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            <SubmissionComments>Switched from F606W to F350LP and revised the discussion on observing details.</SubmissionComments>
            
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            <SubmissionLog>Assigned ID: 1047

----- Attempting Submission 1 (Sun Feb 24 14:12:55 GMT 2013) -----
  HST Phase I Proposal 1047 (HST_MBC_TOO_2013_v4_submitted.pdf.apt) successfully submitted.

----- Attempting Submission 2 (Sun Feb 24 23:53:57 GMT 2013) -----</SubmissionLog>
            
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            <SubmissionComments>Please schedule V2 as soon as possible, consistent
with being a "non-disruptive" ToO. After analysis of
the V1 data, we see that another set of observations at
the earliest feasible date is scientifically desired.

I updated the target's orbital elements to JPL2. 
Also, since V1 has already executed using the JPL1 elements,
I created a new target for V2. It's the same target, but with
improved orbital elements.</SubmissionComments>
            
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            <SubmissionLog>----- Attempting Submission 1 (Sat Jun 15 14:20:53 GMT 2013) -----

----- Attempting Submission 2 (Wed Aug 28 12:49:06 GMT 2013) -----

----- Attempting Submission 3 (Wed Aug 28 17:32:44 GMT 2013) -----
  HST Phase II Proposal 13475 (13475.apt) successfully submitted.

----- Attempting Submission 4 (Wed Aug 28 18:10:05 GMT 2013) -----

----- Attempting Submission 5 (Wed Aug 28 20:39:24 GMT 2013) -----

----- Attempting Submission 6 (Fri Aug 30 12:29:59 GMT 2013) -----

----- Attempting Submission 7 (Wed Sep 11 17:09:31 GMT 2013) -----</SubmissionLog>
            
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      <Title>Hubble Imaging of a Newly Discovered Main Belt Comet</Title>
      
      <Abstract>Main-belt comets (MBCs, or ``active asteroids'') have the orbital
characteristics of asteroids but also show transient, comet-like activity.
Examples of mass-loss likely caused by ice sublimation and by impact
have been established, while numerous additional processes are
capable of launching material from asteroids.  We propose two-orbits of
non-disruptive, target-of-opportunity observations of the next MBC 
discovered in order to help determine the process driving mass-loss.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="David"
         LastName="Jewitt"
         ESAMember="false"
         UniqueID="4421"
         Institution="University of California - Los Angeles"
         Country="USA"
         State="CA"
         Contact="true" />
      
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         FirstName="Harold"
         MiddleInitial="A."
         LastName="Weaver"
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         Institution="The Johns Hopkins University Applied Physics Laboratory"
         Country="USA"
         State="MD"
         Contact="true"
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         FirstName="Jessica"
         LastName="Agarwal"
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         UniqueID="9402"
         Institution="Max Planck Institute for Solar System Research"
         Country="DEU"
         Contact="false"
         AdminUSPI="false" />
      
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         FirstName="Stephen"
         MiddleInitial="M."
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         UniqueID="1202"
         Institution="University of Arizona"
         Country="USA"
         State="AZ"
         Contact="false"
         AdminUSPI="false" />
      
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         FirstName="Max"
         LastName="Mutchler"
         ESAMember="false"
         UniqueID="3468"
         Institution="Space Telescope Science Institute"
         Country="USA"
         State="MD"
         Contact="true"
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            <ObservingDescription>This proposal is a straightforward continuation of our (so-far un-triggered) ToO approved in Cycle 20. We request two single-orbit HST visits to image a newly-discovered MBC. The basic objective is to characterize the early-time morphology and establish the initial rates of change in the appearance, so that the need for additional HST observations and their optimum cadence can be realistically determined. In some cases (as with P/2010 A2, for instance), the initial observations alone will be enough to determine whether the morphology is more consistent with sublimation or another origin. In others, careful study of the photometry and evolution over long intervals will be needed for this purpose. Our observing strategy is to take both short and long exposures using WFC3 and a single filter (F606W). Asteroid Scheila, with its ultra-bright nucleus V~13.7, represents an end-member case. We used an exposure time of 0.5 sec (the shortest available) to obtain S/N~200 on the nucleus itself in search of structure at ~100 km scales. An intermediate exposure time of ~40 s brought out the near-nucleus environment without saturating too many pixels, while long exposures of ~400 s provided the deepest search for debris. We plan to take a sequence of at least 3 images (one for each exposure time) at one location on the CCD and then repeat that sequence of images at a dithered location (offset by 0.2'' in each dimension). Dithered, multiple images provide protection from bad pixels and cosmic ray strikes that otherwise might compromise the photometry. Previous HST observations show that the timescale for substantial change ranges from several weeks (Scheila) to several months (P/2010 A2). 

Therefore, while the first observation should be scheduled as soon as possible after discovery of activity, the science does not require that the first visit be secured within the first two weeks. So ours is a non-disruptive Target of Opportunity program, which will not require heroic scheduling. The first visit will set the scene, by establishing the high-resolution morphology of the object (at ~60 km/pixel at 2 AU geocentric distance). The second visit, ideally separated from the first by ~14 days, will reveal the changes. The two visits together will allow us to make a rational decision about the need for further observations with HST. Main-belt targets have apparent rates of motion typically ~50''/hr, which are easily within Hubble's tracking capabilities. This rate of motion is also slow enough to keep a single pair of guide stars within the FGS pickles for an entire visibility window. The ephemeris uncertainty of numbered asteroids is negligible (sub-arcsecond), compared to the WFC3 field-of-view of 162x162''. For newly discovered objects the uncertainty can be larger but, as we showed even for the low surface brightness and morphologically complex example set by P/2010 A2, attaining 1" to 2" accuracy is straightforward. Ephemeris issues are of no concern to this observation. We understand that we will have essentially no control over the spacecraft roll angle, which means we will not be able to optimize the orientation of the dust tail on the CCD (i.e., to orient the tail along the longest dimension of the detector). However, the field-of-view of the camera is large enough that we should obtain excellent data on a portion of the tail, no matter what spacecraft roll angle is used.</ObservingDescription>
            
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         <Comments>Updated to JPL #2 orbital elements</Comments>
         
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