMT 2005) -----
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      <Title>Caught in the Act with HST -- Active Jet Sculpting in the Young Preplanetary Nebulae IRAS 22036+5306</Title>
      
      <Abstract>We have discovered an extended, highly-structured and bipolar nebula surrounding the post-AGB object IRAS22036+5306 (I22036), in a Cycle 10 WFPC2 imaging survey of very young pre-planetary nebulae (PPNs). Young PPNs like I22036, objects in rapid transition
between the AGB and Planetary Nebulae (PN) phases, retain direct signatures, in the spatial character of their outflows, of the physical mechanisms which transform slowly expanding, round circumstellar AGB envelopes into highly aspherical PNs with fast-expanding
elongated lobes along one or more axes. I22036 shows intriguing evidence for the presence of jets in the HST images, and VLA A-array maps show OH maser emission in a linear structure along the nebular axis. Our ground-based echelle H-alpha spectra show
high-velocity blue-shifted absorption in a very broad (~2000 km/s) line profile, and mm-wave CO J=1-0 interferometric data show a bipolar molecular outflow.

There are very few young PPNs like I22036 which show clear morphological &amp; kinematical evidence of the presence of jets and their working surfaces, making it unquestionably a key object for understanding how jets can sculpt out bipolar lobes in a progenitor AGB
star wind. Using ground-based long-slit spectroscopy with the Keck/ESI, we have partially spatially resolved the H-alpha emission in this object. We now propose to image I22036 in F658N, F631N, F606W and F814W in order to identify accurately the location and
structure of the shocked gas, and its relation to the jets and their working surfaces. An important goal is to determine whether we can characterise the forward and reverse shocks near the heads of the knotty jets. The proposed HST imaging will help us to
understand the spatio-kinematic structure of the outflowing gas in the bipolar lobes, and allow us to study the relationships between the important dynamical components of this nebula. Supporting ground-based observations such as Zeeman measurements of polarised
OH masers with the VLBA to search for magnetic fields in I22036 are being pursued for testing magnetic-collimation models for jets in PPNs.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Raghvendra"
         LastName="Sahai"
         ESAMember="false">
         
         <Address
            Institution="Jet Propulsion Laboratory"
            USState="CA"
            Country="USA" />
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      <CoInvestigator
         Honorific="Dr."
         FirstName="Mark"
         LastName="Morris"
         ESAMember="false"
         AdminUSPI="false"
         Contact="false">
         
         <Address
            Institution="University of California - Los Angeles"
            USState="CA"
            Country="USA" />
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      <CoInvestigator
         Honorific="Dr."
         FirstName="Carmen"
         LastName="Sanchez Contreras"
         ESAMember="false"
         AdminUSPI="false"
         Contact="false">
         
         <Address
            Institution="California Institute of Technology"
            USState="CA"
            Country="USA" />
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      <CoInvestigator
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         FirstName="Mark"
         LastName="Claussen"
         ESAMember="false"
         AdminUSPI="false"
         Contact="false">
         
         <Address
            Institution="Associated Universities, Inc."
            USState="VA"
            Country="USA" />
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            <ObservingDescription>We will obtain deep 4-point dithered observations with the HRC on ACS through the broad-band
F606W \&amp; F814W, and the narrow-band F658N filter. Our goal is to make a significant
improvement in sensitivity over the previous SNAPshot imaging observations, where we used
relatively short exposure times (typically 8-10 minutes).
So we will now use total integration times of about $\sim$2400 sec (1 orbit) each for F606W 
\&amp; F814W, which will provide a significant improvement over the previous data. We will use
F606W images to subtract the continuum from the emission line filter images.

The longest exposure time (about 5000 sec) will be used for the F658N imaging, which will
contain both scattered (continuum+H$\alpha$) photons, and local H$\alpha$ emission. This
will provide a signal-to-noise ratio (S/N)$&gt;$60 in the H$\alpha$ line wings (at
$\pm$1000\kms) towards the nebular center and S/N$&gt;$20 towards the lobes. These S/N ratios
have been estimated from the intensity of the H$\alpha$ line in one pixel (0.3$''$) of our
ESI long-slit spectrum (slit width=0.5$''$, Figure 2) towards the nebular center and
towards the lobes and assuming that the H$\alpha$ brightness distribution is roughly
uniform within a region with size $&lt;$0.3$''$x0.3$''$. We would like to be able to separate
the scattered H$\alpha$ emission from the local emission, either through appropriate
differencing or ratioing. We recognize that this may not provide a precise quantitative
measurement of the H$\alpha$ intensity because of imperfect removal of the scattered light
due to variable circumstellar extinction, but that does not affect the main goal of the
proposal, namely to delineate the regions of active shocks in these nebulae.

We will also image the OI 6300A emission, which is most likely to be only local emission and
not scattered, with WFPC2 through the F631N filter. The exposure time with such a filter
will be about 2400\,s with the wide field (WFC) camera mode, which will provide S/N in the
line wings (up to $\pm$500\kms) of S/N$&gt;$20 towards the center and S/N$&gt;$7 in the lobes.
This S/N has been estimated by taking into account that the OI line is a factor of
$\sim$4-5 weaker than H$\alpha$ (from our Keck+ESI spectrum).</ObservingDescription>
            
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