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----- Attempting Submission 1 (Mon Apr 06 18:32:20 GMT 2020) -----</SubmissionLog>
            
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----- Attempting Submission 2 (Thu Apr 09 13:41:39 GMT 2020) -----</SubmissionLog>
            
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      <Title>Breakup of Long-Period Comet C/2019 Y4 (ATLAS)</Title>
      
      <Abstract>We seek HST time with the WFC3 camera in order to study the on-going break-up of long-period comet C/2019 Y4 (ATLAS).  Break-up of comets may be the dominant destruction process of these bodies, yet is poorly studied because breakups occur unpredictably and evolve rapidly, require timely observations which are difficult to secure.  We propose a 4 orbit allocation to measure the temporal evolution of the fragments, in order to measure the brightness and velocity distributions and to measure fragment nn-gravitational acceleration caused by outgassing forces (the latter are a measure of fragment size).  We will also seek evidence for rotational and other modulation of the primary nucleus and fragments, indicative of patchy distribution of surface volatiles.  A Monte-Carlo dust model will be applied to imaged of the diffuse envelope.  C/2019 Y4 has the potential to be one of only a handful of disrupting comets ever studied at HST resolution, and to set exciting constraints on models of the breakup mechanism.</Abstract>
      
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         Institution="The Johns Hopkins University Applied Physics Laboratory"
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         Institution="University of California - Los Angeles"
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            <ObservingDescription>We request observations of comet ATLAS with HST and WFC3, using the F350LP broadband filter. We request 2 to 3 day spacing between visits in order to connect fragments and their motion between orbits, thereby to measure the velocities and accelerations. In each orbit, we will obtain six 260s integrations on the comet, dithered to provide protection from chip defects. The six images, when combined, will also provide adequate protection from cosmic rays. The WFC3 Exposure Time Calculator indicates that, for a point source, solar-type spectrum, a signal-to-noise ratio of 6 is reached in 230 s at V = 26 in the F350LP filter (optimal extraction yields SNR=13). For example, at opposition and heliocentric distance R = 1 AU, magnitude V = 26 corresponds to an object radius 25 m (geometric albedo 0.04 assumed). These are upper limits to the point source thresholds because at least some of the fragments are embedded in their own dust comae. However, it is clear that HST offers unprecedented sensitivity to faint fragments. We use F350LP because the F350LP count rate is 1.6 higher for a target with a solar-type spectrum than other commonly used broadband filters (e.g., F606W), providing a better count rate and signal-to-noise ratio. We also plan to dither the exposures to mitigate the effects from bad pixels, cosmic rays, and the inter-chip gap. Angular non-sidereal rates peak at about 10000 hour1 and are well within the range of HST capabilities. The ephemeris uncertainty is 3 sigma &lt; 1 arcsec, of no concern given the field of view of WFC3. We request Disruptive Scheduling for these observations. This is necessary because of the expected rapid photometric and morphological development of the fragments as seen in other disintegrating comets. Comet ATLAS will be in the HSTs 55 Sun exclusion zone from UT 2020 April 30 to UT 2020 September 7. Therefore, we must observe with HST before 2020 April 30, but earlier dates are preferred. The apparent rates of motion relative to sidereal are &lt; 1 arcsec/hour, which are easily within Hubble's tracking capabilities. These rates of motion are also slow enough to keep a single pair of guide stars within the FGS pickles for an entire visibility window. The ephemeris uncertainties are typically at the 1 arcsec level. We understand that we will have essentially no control over the spacecraft roll angle.</ObservingDescription>
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