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----- Attempting Submission 1 (Thu Mar 19 18:41:33 GMT 2026) -----
HST Phase I Proposal 6949  successfully submitted.
Receipt: # 6949-1</SubmissionLog>
            
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HST Phase II Proposal 18238  successfully submitted.
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      <Title>AT2018cow: A Unique Laboratory for Super-Eddington Accretion and Black-hole Growth</Title>
      
      <Abstract>Black-hole accretion via a disk plays a fundamental role in astronomy. In the past decade, a number of accretion-powered systems have been discovered that defy standard models, motivating new frameworks for disk evolution that accurately treat the poorly understood regime of super-Eddington accretion. An ideal test case for new disk-evolution models is AT2018cow, an accretion-powered transient in a galaxy only 60 Mpc away. We propose to observe AT2018cow's accretion disk using JWST and HST. We will model the newly observed UVOIR SED, together with existing X-ray observations, using a new framework for the long-term evolution of accretion disks that takes super-Eddington accretion into account. The observations and modeling will enable us to both refine the modeling framework and infer the black-hole mass (a key degeneracy between competing progenitor models). JWST/NIRCam is essential because its angular resolution will enable AT2018cow to be separated from the background much better than the existing HST measurements. NIRCam's NIR sensitivity also has the potential to detect an underlying compact cluster, which would further help distinguish between progenitor scenarios and enable the cluster contribution to be jointly modeled with the accretion disk emission. A newly formed accretion disk in a very nearby system that underwent super-Eddington accretion is a rare opportunity: AT2018cow is a unique probe of a poorly understood regime of accretion physics that is likely critical for understanding massive BH growth at high redshift, as well as for determining the progenitors of new transient classes.</Abstract>
      
      <PrincipalInvestigator
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         MiddleInitial="Yen Qin"
         LastName="Ho"
         ESAMember="false"
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         Retired="false"
         UniqueID="25270"
         Institution="Cornell University"
         Country="USA"
         State="NY"
         Contact="true" />
      
      <CoInvestigator
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         MiddleInitial="James"
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         UniqueID="6925"
         Institution="Radboud University Nijmegen"
         Country="NLD"
         Contact="false"
         AdminUSPI="false" />
      
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         FirstName="Daniel"
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         UniqueID="8520"
         Institution="Liverpool John Moores University"
         Country="GBR"
         State="England"
         Contact="false"
         AdminUSPI="false" />
      
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         FirstName="Eliot"
         LastName="Quataert"
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         UniqueID="6112"
         Institution="Princeton University"
         Country="USA"
         State="NJ"
         Contact="false"
         AdminUSPI="false" />
      
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         LastName="Camilo"
         ESAMember="false"
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         UniqueID="55874"
         Institution="Cornell University"
         Country="USA"
         State="NY"
         Contact="false"
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         FirstName="Rahul"
         LastName="Jayaraman"
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         UniqueID="47267"
         Institution="Cornell University"
         Country="USA"
         State="NY"
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         FirstName="Anne"
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         Institution="University of Bath"
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         FirstName="Mila"
         LastName="Winter-Granic"
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         Institution="Princeton University"
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         FirstName="Stephen"
         MiddleInitial="Bradley"
         LastName="Cenko"
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         UniqueID="7374"
         Institution="NASA Goddard Space Flight Center"
         Country="USA"
         State="MD"
         Contact="false"
         AdminUSPI="false" />
      
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We use the UVIS2-C1K1C-SUB as we only need to image the compact source, not the extended emission from the galaxy.  This also increases possible exposure time by making the readout faster.

We use a FLASH level of 21 electrons to maintain charge transfer efficiency, and this threshold would set the lamp at a higher setting and reduce overheads.</ObservingDescription>
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      <TeamExpertise>Our team includes experts in the analysis of JWST/NIRCam and HST/WFC3 data (Andrew Levan, Anne Inkenhaag). Our team also includes experts in accretion-disk modeling: co-Is Mila Winter-Granic and Eliot Quataert developed the new framework for the evolution of super-Eddington accretion disks employed here. Finally, our team includes experts on AT2018cow itself and on interpreting the multiwavelength emission from accretion-powered transients, including taking their underlying cluster properties into account (Daniel Perley, Andrew Levan, Anne Inkenhaag, Anna Ho, Brad Cenko, Michael Camilo, Rahul Jayaraman). Therefore the team is well prepared to reduce, analyze, model, and interpret the observations that we are proposing.</TeamExpertise>
      
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319.87&#xA;06 Jan 2026&#x9;&#x9;&#x9;308.97 - 318.97&#xA;07 Jan 2026&#x9;&#x9;&#x9;308.08 - 318.08&#xA;08 Jan 2026&#x9;&#x9;&#x9;307.19 - 317.19&#xA;09 Jan 2026&#x9;&#x9;&#x9;306.32 - 316.32&#xA;10 Jan 2026&#x9;&#x9;&#x9;305.46 - 315.46&#xA;11 Jan 2026&#x9;&#x9;&#x9;304.61 - 314.61&#xA;12 Jan 2026&#x9;&#x9;&#x9;303.77 - 313.77&#xA;13 Jan 2026&#x9;&#x9;&#x9;302.94 - 312.94&#xA;14 Jan 2026&#x9;&#x9;&#x9;302.12 - 312.12&#xA;15 Jan 2026&#x9;&#x9;&#x9;301.30 - 311.30&#xA;16 Jan 2026&#x9;&#x9;&#x9;300.50 - 310.50&#xA;17 Jan 2026&#x9;&#x9;&#x9;299.70 - 309.70&#xA;18 Jan 2026&#x9;&#x9;&#x9;298.91 - 308.91&#xA;19 Jan 2026&#x9;&#x9;&#x9;298.12 - 308.12&#xA;20 Jan 2026&#x9;&#x9;&#x9;297.35 - 307.35&#xA;21 Jan 2026&#x9;&#x9;&#x9;296.58 - 306.58&#xA;22 Jan 2026&#x9;&#x9;&#x9;295.81 - 305.81&#xA;23 Jan 2026&#x9;&#x9;&#x9;295.06 - 305.06&#xA;24 Jan 2026&#x9;&#x9;&#x9;294.31 - 304.31&#xA;25 Jan 2026&#x9;&#x9;&#x9;293.56 - 303.56&#xA;26 Jan 2026&#x9;&#x9;&#x9;292.82 - 302.82&#xA;27 Jan 2026&#x9;&#x9;&#x9;292.08 - 302.08&#xA;28 Jan 2026&#x9;&#x9;&#x9;291.35 - 301.35&#xA;29 Jan 2026&#x9;&#x9;&#x9;290.63 - 300.63&#xA;30 Jan 2026&#x9;&#x9;&#x9;289.91 - 299.91&#xA;31 Jan 2026&#x9;&#x9;&#x9;289.19 - 289.19&#xA;01 Feb 2026&#x9;&#x9;&#x9;288.48 - 298.48&#xA;02 Feb 2026&#x9;&#x9;&#x9;287.77 - 297.77&#xA;03 Feb 2026&#x9;&#x9;&#x9;287.06 - 297.06&#xA;04 Feb 2026&#x9;&#x9;&#x9;286.36 - 296.36&#xA;05 Feb 2026&#x9;&#x9;&#x9;285.65 - 295.65&#xA;06 Feb 2026&#x9;&#x9;&#x9;284.96 - 294.96&#xA;07 Feb 2026&#x9;&#x9;&#x9;284.26 - 294.26&#xA;08 Feb 2026&#x9;&#x9;&#x9;283.57 - 293.57&#xA;09 Feb 2026&#x9;&#x9;&#x9;282.87 - 292.87&#xA;10 Feb 2026&#x9;&#x9;&#x9;282.18 - 292.18&#xA;11 Feb 2026&#x9;&#x9;&#x9;281.49 - 291.49&#xA;12 Feb 2026&#x9;&#x9;&#x9;280.81 - 290.81&#xA;13 Feb 2026&#x9;&#x9;&#x9;280.12 - 290.12&#xA;14 Feb 2026&#x9;&#x9;&#x9;279.43 - 289.43&#xA;15 Feb 2026&#x9;&#x9;&#x9;278.75 - 288.75&#xA;16 Feb 2026&#x9;&#x9;&#x9;268.06 - 298.06&#xA;17 Feb 2026&#x9;&#x9;&#x9;267.38 - 297.38&#xA;18 Feb 2026&#x9;&#x9;&#x9;266.69 - 296.69&#xA;19 Feb 2026&#x9;&#x9;&#x9;266.01 - 296.01&#xA;20 Feb 2026&#x9;&#x9;&#x9;265.32 - 295.32&#xA;21 Feb 2026&#x9;&#x9;&#x9;264.63 - 294.63&#xA;22 Feb 2026&#x9;&#x9;&#x9;263.94 - 293.94&#xA;23 Feb 2026&#x9;&#x9;&#x9;263.26 - 293.26&#xA;24 Feb 2026&#x9;&#x9;&#x9;262.56 - 292.56&#xA;25 Feb 2026&#x9;&#x9;&#x9;261.87 - 276.87&#xA;26 Feb 2026&#x9;&#x9;&#x9;261.18 - 266.18&#xA;28 Feb 2026&#x9;&#x9;&#x9;259.78 - 264.78&#x9;279.78 - 289.78&#xA;01 Mar 2026&#x9;&#x9;&#x9;251.28 - 296.88&#xA;02 Mar 2026&#x9;&#x9;&#x9;250.47 - 296.27&#xA;03 Mar 2026&#x9;&#x9;&#x9;249.76 - 295.56&#xA;04 Mar 2026&#x9;&#x9;&#x9;248.95 - 294.95&#xA;05 Mar 2026&#x9;&#x9;&#x9;248.24 - 294.24&#xA;06 Mar 2026&#x9;&#x9;&#x9;267.52 - 293.52&#xA;07 Mar 2026&#x9;&#x9;&#x9;276.70 - 292.90&#xA;08 Mar 2026&#x9;&#x9;&#x9;287.37 - 292.37&#xA;20 Mar 2026&#x9;&#x9;&#x9;279.31 - 284.31&#xA;21 Mar 2026&#x9;&#x9;&#x9;274.50 - 283.70&#xA;22 Mar 2026&#x9;&#x9;&#x9;268.69 - 282.89&#xA;23 Mar 2026&#x9;&#x9;&#x9;262.70 - 282.22&#xA;24 Mar 2026&#x9;&#x9;&#x9;256.87 - 281.39&#xA;25 Mar 2026&#x9;&#x9;&#x9;251.03 - 280.55&#xA;26 Mar 2026&#x9;&#x9;&#x9;246.31 - 256.31&#x9;271.31 - 278.57&#xA;27 Mar 2026&#x9;&#x9;&#x9;240.45 - 260.45&#x9;272.71 - 277.71&#xA;28 Mar 2026&#x9;&#x9;&#x9;234.58 - 276.84&#xA;29 Mar 2026&#x9;&#x9;&#x9;228.70 - 275.96&#xA;30 Mar 2026&#x9;&#x9;&#x9;228.79 - 274.09&#xA;31 Mar 2026&#x9;&#x9;&#x9;227.89 - 273.19&#xA;01 Apr 2026&#x9;&#x9;&#x9;226.98 - 272.28&#xA;02 Apr 2026&#x9;&#x9;&#x9;226.06 - 271.36&#xA;03 Apr 2026&#x9;&#x9;&#x9;225.13 - 270.43&#xA;04 Apr 2026&#x9;&#x9;&#x9;225.08 - 268.58&#xA;05 Apr 2026&#x9;&#x9;&#x9;224.12 - 267.62&#xA;06 Apr 2026&#x9;&#x9;&#x9;223.15 - 266.65&#xA;07 Apr 2026&#x9;&#x9;&#x9;222.17 - 265.67&#xA;08 Apr 2026&#x9;&#x9;&#x9;221.18 - 264.68&#xA;09 Apr 2026&#x9;&#x9;&#x9;220.17 - 263.67&#xA;10 Apr 2026&#x9;&#x9;&#x9;219.93 - 261.87&#xA;11 Apr 2026&#x9;&#x9;&#x9;218.90 - 260.84&#xA;12 Apr 2026&#x9;&#x9;&#x9;217.85 - 259.79&#xA;13 Apr 2026&#x9;&#x9;&#x9;216.79 - 258.73&#xA;14 Apr 2026&#x9;&#x9;&#x9;215.71 - 257.65&#xA;15 Apr 2026&#x9;&#x9;&#x9;214.62 - 256.56&#xA;16 Apr 2026&#x9;&#x9;&#x9;214.22 - 254.76&#xA;17 Apr 2026&#x9;&#x9;&#x9;213.10 - 253.64&#xA;18 Apr 2026&#x9;&#x9;&#x9;211.97 - 252.51&#xA;19 Apr 2026&#x9;&#x9;&#x9;210.82 - 251.36&#xA;20 Apr 2026&#x9;&#x9;&#x9;209.66 - 250.20&#xA;21 Apr 2026&#x9;&#x9;&#x9;208.49 - 249.03&#xA;22 Apr 2026&#x9;&#x9;&#x9;207.30 - 247.84&#xA;23 Apr 2026&#x9;&#x9;&#x9;206.72 - 246.00&#xA;24 Apr 2026&#x9;&#x9;&#x9;Date not checked.&#xA;25 Apr 2026&#x9;&#x9;&#x9;Date not checked.&#xA;26 Apr 2026&#x9;&#x9;&#x9;Date not checked.&#xA;27 Apr 2026&#x9;&#x9;&#x9;Date not checked.&#xA;28 Apr 2026&#x9;&#x9;&#x9;Date not checked.&#xA;29 Apr 2026&#x9;&#x9;&#x9;Date not checked.&#xA;30 Apr 2026&#x9;&#x9;&#x9;Date not checked.&#xA;01 May 2026&#x9;&#x9;&#x9;Date not checked.&#xA;02 May 2026&#x9;&#x9;&#x9;Date not checked.&#xA;03 May 2026&#x9;&#x9;&#x9;Date not checked.&#xA;04 May 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 May 2026&#x9;&#x9;&#x9;200.00 - 205.47&#xA;24 May 2026&#x9;&#x9;&#x9;164.31 - 164.31&#x9;190.00 - 204.07&#xA;25 May 2026&#x9;&#x9;&#x9;162.92 - 162.92&#x9;175.00 - 202.68&#xA;26 May 2026&#x9;&#x9;&#x9;161.53 - 201.29&#xA;27 May 2026&#x9;&#x9;&#x9;160.16 - 199.92&#xA;28 May 2026&#x9;&#x9;&#x9;158.79 - 198.55&#xA;29 May 2026&#x9;&#x9;&#x9;Date not checked.&#xA;30 May 2026&#x9;&#x9;&#x9;Date not checked.&#xA;31 May 2026&#x9;&#x9;&#x9;Date not checked.&#xA;01 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;02 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;03 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;04 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;05 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;06 Jun 2026&#x9;&#x9;&#x9;177.22 - 186.50&#xA;07 Jun 2026&#x9;&#x9;&#x9;180.00 - 185.25&#xA;08 Jun 2026&#x9;&#x9;&#x9;184.02 - 184.02&#xA;14 Jul 2026&#x9;&#x9;&#x9;144.35 - 144.35&#xA;15 Jul 2026&#x9;&#x9;&#x9;143.57 - 143.57&#xA;16 Jul 2026&#x9;&#x9;&#x9;142.99 - 146.79&#xA;19 Jul 2026&#x9;&#x9;&#x9;149.22 - 149.22&#xA;06 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;07 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;08 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;09 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;10 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;11 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;12 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;13 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;14 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;18 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;19 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;20 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;21 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;22 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;24 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;25 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;26 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;27 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;28 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;29 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;30 Nov 2026&#x9;&#x9;&#x9;Date not checked.&#xA;01 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;14 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;18 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;19 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;20 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;21 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;22 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;24 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;25 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;26 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;27 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;28 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;29 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;30 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;05 Jan 2027&#x9;&#x9;&#x9;310.10 - 320.10&#xA;06 Jan 2027&#x9;&#x9;&#x9;309.20 - 319.20&#xA;07 Jan 2027&#x9;&#x9;&#x9;308.30 - 318.30&#xA;08 Jan 2027&#x9;&#x9;&#x9;307.42 - 317.42&#xA;09 Jan 2027&#x9;&#x9;&#x9;306.55 - 316.55&#xA;10 Jan 2027&#x9;&#x9;&#x9;305.68 - 315.68&#xA;11 Jan 2027&#x9;&#x9;&#x9;304.83 - 314.83&#xA;12 Jan 2027&#x9;&#x9;&#x9;303.99 - 313.99&#xA;13 Jan 2027&#x9;&#x9;&#x9;303.15 - 313.15&#xA;14 Jan 2027&#x9;&#x9;&#x9;302.33 - 312.33&#xA;15 Jan 2027&#x9;&#x9;&#x9;301.51 - 311.51&#xA;16 Jan 2027&#x9;&#x9;&#x9;300.70 - 310.70&#xA;17 Jan 2027&#x9;&#x9;&#x9;299.90 - 309.90&#xA;18 Jan 2027&#x9;&#x9;&#x9;299.11 - 309.11&#xA;19 Jan 2027&#x9;&#x9;&#x9;298.32 - 308.32&#xA;20 Jan 2027&#x9;&#x9;&#x9;297.55 - 307.55&#xA;21 Jan 2027&#x9;&#x9;&#x9;296.77 - 306.77&#xA;22 Jan 2027&#x9;&#x9;&#x9;296.01 - 306.01&#xA;23 Jan 2027&#x9;&#x9;&#x9;295.25 - 305.25&#xA;24 Jan 2027&#x9;&#x9;&#x9;294.50 - 304.50&#xA;25 Jan 2027&#x9;&#x9;&#x9;293.75 - 303.75&#xA;26 Jan 2027&#x9;&#x9;&#x9;293.01 - 303.01&#xA;27 Jan 2027&#x9;&#x9;&#x9;292.27 - 302.27&#xA;28 Jan 2027&#x9;&#x9;&#x9;291.54 - 301.54&#xA;29 Jan 2027&#x9;&#x9;&#x9;290.81 - 300.81&#xA;30 Jan 2027&#x9;&#x9;&#x9;290.09 - 300.09&#xA;31 Jan 2027&#x9;&#x9;&#x9;289.37 - 299.37&#xA;01 Feb 2027&#x9;&#x9;&#x9;288.66 - 298.66&#xA;02 Feb 2027&#x9;&#x9;&#x9;287.95 - 297.95&#xA;03 Feb 2027&#x9;&#x9;&#x9;287.24 - 297.24&#xA;04 Feb 2027&#x9;&#x9;&#x9;286.54 - 296.54&#xA;05 Feb 2027&#x9;&#x9;&#x9;285.83 - 295.83&#xA;06 Feb 2027&#x9;&#x9;&#x9;285.13 - 295.13&#xA;07 Feb 2027&#x9;&#x9;&#x9;284.44 - 294.44&#xA;08 Feb 2027&#x9;&#x9;&#x9;283.74 - 293.74&#xA;09 Feb 2027&#x9;&#x9;&#x9;283.05 - 293.05&#xA;10 Feb 2027&#x9;&#x9;&#x9;282.36 - 292.36&#xA;11 Feb 2027&#x9;&#x9;&#x9;281.67 - 291.67&#xA;12 Feb 2027&#x9;&#x9;&#x9;280.98 - 290.98&#xA;13 Feb 2027&#x9;&#x9;&#x9;280.30 - 290.30&#xA;14 Feb 2027&#x9;&#x9;&#x9;279.61 - 289.61&#xA;15 Feb 2027&#x9;&#x9;&#x9;278.92 - 288.92&#xA;16 Feb 2027&#x9;&#x9;&#x9;268.24 - 268.24&#xA;19 Feb 2027&#x9;&#x9;&#x9;266.18 - 296.18&#xA;20 Feb 2027&#x9;&#x9;&#x9;265.50 - 295.50&#xA;21 Feb 2027&#x9;&#x9;&#x9;264.81 - 294.81&#xA;22 Feb 2027&#x9;&#x9;&#x9;264.12 - 294.12&#xA;23 Feb 2027&#x9;&#x9;&#x9;263.43 - 293.43&#xA;24 Feb 2027&#x9;&#x9;&#x9;262.74 - 292.74&#xA;25 Feb 2027&#x9;&#x9;&#x9;262.05 - 292.05&#xA;26 Feb 2027&#x9;&#x9;&#x9;261.35 - 291.35&#xA;27 Feb 2027&#x9;&#x9;&#x9;260.66 - 290.66&#xA;28 Feb 2027&#x9;&#x9;&#x9;259.96 - 289.96&#xA;01 Mar 2027&#x9;&#x9;&#x9;251.46 - 297.06&#xA;02 Mar 2027&#x9;&#x9;&#x9;250.75 - 296.35&#xA;03 Mar 2027&#x9;&#x9;&#x9;249.95 - 295.75&#xA;04 Mar 2027&#x9;&#x9;&#x9;249.14 - 295.14&#xA;05 Mar 2027&#x9;&#x9;&#x9;248.42 - 294.42&#xA;06 Mar 2027&#x9;&#x9;&#x9;247.70 - 293.70&#xA;07 Mar 2027&#x9;&#x9;&#x9;246.88 - 293.08&#xA;08 Mar 2027&#x9;&#x9;&#x9;245.95 - 292.55&#xA;09 Mar 2027&#x9;&#x9;&#x9;245.22 - 291.82&#xA;10 Mar 2027&#x9;&#x9;&#x9;254.39 - 291.19&#xA;11 Mar 2027&#x9;&#x9;&#x9;268.55 - 290.55&#xA;12 Mar 2027&#x9;&#x9;&#x9;282.80 - 289.80&#xA;13 Mar 2027&#x9;&#x9;&#x9;289.15 - 289.15&#xA;25 Mar 2027&#x9;&#x9;&#x9;280.77 - 280.77&#xA;26 Mar 2027&#x9;&#x9;&#x9;273.79 - 278.79&#xA;27 Mar 2027&#x9;&#x9;&#x9;270.67 - 277.93&#xA;28 Mar 2027&#x9;&#x9;&#x9;264.80 - 277.06&#xA;29 Mar 2027&#x9;&#x9;&#x9;258.93 - 276.19&#xA;30 Mar 2027&#x9;&#x9;&#x9;253.04 - 275.30&#xA;31 Mar 2027&#x9;&#x9;&#x9;243.12 - 273.42&#xA;01 Apr 2027&#x9;&#x9;&#x9;237.22 - 272.52&#xA;02 Apr 2027&#x9;&#x9;&#x9;231.30 - 271.60&#xA;03 Apr 2027&#x9;&#x9;&#x9;225.37 - 270.67&#xA;04 Apr 2027&#x9;&#x9;&#x9;224.42 - 269.72&#xA;05 Apr 2027&#x9;&#x9;&#x9;224.37 - 267.87&#xA;06 Apr 2027&#x9;&#x9;&#x9;223.40 - 266.90&#xA;07 Apr 2027&#x9;&#x9;&#x9;222.43 - 265.93&#xA;08 Apr 2027&#x9;&#x9;&#x9;221.43 - 264.93&#xA;09 Apr 2027&#x9;&#x9;&#x9;220.43 - 263.93&#xA;10 Apr 2027&#x9;&#x9;&#x9;220.19 - 262.13&#xA;11 Apr 2027&#x9;&#x9;&#x9;219.16 - 261.10&#xA;12 Apr 2027&#x9;&#x9;&#x9;218.12 - 260.06&#xA;13 Apr 2027&#x9;&#x9;&#x9;217.06 - 257.06&#xA;14 Apr 2027&#x9;&#x9;&#x9;215.99 - 257.93&#xA;15 Apr 2027&#x9;&#x9;&#x9;214.90 - 256.84&#xA;16 Apr 2027&#x9;&#x9;&#x9;214.50 - 255.04&#xA;17 Apr 2027&#x9;&#x9;&#x9;213.39 - 253.93&#xA;18 Apr 2027&#x9;&#x9;&#x9;212.26 - 252.80&#xA;19 Apr 2027&#x9;&#x9;&#x9;211.12 - 251.66&#xA;20 Apr 2027&#x9;&#x9;&#x9;209.96 - 250.50&#xA;21 Apr 2027&#x9;&#x9;&#x9;208.79 - 249.33&#xA;22 Apr 2027&#x9;&#x9;&#x9;207.60 - 248.14&#xA;23 Apr 2027&#x9;&#x9;&#x9;207.03 - 246.31&#xA;24 Apr 2027&#x9;&#x9;&#x9;205.82 - 245.10&#xA;25 Apr 2027&#x9;&#x9;&#x9;204.59 - 243.87&#xA;26 Apr 2027&#x9;&#x9;&#x9;203.35 - 242.63&#xA;27 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xA;28 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xA;29 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xA;"
                        Label="Roll Ranges Report"
                        Target="SN-2018COW"
                        Coordinates="RA: 16 16 0.2200,  DEC: +22 16 4.91"
                        Prefix="Orient"
                        Units="U3">
                        
                        <StConstraintSchedulingWindows
                           Name="Roll Report Data"
                           Type="Roll Ranges"
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