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   <!--Date: Fri Feb 23 18:04:05 GMT 2018-->
   
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            <ErrorText>LONG SU LIKELY TO INTERSECT THE SAA</ErrorText>
            
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            <SubmissionLog>----- Attempting Submission 3 (Fri Feb 23 18:04:05 GMT 2018) -----</SubmissionLog>
            
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   <ProposalInformation
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      SnapPriority="Normal Priority"
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      Cycle="25"
      STScIEditNumber="7">
      
      <Title>The KELT-11b Opportunity: Measuring the Atmospheric Water Abundance for a Sub-Saturn-Mass Planet around a Metal-Rich Star</Title>
      
      <Abstract>Measurements of exoplanet atmosphere composition provide an unparalleled window into planetary nature and origins.  Water in particular is an important tracer of the planet formation process because it is a dominant component by mass of icy planetesimals.  Exoplanets provide the opportunity to measure water abundance over a wide range of planet masses and thereby test predictions of planet population synthesis models.  So far, however, precise constraints on water abundance have been limited to Jupiter-mass objects. 

Here we propose to measure the transmission spectrum of the recently discovered low density sub-Saturn KELT-11b with HST/WFC3. We will use this measurement to determine the planet's atmospheric water abundance.  KELT-11b is one of the few Saturn-mass planets for which we can obtain constraints on the water abundance with a modest amount of telescope time. Our results will enable meaningful comparison with both objects in the Solar System and with the other few planets in the sub-Saturn population. This program will also be the first investigation of the metal enhancement of a planet with a metal-rich host star. Even if the atmosphere is cloudy, our data will be sufficiently precise to detect water above a 1 mbar cloud-deck,  and will constrain cloud physics in a new regime of surface gravity.  These measurements will set the stage for comparative planetology that will be possible with JWST.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Knicole"
         LastName="Colon"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="16793"
         Institution="NASA Goddard Space Flight Center"
         Country="USA"
         State="MD"
         Contact="true" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Laura"
         LastName="Kreidberg"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="13453"
         Institution="Harvard University"
         Country="USA"
         State="MA"
         Contact="true"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Daniel"
         LastName="Angerhausen"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="13421"
         Institution="University of Bern"
         Country="CHE"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Thomas"
         MiddleInitial="G."
         LastName="Beatty"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="13647"
         Institution="The Pennsylvania State University"
         Country="USA"
         State="PA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Diana"
         LastName="Dragomir"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="12912"
         Institution="Massachusetts Institute of Technology"
         Country="USA"
         State="MA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Prof."
         FirstName="Jonathan"
         LastName="Fortney"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="8485"
         Institution="University of California - Santa Cruz"
         Country="USA"
         State="CA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Prof."
         FirstName="John"
         MiddleInitial="Asher"
         LastName="Johnson"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="13138"
         Institution="Harvard University"
         Country="USA"
         State="MA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Michael"
         LastName="Line"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="13777"
         Institution="Arizona State University"
         Country="USA"
         State="AZ"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Eric"
         MiddleInitial="David"
         LastName="Lopez"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="16790"
         Institution="NASA Goddard Space Flight Center"
         Country="USA"
         State="MD"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Nikku"
         LastName="Madhusudhan"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="8999"
         Institution="University of Cambridge"
         Country="GBR"
         State="England"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Avi"
         LastName="Mandell"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="9000"
         Institution="NASA Goddard Space Flight Center"
         Country="USA"
         State="MD"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         FirstName="Brett"
         MiddleInitial="M."
         LastName="Morris"
         ESAMember="false"
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         Retired="false"
         UniqueID="14212"
         Institution="University of Washington"
         Country="USA"
         State="WA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         FirstName="Joshua"
         LastName="Pepper"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="16800"
         Institution="Lehigh University"
         Country="USA"
         State="PA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Joseph"
         MiddleInitial="E."
         LastName="Rodriguez"
         Suffix="Jr."
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="12656"
         Institution="Harvard University"
         Country="USA"
         State="MA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Prof."
         FirstName="Keivan"
         MiddleInitial="G."
         LastName="Stassun"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="6007"
         Institution="Vanderbilt University"
         Country="USA"
         State="TN"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Kevin"
         MiddleInitial="B."
         LastName="Stevenson"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="12419"
         Institution="Space Telescope Science Institute"
         Country="USA"
         State="MD"
         Contact="false"
         AdminUSPI="false" />
      
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            <ObservingDescription>We will obtain time series spectroscopy of the KELT-11b planetary system with the WFC3 instrument during one transit of the planet. We will use the G141 grism and the 512x512 subarray. The observation will consist of 9 sequential HST orbits to obtain quasi-continuous coverage of the planet's transit. Nine orbits are required to observe the transit and measure the out-of-transit baseline flux level. In addition, based on a recent paper by Zhou et al. (2017) which includes a new systematics model of WFC3 data, it is no longer necessary to discard the first orbit in a visit in order to decrease instrument systematics in the data. The observation duration is longer than usual for exoplanet transit spectroscopy because the transit duration is over 7.0 hours thanks to the slightly evolved host star.

We will obtain a direct image of the target star with the F130N filter at the beginning of each orbit for wavelength calibration. The remainder of each orbit will consist of 46.696 s exposures with the NSAMP = 3, SPARS25 readout pattern. To keep the fluence below saturation, we will use spatial scan mode with a 0.96 arcsec/sec scan rate (yielding a total scan height of 345 pixels). Using past WFC3 observations of similar targets as a benchmark, we estimate the maximum expected per pixel counts to be below 40k electrons. To maximize the duty cycle of the observations, we will alternate between forward and reverse scanning along the detector. This is the same observational strategy we used extensively for transit/eclipse observations in our programs in Cycles 20, 21, 22, and 23 which yielded photon-noise limited light curves.

The proposed observations are time-critical and must be centered on the transit of the planet. Transits occur often (every 4.7 days), so there are many opportunities to observe the planet. The observations must also be scheduled to avoid crossing the South Atlantic Anomaly. 

The observations will not need to be coordinated with other observatories. When the HST observations are scheduled, we will arrange for simultaneous ground-based optical and IR photometry in order to trace the intrinsic variability of the system. These observations will be performed with small-to-mid-sized telescopes which are easily accessible to the world-wide KELT network of collaborators of the proposers.</ObservingDescription>
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         <ProprietaryPeriod
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         <Treasury>false</Treasury>
         
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         <NoDuplicateProposalSubmissions>false</NoDuplicateProposalSubmissions>
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         <Availability>SUPPORTED</Availability>
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            <Description>EXTRA-SOLAR PLANETARY SYSTEM</Description>
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                        RollRanges="29 Oct 2017&#x9;&#x9;&#x9;274.85 - 284.85&#xA;30 Oct 2017&#x9;&#x9;&#x9;275.30 - 285.30&#xA;31 Oct 2017&#x9;&#x9;&#x9;275.73 - 285.73&#xA;01 Nov 2017&#x9;&#x9;&#x9;276.16 - 286.16&#xA;02 Nov 2017&#x9;&#x9;&#x9;276.57 - 286.57&#xA;03 Nov 2017&#x9;&#x9;&#x9;276.97 - 286.97&#xA;04 Nov 2017&#x9;&#x9;&#x9;277.37 - 287.37&#xA;05 Nov 2017&#x9;&#x9;&#x9;277.76 - 287.76&#xA;06 Nov 2017&#x9;&#x9;&#x9;278.14 - 288.14&#xA;07 Nov 2017&#x9;&#x9;&#x9;278.51 - 288.51&#xA;08 Nov 2017&#x9;&#x9;&#x9;278.88 - 288.88&#xA;09 Nov 2017&#x9;&#x9;&#x9;279.23 - 289.23&#xA;10 Nov 2017&#x9;&#x9;&#x9;279.59 - 289.59&#xA;11 Nov 2017&#x9;&#x9;&#x9;279.93 - 289.93&#xA;12 Nov 2017&#x9;&#x9;&#x9;280.27 - 290.27&#xA;13 Nov 2017&#x9;&#x9;&#x9;280.61 - 290.61&#xA;14 Nov 2017&#x9;&#x9;&#x9;280.94 - 290.94&#xA;15 Nov 2017&#x9;&#x9;&#x9;281.27 - 291.27&#xA;16 Nov 2017&#x9;&#x9;&#x9;281.59 - 291.59&#xA;17 Nov 2017&#x9;&#x9;&#x9;281.90 - 291.90&#xA;18 Nov 2017&#x9;&#x9;&#x9;282.22 - 292.22&#xA;19 Nov 2017&#x9;&#x9;&#x9;282.53 - 292.53&#xA;20 Nov 2017&#x9;&#x9;&#x9;282.83 - 292.83&#xA;21 Nov 2017&#x9;&#x9;&#x9;283.14 - 293.14&#xA;22 Nov 2017&#x9;&#x9;&#x9;283.44 - 293.44&#xA;23 Nov 2017&#x9;&#x9;&#x9;283.73 - 293.73&#xA;24 Nov 2017&#x9;&#x9;&#x9;284.03 - 294.03&#xA;25 Nov 2017&#x9;&#x9;&#x9;284.32 - 294.32&#xA;26 Nov 2017&#x9;&#x9;&#x9;284.61 - 294.61&#xA;27 Nov 2017&#x9;&#x9;&#x9;284.90 - 294.90&#xA;28 Nov 2017&#x9;&#x9;&#x9;285.19 - 295.19&#xA;29 Nov 2017&#x9;&#x9;&#x9;285.47 - 295.47&#xA;30 Nov 2017&#x9;&#x9;&#x9;285.75 - 295.75&#xA;01 Dec 2017&#x9;&#x9;&#x9;286.04 - 296.04&#xA;02 Dec 2017&#x9;&#x9;&#x9;286.32 - 296.32&#xA;03 Dec 2017&#x9;&#x9;&#x9;286.60 - 296.60&#xA;04 Dec 2017&#x9;&#x9;&#x9;286.87 - 296.87&#xA;05 Dec 2017&#x9;&#x9;&#x9;287.15 - 297.15&#xA;06 Dec 2017&#x9;&#x9;&#x9;287.43 - 297.43&#xA;07 Dec 2017&#x9;&#x9;&#x9;287.71 - 297.71&#xA;08 Dec 2017&#x9;&#x9;&#x9;287.99 - 297.99&#xA;09 Dec 2017&#x9;&#x9;&#x9;270.86 - 315.66&#xA;10 Dec 2017&#x9;&#x9;&#x9;271.04 - 316.04&#xA;11 Dec 2017&#x9;&#x9;&#x9;271.32 - 316.32&#xA;12 Dec 2017&#x9;&#x9;&#x9;271.60 - 316.60&#xA;13 Dec 2017&#x9;&#x9;&#x9;271.88 - 316.88&#xA;14 Dec 2017&#x9;&#x9;&#x9;272.16 - 317.16&#xA;15 Dec 2017&#x9;&#x9;&#x9;272.34 - 317.54&#xA;16 Dec 2017&#x9;&#x9;&#x9;272.62 - 317.82&#xA;17 Dec 2017&#x9;&#x9;&#x9;272.81 - 318.19&#xA;18 Dec 2017&#x9;&#x9;&#x9;273.09 - 318.49&#xA;19 Dec 2017&#x9;&#x9;&#x9;273.27 - 318.87&#xA;20 Dec 2017&#x9;&#x9;&#x9;273.46 - 319.26&#xA;21 Dec 2017&#x9;&#x9;&#x9;273.65 - 319.65&#xA;22 Dec 2017&#x9;&#x9;&#x9;273.94 - 319.94&#xA;23 Dec 2017&#x9;&#x9;&#x9;274.14 - 320.34&#xA;24 Dec 2017&#x9;&#x9;&#x9;274.23 - 320.83&#xA;25 Dec 2017&#x9;&#x9;&#x9;274.43 - 321.23&#xA;26 Dec 2017&#x9;&#x9;&#x9;274.64 - 321.64&#xA;27 Dec 2017&#x9;&#x9;&#x9;274.84 - 322.04&#xA;28 Dec 2017&#x9;&#x9;&#x9;274.95 - 322.55&#xA;29 Dec 2017&#x9;&#x9;&#x9;275.16 - 322.96&#xA;30 Dec 2017&#x9;&#x9;&#x9;275.28 - 323.48&#xA;31 Dec 2017&#x9;&#x9;&#x9;275.50 - 323.90&#xA;01 Jan 2018&#x9;&#x9;&#x9;275.83 - 324.23&#xA;02 Jan 2018&#x9;&#x9;&#x9;275.96 - 324.76&#xA;03 Jan 2018&#x9;&#x9;&#x9;276.09 - 325.29&#xA;04 Jan 2018&#x9;&#x9;&#x9;276.27 - 325.79&#xA;05 Jan 2018&#x9;&#x9;&#x9;276.62 - 326.14&#xA;06 Jan 2018&#x9;&#x9;&#x9;278.10 - 325.36&#xA;07 Jan 2018&#x9;&#x9;&#x9;278.46 - 325.72&#xA;08 Jan 2018&#x9;&#x9;&#x9;278.83 - 326.09&#xA;09 Jan 2018&#x9;&#x9;&#x9;280.18 - 325.48&#xA;10 Jan 2018&#x9;&#x9;&#x9;280.56 - 325.86&#xA;11 Jan 2018&#x9;&#x9;&#x9;280.95 - 326.25&#xA;12 Jan 2018&#x9;&#x9;&#x9;282.25 - 325.75&#xA;13 Jan 2018&#x9;&#x9;&#x9;282.65 - 326.15&#xA;14 Jan 2018&#x9;&#x9;&#x9;283.07 - 326.57&#xA;15 Jan 2018&#x9;&#x9;&#x9;284.27 - 326.21&#xA;16 Jan 2018&#x9;&#x9;&#x9;284.71 - 326.65&#xA;17 Jan 2018&#x9;&#x9;&#x9;285.16 - 327.10&#xA;18 Jan 2018&#x9;&#x9;&#x9;286.32 - 326.86&#xA;19 Jan 2018&#x9;&#x9;&#x9;286.79 - 327.33&#xA;20 Jan 2018&#x9;&#x9;&#x9;287.27 - 327.81&#xA;21 Jan 2018&#x9;&#x9;&#x9;288.40 - 327.68&#xA;22 Jan 2018&#x9;&#x9;&#x9;288.92 - 328.20&#xA;23 Jan 2018&#x9;&#x9;&#x9;289.45 - 328.73&#xA;24 Jan 2018&#x9;&#x9;&#x9;289.75 - 329.51&#xA;25 Jan 2018&#x9;&#x9;&#x9;290.32 - 330.08&#xA;26 Jan 2018&#x9;&#x9;&#x9;290.90 - 330.66&#xA;27 Jan 2018&#x9;&#x9;&#x9;291.51 - 331.27&#xA;28 Jan 2018&#x9;&#x9;&#x9;291.95 - 332.09&#xA;29 Jan 2018&#x9;&#x9;&#x9;292.60 - 332.74&#xA;30 Jan 2018&#x9;&#x9;&#x9;293.27 - 333.41&#xA;31 Jan 2018&#x9;&#x9;&#x9;293.39 - 334.71&#xA;01 Feb 2018&#x9;&#x9;&#x9;294.12 - 335.44&#xA;02 Feb 2018&#x9;&#x9;&#x9;294.88 - 336.20&#xA;03 Feb 2018&#x9;&#x9;&#x9;294.77 - 337.89&#xA;04 Feb 2018&#x9;&#x9;&#x9;295.60 - 338.72&#xA;05 Feb 2018&#x9;&#x9;&#x9;296.47 - 339.59&#xA;06 Feb 2018&#x9;&#x9;&#x9;297.38 - 340.50&#xA;07 Feb 2018&#x9;&#x9;&#x9;297.12 - 342.66&#xA;08 Feb 2018&#x9;&#x9;&#x9;298.11 - 343.65&#xA;09 Feb 2018&#x9;&#x9;&#x9;299.16 - 344.70&#xA;10 Feb 2018&#x9;&#x9;&#x9;298.58 - 347.48&#xA;11 Feb 2018&#x9;&#x9;&#x9;299.74 - 348.64&#xA;12 Feb 2018&#x9;&#x9;&#x9;300.96 - 349.86&#xA;13 Feb 2018&#x9;&#x9;&#x9;302.25 - 351.15&#xA;14 Feb 2018&#x9;&#x9;&#x9;301.24 - 354.90&#xA;15 Feb 2018&#x9;&#x9;&#x9;302.68 - 356.34&#xA;16 Feb 2018&#x9;&#x9;&#x9;304.20 - 357.86&#xA;17 Feb 2018&#x9;&#x9;&#x9;305.81 - 359.47&#xA;18 Feb 2018&#x9;&#x9;&#x9;304.35 - 004.35&#xA;19 Feb 2018&#x9;&#x9;&#x9;306.17 - 006.17&#xA;20 Feb 2018&#x9;&#x9;&#x9;308.09 - 008.09&#xA;21 Feb 2018&#x9;&#x9;&#x9;310.14 - 010.14&#xA;22 Feb 2018&#x9;&#x9;&#x9;312.30 - 012.30&#xA;23 Feb 2018&#x9;&#x9;&#x9;314.60 - 014.60&#xA;24 Feb 2018&#x9;&#x9;&#x9;317.03 - 017.03&#xA;25 Feb 2018&#x9;&#x9;&#x9;319.61 - 019.61&#xA;26 Feb 2018&#x9;&#x9;&#x9;322.32 - 022.32&#xA;27 Feb 2018&#x9;&#x9;&#x9;325.18 - 025.18&#xA;28 Feb 2018&#x9;&#x9;&#x9;328.19 - 028.19&#xA;01 Mar 2018&#x9;&#x9;&#x9;331.33 - 031.33&#xA;02 Mar 2018&#x9;&#x9;&#x9;334.60 - 034.60&#xA;03 Mar 2018&#x9;&#x9;&#x9;337.99 - 037.99&#xA;04 Mar 2018&#x9;&#x9;&#x9;341.48 - 041.48&#xA;05 Mar 2018&#x9;&#x9;&#x9;345.05 - 045.05&#xA;06 Mar 2018&#x9;&#x9;&#x9;348.67 - 048.67&#xA;07 Mar 2018&#x9;&#x9;&#x9;352.33 - 052.33&#xA;08 Mar 2018&#x9;&#x9;&#x9;355.99 - 055.99&#xA;09 Mar 2018&#x9;&#x9;&#x9;359.63 - 059.63&#xA;10 Mar 2018&#x9;&#x9;&#x9;003.22 - 063.22&#xA;11 Mar 2018&#x9;&#x9;&#x9;006.74 - 066.74&#xA;12 Mar 2018&#x9;&#x9;&#x9;010.16 - 070.16&#xA;13 Mar 2018&#x9;&#x9;&#x9;013.46 - 073.46&#xA;14 Mar 2018&#x9;&#x9;&#x9;016.64 - 076.64&#xA;15 Mar 2018&#x9;&#x9;&#x9;019.69 - 079.69&#xA;16 Mar 2018&#x9;&#x9;&#x9;022.59 - 082.59&#xA;17 Mar 2018&#x9;&#x9;&#x9;025.35 - 085.35&#xA;18 Mar 2018&#x9;&#x9;&#x9;027.96 - 087.96&#xA;19 Mar 2018&#x9;&#x9;&#x9;030.43 - 090.43&#xA;20 Mar 2018&#x9;&#x9;&#x9;032.77 - 092.77&#xA;21 Mar 2018&#x9;&#x9;&#x9;034.97 - 094.97&#xA;22 Mar 2018&#x9;&#x9;&#x9;037.05 - 097.05&#xA;23 Mar 2018&#x9;&#x9;&#x9;039.01 - 099.01&#xA;24 Mar 2018&#x9;&#x9;&#x9;040.85 - 100.85&#xA;25 Mar 2018&#x9;&#x9;&#x9;042.59 - 102.59&#xA;26 Mar 2018&#x9;&#x9;&#x9;047.40 - 101.06&#xA;27 Mar 2018&#x9;&#x9;&#x9;048.95 - 102.61&#xA;28 Mar 2018&#x9;&#x9;&#x9;050.41 - 104.07&#xA;29 Mar 2018&#x9;&#x9;&#x9;051.79 - 105.45&#xA;30 Mar 2018&#x9;&#x9;&#x9;055.48 - 104.38&#xA;31 Mar 2018&#x9;&#x9;&#x9;056.72 - 105.62&#xA;01 Apr 2018&#x9;&#x9;&#x9;057.90 - 106.80&#xA;02 Apr 2018&#x9;&#x9;&#x9;059.01 - 107.91&#xA;03 Apr 2018&#x9;&#x9;&#x9;061.75 - 107.29&#xA;04 Apr 2018&#x9;&#x9;&#x9;062.76 - 108.30&#xA;05 Apr 2018&#x9;&#x9;&#x9;063.73 - 109.27&#xA;06 Apr 2018&#x9;&#x9;&#x9;065.85 - 108.97&#xA;07 Apr 2018&#x9;&#x9;&#x9;066.73 - 109.85&#xA;08 Apr 2018&#x9;&#x9;&#x9;067.57 - 110.69&#xA;09 Apr 2018&#x9;&#x9;&#x9;068.37 - 111.49&#xA;10 Apr 2018&#x9;&#x9;&#x9;070.04 - 111.36&#xA;11 Apr 2018&#x9;&#x9;&#x9;070.77 - 112.09&#xA;12 Apr 2018&#x9;&#x9;&#x9;071.48 - 112.80&#xA;13 Apr 2018&#x9;&#x9;&#x9;072.75 - 112.89&#xA;14 Apr 2018&#x9;&#x9;&#x9;073.41 - 113.55&#xA;15 Apr 2018&#x9;&#x9;&#x9;074.04 - 114.18&#xA;16 Apr 2018&#x9;&#x9;&#x9;074.65 - 114.79&#xA;17 Apr 2018&#x9;&#x9;&#x9;075.42 - 115.18&#xA;18 Apr 2018&#x9;&#x9;&#x9;075.99 - 115.75&#xA;19 Apr 2018&#x9;&#x9;&#x9;076.54 - 116.30&#xA;20 Apr 2018&#x9;&#x9;&#x9;077.31 - 116.59&#xA;21 Apr 2018&#x9;&#x9;&#x9;077.83 - 117.11&#xA;22 Apr 2018&#x9;&#x9;&#x9;078.33 - 117.61&#xA;23 Apr 2018&#x9;&#x9;&#x9;078.18 - 118.72&#xA;24 Apr 2018&#x9;&#x9;&#x9;078.65 - 119.19&#xA;25 Apr 2018&#x9;&#x9;&#x9;079.11 - 119.65&#xA;26 Apr 2018&#x9;&#x9;&#x9;079.56 - 120.10&#xA;27 Apr 2018&#x9;&#x9;&#x9;079.29 - 121.23&#xA;28 Apr 2018&#x9;&#x9;&#x9;079.71 - 121.65&#xA;29 Apr 2018&#x9;&#x9;&#x9;080.13 - 122.07&#xA;30 Apr 2018&#x9;&#x9;&#x9;079.75 - 123.25&#xA;01 May 2018&#x9;&#x9;&#x9;080.14 - 123.64&#xA;02 May 2018&#x9;&#x9;&#x9;080.53 - 124.03&#xA;03 May 2018&#x9;&#x9;&#x9;080.01 - 125.31&#xA;04 May 2018&#x9;&#x9;&#x9;080.38 - 125.68&#xA;05 May 2018&#x9;&#x9;&#x9;080.74 - 126.04&#xA;06 May 2018&#x9;&#x9;&#x9;080.11 - 127.37&#xA;07 May 2018&#x9;&#x9;&#x9;080.46 - 127.72&#xA;08 May 2018&#x9;&#x9;&#x9;080.80 - 128.06&#xA;09 May 2018&#x9;&#x9;&#x9;081.14 - 128.40&#xA;10 May 2018&#x9;&#x9;&#x9;080.34 - 129.86&#xA;11 May 2018&#x9;&#x9;&#x9;080.66 - 130.18&#xA;12 May 2018&#x9;&#x9;&#x9;081.14 - 130.34&#xA;13 May 2018&#x9;&#x9;&#x9;081.66 - 130.46&#xA;14 May 2018&#x9;&#x9;&#x9;082.17 - 130.57&#xA;15 May 2018&#x9;&#x9;&#x9;082.58 - 130.78&#xA;16 May 2018&#x9;&#x9;&#x9;083.08 - 130.88&#xA;17 May 2018&#x9;&#x9;&#x9;083.48 - 131.08&#xA;18 May 2018&#x9;&#x9;&#x9;083.97 - 131.17&#xA;19 May 2018&#x9;&#x9;&#x9;084.36 - 131.36&#xA;20 May 2018&#x9;&#x9;&#x9;084.75 - 131.55&#xA;21 May 2018&#x9;&#x9;&#x9;085.04 - 131.84&#xA;22 May 2018&#x9;&#x9;&#x9;085.42 - 132.02&#xA;23 May 2018&#x9;&#x9;&#x9;085.90 - 132.10&#xA;24 May 2018&#x9;&#x9;&#x9;086.28 - 132.28&#xA;25 May 2018&#x9;&#x9;&#x9;086.56 - 132.56&#xA;26 May 2018&#x9;&#x9;&#x9;086.93 - 132.73&#xA;27 May 2018&#x9;&#x9;&#x9;087.30 - 132.90&#xA;28 May 2018&#x9;&#x9;&#x9;087.67 - 133.07&#xA;29 May 2018&#x9;&#x9;&#x9;087.95 - 133.33&#xA;30 May 2018&#x9;&#x9;&#x9;088.31 - 133.51&#xA;31 May 2018&#x9;&#x9;&#x9;088.57 - 133.77&#xA;01 Jun 2018&#x9;&#x9;&#x9;088.94 - 133.94&#xA;02 Jun 2018&#x9;&#x9;&#x9;089.20 - 134.20&#xA;03 Jun 2018&#x9;&#x9;&#x9;089.47 - 134.47&#xA;04 Jun 2018&#x9;&#x9;&#x9;089.73 - 134.73&#xA;05 Jun 2018&#x9;&#x9;&#x9;089.99 - 134.99&#xA;06 Jun 2018&#x9;&#x9;&#x9;090.25 - 135.25&#xA;07 Jun 2018&#x9;&#x9;&#x9;090.61 - 135.41&#xA;08 Jun 2018&#x9;&#x9;&#x9;108.27 - 118.27&#xA;09 Jun 2018&#x9;&#x9;&#x9;108.54 - 118.54&#xA;10 Jun 2018&#x9;&#x9;&#x9;108.80 - 118.80&#xA;11 Jun 2018&#x9;&#x9;&#x9;109.06 - 119.06&#xA;12 Jun 2018&#x9;&#x9;&#x9;109.32 - 119.32&#xA;13 Jun 2018&#x9;&#x9;&#x9;109.58 - 119.58&#xA;14 Jun 2018&#x9;&#x9;&#x9;109.85 - 119.85&#xA;15 Jun 2018&#x9;&#x9;&#x9;110.11 - 120.11&#xA;16 Jun 2018&#x9;&#x9;&#x9;110.38 - 120.38&#xA;17 Jun 2018&#x9;&#x9;&#x9;110.64 - 120.64&#xA;18 Jun 2018&#x9;&#x9;&#x9;110.91 - 120.91&#xA;19 Jun 2018&#x9;&#x9;&#x9;111.18 - 121.18&#xA;20 Jun 2018&#x9;&#x9;&#x9;111.45 - 121.45&#xA;21 Jun 2018&#x9;&#x9;&#x9;111.72 - 121.72&#xA;22 Jun 2018&#x9;&#x9;&#x9;112.00 - 122.00&#xA;23 Jun 2018&#x9;&#x9;&#x9;112.27 - 122.27&#xA;24 Jun 2018&#x9;&#x9;&#x9;112.55 - 122.55&#xA;25 Jun 2018&#x9;&#x9;&#x9;112.83 - 122.83&#xA;26 Jun 2018&#x9;&#x9;&#x9;113.12 - 123.12&#xA;27 Jun 2018&#x9;&#x9;&#x9;113.40 - 123.40&#xA;28 Jun 2018&#x9;&#x9;&#x9;113.69 - 123.69&#xA;29 Jun 2018&#x9;&#x9;&#x9;113.98 - 123.98&#xA;30 Jun 2018&#x9;&#x9;&#x9;114.28 - 124.28&#xA;01 Jul 2018&#x9;&#x9;&#x9;114.58 - 124.58&#xA;02 Jul 2018&#x9;&#x9;&#x9;114.88 - 124.88&#xA;03 Jul 2018&#x9;&#x9;&#x9;115.19 - 125.19&#xA;04 Jul 2018&#x9;&#x9;&#x9;115.50 - 125.50&#xA;05 Jul 2018&#x9;&#x9;&#x9;115.82 - 125.82&#xA;06 Jul 2018&#x9;&#x9;&#x9;116.14 - 126.14&#xA;07 Jul 2018&#x9;&#x9;&#x9;116.46 - 126.46&#xA;08 Jul 2018&#x9;&#x9;&#x9;116.80 - 126.80&#xA;09 Jul 2018&#x9;&#x9;&#x9;117.13 - 127.13&#xA;10 Jul 2018&#x9;&#x9;&#x9;117.47 - 127.47&#xA;11 Jul 2018&#x9;&#x9;&#x9;117.82 - 127.82&#xA;12 Jul 2018&#x9;&#x9;&#x9;118.18 - 128.18&#xA;13 Jul 2018&#x9;&#x9;&#x9;118.54 - 128.54&#xA;14 Jul 2018&#x9;&#x9;&#x9;118.91 - 128.91&#xA;15 Jul 2018&#x9;&#x9;&#x9;119.29 - 129.29&#xA;16 Jul 2018&#x9;&#x9;&#x9;119.68 - 129.68&#xA;17 Jul 2018&#x9;&#x9;&#x9;120.07 - 130.07&#xA;18 Jul 2018&#x9;&#x9;&#x9;120.47 - 130.47&#xA;19 Jul 2018&#x9;&#x9;&#x9;120.89 - 130.89&#xA;20 Jul 2018&#x9;&#x9;&#x9;121.31 - 131.31&#xA;29 Oct 2018&#x9;&#x9;&#x9;274.74 - 284.74&#xA;30 Oct 2018&#x9;&#x9;&#x9;275.18 - 285.18&#xA;31 Oct 2018&#x9;&#x9;&#x9;275.62 - 285.62&#xA;01 Nov 2018&#x9;&#x9;&#x9;276.05 - 286.05&#xA;02 Nov 2018&#x9;&#x9;&#x9;276.46 - 286.46&#xA;03 Nov 2018&#x9;&#x9;&#x9;276.87 - 286.87&#xA;04 Nov 2018&#x9;&#x9;&#x9;277.27 - 287.27&#xA;05 Nov 2018&#x9;&#x9;&#x9;277.66 - 287.66&#xA;06 Nov 2018&#x9;&#x9;&#x9;278.04 - 288.04&#xA;07 Nov 2018&#x9;&#x9;&#x9;278.42 - 288.42&#xA;08 Nov 2018&#x9;&#x9;&#x9;278.78 - 288.78&#xA;09 Nov 2018&#x9;&#x9;&#x9;279.14 - 289.14&#xA;10 Nov 2018&#x9;&#x9;&#x9;279.50 - 289.50&#xA;11 Nov 2018&#x9;&#x9;&#x9;279.84 - 289.84&#xA;12 Nov 2018&#x9;&#x9;&#x9;280.19 - 290.19&#xA;13 Nov 2018&#x9;&#x9;&#x9;280.52 - 290.52&#xA;14 Nov 2018&#x9;&#x9;&#x9;280.86 - 290.86&#xA;15 Nov 2018&#x9;&#x9;&#x9;281.18 - 291.18&#xA;16 Nov 2018&#x9;&#x9;&#x9;281.51 - 291.51&#xA;17 Nov 2018&#x9;&#x9;&#x9;281.82 - 291.82&#xA;18 Nov 2018&#x9;&#x9;&#x9;282.14 - 292.14&#xA;19 Nov 2018&#x9;&#x9;&#x9;282.45 - 292.45&#xA;20 Nov 2018&#x9;&#x9;&#x9;282.76 - 292.76&#xA;21 Nov 2018&#x9;&#x9;&#x9;283.06 - 293.06&#xA;22 Nov 2018&#x9;&#x9;&#x9;283.36 - 293.36&#xA;23 Nov 2018&#x9;&#x9;&#x9;283.66 - 293.66&#xA;24 Nov 2018&#x9;&#x9;&#x9;283.95 - 293.95&#xA;25 Nov 2018&#x9;&#x9;&#x9;284.25 - 294.25&#xA;26 Nov 2018&#x9;&#x9;&#x9;284.54 - 294.54&#xA;27 Nov 2018&#x9;&#x9;&#x9;284.83 - 294.83&#xA;28 Nov 2018&#x9;&#x9;&#x9;285.11 - 295.11&#xA;29 Nov 2018&#x9;&#x9;&#x9;285.40 - 295.40&#xA;30 Nov 2018&#x9;&#x9;&#x9;285.68 - 295.68&#xA;01 Dec 2018&#x9;&#x9;&#x9;285.96 - 295.96&#xA;02 Dec 2018&#x9;&#x9;&#x9;286.24 - 296.24&#xA;03 Dec 2018&#x9;&#x9;&#x9;286.52 - 296.52&#xA;04 Dec 2018&#x9;&#x9;&#x9;286.80 - 296.80&#xA;05 Dec 2018&#x9;&#x9;&#x9;287.08 - 297.08&#xA;06 Dec 2018&#x9;&#x9;&#x9;287.36 - 297.36&#xA;07 Dec 2018&#x9;&#x9;&#x9;287.64 - 297.64&#xA;08 Dec 2018&#x9;&#x9;&#x9;287.91 - 297.91&#xA;09 Dec 2018&#x9;&#x9;&#x9;270.79 - 315.59&#xA;10 Dec 2018&#x9;&#x9;&#x9;270.97 - 315.97&#xA;11 Dec 2018&#x9;&#x9;&#x9;271.25 - 316.25&#xA;12 Dec 2018&#x9;&#x9;&#x9;271.53 - 316.53&#xA;13 Dec 2018&#x9;&#x9;&#x9;271.80 - 316.80&#xA;14 Dec 2018&#x9;&#x9;&#x9;272.08 - 317.08&#xA;15 Dec 2018&#x9;&#x9;&#x9;272.26 - 317.46&#xA;16 Dec 2018&#x9;&#x9;&#x9;272.55 - 317.75&#xA;17 Dec 2018&#x9;&#x9;&#x9;272.74 - 318.12&#xA;18 Dec 2018&#x9;&#x9;&#x9;273.01 - 318.41&#xA;19 Dec 2018&#x9;&#x9;&#x9;273.20 - 318.80&#xA;20 Dec 2018&#x9;&#x9;&#x9;273.39 - 319.19&#xA;21 Dec 2018&#x9;&#x9;&#x9;273.58 - 319.58&#xA;22 Dec 2018&#x9;&#x9;&#x9;273.87 - 319.87&#xA;23 Dec 2018&#x9;&#x9;&#x9;274.16 - 320.16&#xA;24 Dec 2018&#x9;&#x9;&#x9;274.36 - 320.56&#xA;25 Dec 2018&#x9;&#x9;&#x9;274.46 - 321.06&#xA;26 Dec 2018&#x9;&#x9;&#x9;274.66 - 321.46&#xA;27 Dec 2018&#x9;&#x9;&#x9;274.86 - 321.86&#xA;28 Dec 2018&#x9;&#x9;&#x9;275.07 - 322.27&#xA;29 Dec 2018&#x9;&#x9;&#x9;275.18 - 322.78&#xA;30 Dec 2018&#x9;&#x9;&#x9;275.40 - 323.20&#xA;31 Dec 2018&#x9;&#x9;&#x9;275.52 - 323.72&#xA;01 Jan 2019&#x9;&#x9;&#x9;275.74 - 324.14&#xA;02 Jan 2019&#x9;&#x9;&#x9;275.87 - 324.67&#xA;03 Jan 2019&#x9;&#x9;&#x9;276.01 - 325.21&#xA;04 Jan 2019&#x9;&#x9;&#x9;276.19 - 325.71&#xA;05 Jan 2019&#x9;&#x9;&#x9;276.53 - 326.05&#xA;06 Jan 2019&#x9;&#x9;&#x9;278.01 - 325.27&#xA;07 Jan 2019&#x9;&#x9;&#x9;278.37 - 325.63&#xA;08 Jan 2019&#x9;&#x9;&#x9;278.73 - 325.99&#xA;09 Jan 2019&#x9;&#x9;&#x9;280.09 - 325.39&#xA;10 Jan 2019&#x9;&#x9;&#x9;280.46 - 325.76&#xA;11 Jan 2019&#x9;&#x9;&#x9;280.85 - 326.15&#xA;12 Jan 2019&#x9;&#x9;&#x9;282.14 - 325.64&#xA;13 Jan 2019&#x9;&#x9;&#x9;282.55 - 326.05&#xA;14 Jan 2019&#x9;&#x9;&#x9;282.96 - 326.46&#xA;15 Jan 2019&#x9;&#x9;&#x9;284.16 - 326.10&#xA;16 Jan 2019&#x9;&#x9;&#x9;284.60 - 326.54&#xA;17 Jan 2019&#x9;&#x9;&#x9;285.04 - 326.98&#xA;18 Jan 2019&#x9;&#x9;&#x9;286.20 - 326.74&#xA;19 Jan 2019&#x9;&#x9;&#x9;286.67 - 327.21&#xA;20 Jan 2019&#x9;&#x9;&#x9;287.15 - 327.69&#xA;21 Jan 2019&#x9;&#x9;&#x9;287.64 - 328.18&#xA;22 Jan 2019&#x9;&#x9;&#x9;288.78 - 328.06&#xA;23 Jan 2019&#x9;&#x9;&#x9;289.31 - 328.59&#xA;24 Jan 2019&#x9;&#x9;&#x9;289.85 - 329.13&#xA;25 Jan 2019&#x9;&#x9;&#x9;290.17 - 329.93&#xA;26 Jan 2019&#x9;&#x9;&#x9;290.75 - 330.51&#xA;27 Jan 2019&#x9;&#x9;&#x9;291.35 - 331.11&#xA;28 Jan 2019&#x9;&#x9;&#x9;291.78 - 331.92&#xA;29 Jan 2019&#x9;&#x9;&#x9;292.43 - 332.57&#xA;30 Jan 2019&#x9;&#x9;&#x9;293.10 - 333.24&#xA;31 Jan 2019&#x9;&#x9;&#x9;293.20 - 334.52&#xA;01 Feb 2019&#x9;&#x9;&#x9;293.93 - 335.25&#xA;02 Feb 2019&#x9;&#x9;&#x9;294.68 - 336.00&#xA;03 Feb 2019&#x9;&#x9;&#x9;294.57 - 337.69&#xA;04 Feb 2019&#x9;&#x9;&#x9;295.39 - 338.51&#xA;05 Feb 2019&#x9;&#x9;&#x9;296.24 - 339.36&#xA;06 Feb 2019&#x9;&#x9;&#x9;297.14 - 340.26&#xA;07 Feb 2019&#x9;&#x9;&#x9;296.87 - 342.41&#xA;08 Feb 2019&#x9;&#x9;&#x9;297.85 - 343.39&#xA;09 Feb 2019&#x9;&#x9;&#x9;298.89 - 344.43&#xA;10 Feb 2019&#x9;&#x9;&#x9;298.30 - 347.20&#xA;11 Feb 2019&#x9;&#x9;&#x9;299.44 - 348.34&#xA;12 Feb 2019&#x9;&#x9;&#x9;300.64 - 349.54&#xA;13 Feb 2019&#x9;&#x9;&#x9;301.92 - 350.82&#xA;14 Feb 2019&#x9;&#x9;&#x9;300.88 - 354.54&#xA;15 Feb 2019&#x9;&#x9;&#x9;302.30 - 355.96&#xA;16 Feb 2019&#x9;&#x9;&#x9;303.80 - 357.46&#xA;17 Feb 2019&#x9;&#x9;&#x9;305.39 - 359.05&#xA;18 Feb 2019&#x9;&#x9;&#x9;303.91 - 003.91&#xA;19 Feb 2019&#x9;&#x9;&#x9;305.69 - 005.69&#xA;20 Feb 2019&#x9;&#x9;&#x9;307.59 - 007.59&#xA;21 Feb 2019&#x9;&#x9;&#x9;309.60 - 009.60&#xA;22 Feb 2019&#x9;&#x9;&#x9;311.73 - 011.73&#xA;23 Feb 2019&#x9;&#x9;&#x9;314.00 - 014.00&#xA;24 Feb 2019&#x9;&#x9;&#x9;316.40 - 016.40&#xA;25 Feb 2019&#x9;&#x9;&#x9;318.93 - 018.93&#xA;26 Feb 2019&#x9;&#x9;&#x9;321.61 - 021.61&#xA;27 Feb 2019&#x9;&#x9;&#x9;324.44 - 024.44&#xA;28 Feb 2019&#x9;&#x9;&#x9;327.40 - 027.40&#xA;01 Mar 2019&#x9;&#x9;&#x9;330.51 - 030.51&#xA;02 Mar 2019&#x9;&#x9;&#x9;333.75 - 033.75&#xA;03 Mar 2019&#x9;&#x9;&#x9;337.11 - 037.11&#xA;04 Mar 2019&#x9;&#x9;&#x9;340.57 - 040.57&#xA;05 Mar 2019&#x9;&#x9;&#x9;344.12 - 044.12&#xA;06 Mar 2019&#x9;&#x9;&#x9;347.74 - 047.74&#xA;07 Mar 2019&#x9;&#x9;&#x9;351.39 - 051.39&#xA;08 Mar 2019&#x9;&#x9;&#x9;355.06 - 055.06&#xA;09 Mar 2019&#x9;&#x9;&#x9;358.70 - 058.70&#xA;10 Mar 2019&#x9;&#x9;&#x9;002.31 - 062.31&#xA;11 Mar 2019&#x9;&#x9;&#x9;005.84 - 065.84&#xA;12 Mar 2019&#x9;&#x9;&#x9;009.29 - 069.29&#xA;13 Mar 2019&#x9;&#x9;&#x9;012.63 - 072.63&#xA;14 Mar 2019&#x9;&#x9;&#x9;015.84 - 075.84&#xA;15 Mar 2019&#x9;&#x9;&#x9;018.92 - 078.92&#xA;16 Mar 2019&#x9;&#x9;&#x9;021.86 - 081.86&#xA;17 Mar 2019&#x9;&#x9;&#x9;024.65 - 084.65&#xA;18 Mar 2019&#x9;&#x9;&#x9;027.31 - 087.31&#xA;19 Mar 2019&#x9;&#x9;&#x9;029.81 - 089.81&#xA;20 Mar 2019&#x9;&#x9;&#x9;032.18 - 092.18&#xA;21 Mar 2019&#x9;&#x9;&#x9;034.42 - 094.42&#xA;22 Mar 2019&#x9;&#x9;&#x9;036.53 - 096.53&#xA;23 Mar 2019&#x9;&#x9;&#x9;038.52 - 098.52&#xA;24 Mar 2019&#x9;&#x9;&#x9;040.39 - 100.39&#xA;25 Mar 2019&#x9;&#x9;&#x9;042.15 - 102.15&#xA;26 Mar 2019&#x9;&#x9;&#x9;046.99 - 100.65&#xA;27 Mar 2019&#x9;&#x9;&#x9;048.56 - 102.22&#xA;28 Mar 2019&#x9;&#x9;&#x9;050.05 - 103.71&#xA;29 Mar 2019&#x9;&#x9;&#x9;051.45 - 105.11&#xA;30 Mar 2019&#x9;&#x9;&#x9;055.15 - 104.05&#xA;31 Mar 2019&#x9;&#x9;&#x9;056.41 - 105.31&#xA;01 Apr 2019&#x9;&#x9;&#x9;057.01 - 105.91&#xA;"
                        Label="Roll Ranges Report"
                        Target="HD-93396"
                        Coordinates="RA: 10 46 49.7407,  DEC: -09 23 56.49"
                        Prefix="Orient"
                        Units="U3">
                        
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