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<HSTProposal
   Phase2ID="18190"
   Phase="Phase II"
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   <!--APT Version: Version 2026.5.1  -->
   <!--Date: Mon Sep 14 18:55:56 GMT 2026-->
   
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            SubmissionSuccessCounter="2"
            HasErrors="false"
            Cycle="33"
            IncludeSysInfo="true"
            NotificationAddress="maureenvandenberg@icloud.com">
            
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            <SubmissionComments>The UVIS aperture has been changed to UVIS2, which is a better choice for out program.

note added 14-sep-2026: this is an intermediate version of our observation setup, to check the visibility of our ToO target</SubmissionComments>
            
            <SubmissionCommentsCheckSum>647941735</SubmissionCommentsCheckSum>
            
            <SubmissionLog>----- Attempting Submission 1 (Thu Oct 02 22:21:32 GMT 2025) -----
HST Phase II Proposal 18190  successfully submitted.
Receipt: # 18190-1

----- Attempting Submission 2 (Mon Oct 13 18:59:49 GMT 2025) -----

----- Attempting Submission 3 (Mon Sep 14 18:55:56 GMT 2026) -----</SubmissionLog>
            
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   <ProposalInformation
      Category="GO"
      SnapPriority="Normal Priority"
      PureParallelProposal="false"
      Cycle="33"
      STScIEditNumber="0">
      
      <Title>Transient LMXBs in globular clusters</Title>
      
      <Abstract>Deep Chandra observations of globular clusters have revealed that globular clusters contain numerous quiescent LMXBs, any of which could go into outburst. Recent Chandra studies have confirmed that globular clusters can indeed harbor multiple transients and that more quiescent LMXBs are hiding under the sensitivity limits of even relatively deep Chandra exposures. Both findings have significant implications for studies of accreting neutron stars and have provided better insight into globular cluster compact binary populations. Here we propose a Chandra program to precisely localize new transients in globular clusters. As part of this effort we further request HST observations to identify the optical counterparts of these transients.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Jeroen"
         LastName="Homan"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="7513"
         Institution="Eureka Scientific Inc."
         Country="USA"
         State="CA"
         Contact="true" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Maureen"
         LastName="van den Berg"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="7519"
         Institution="Harvard University"
         Country="USA"
         State="MA"
         Contact="true"
         AdminUSPI="false"
         CoPI="true" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="David"
         MiddleInitial="A."
         LastName="Pooley"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="6662"
         Institution="Eureka Scientific Inc."
         Country="USA"
         State="CA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Craig"
         LastName="Heinke"
         ESAMember="false"
         CSAMember="true"
         Retired="false"
         UniqueID="5929"
         Institution="University of Alberta"
         Country="CAN"
         State="AB"
         Contact="false"
         AdminUSPI="false" />
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>* General background for the program
The goal of this joint Chandra/HST Target-of-Opportunity (ToO) proposal is to measure accurate coordinates of the next two X-ray transients in a globular cluster with Chandra, and to use HST subsequently to look for their optical counterparts inside the Chandra positional error circles. The Chandra error circle is large enough (about 0.6" radius) that it likely contains multiple globular-cluster stars. Comparison of the photometry that is extracted from the observations requested here with photometry from archival HST data reveals highly variable objects in the error circle, and hence the identity of the true counterpart. Our choice for the WFC3/UVIS is driven by the existence of a large body of archival globular-cluster images taken with this camera. We have been allocated time to do Chandra/HST follow-up for two X-ray transients. For the HST component we were granted 4 HST orbits in total (2 orbits per transient). 

* The first trigger - September 2026
Late August 2026, Einstein Probe detected an outburst of an X-ray transient in the globular cluster NGC6440. Subsequent Swift observations in September 2026 confirmed the association of the transient with NGC6440. This X-ray transient has not been confidently identified with any of the known X-ray transients in the cluster. We have triggered our Chandra ToO program to obtain an accurate X-ray position of the source. The Chandra observations will be performed on **late September / early October**. We have triggered the HST component of our program to search for the optical counterpart.

* Visit 1
Our program for Visit 1 to observe NGC6440 consists of observations in the F606W and F814W filters as there are already archival UVIS data in these filters that we can use for comparison. The observations are organized in a 4-point dither-box pattern to improve the resolution. We aim for a S/N&gt;10 for a star of mag [TBD] (F606W, F814W). We also include short observations to get photometry of bright stars, and of stars near bright stars. 

****** Note added 14-sep-2026: this is a preliminary setup to check the visibility of our target for HST *****</ObservingDescription>
         </Phase2Questions>
      </Questions>
      
      <TeamExpertise>All team members have extensive expertise in Chandra data analysis and are experts on (transient) X-ray sources in globular clusters. They all have led past Chandra observations of globular clusters. Dr. Heinke and Dr. Homan have studied and modeled crustal cooling or accretion heated neutron stars. Dr. Homan and Dr. Pooley will lead the analysis of the Chandra data. Dr. van den Berg has extensive expertise with the analysis of HST observations and will lead the analysis of the HST data. All team members will contribute to the interpretation of the data and publishing of the results.</TeamExpertise>
      
      <Orbits
         ThisCycle2GyroPrimary="4"
         ThisCycle2GyroParallel="0"
         NextCycle2GyroPrimary="0"
         NextCycle2GyroParallel="0"
         AfterNext2GyroPrimary="0"
         AfterNext2GyroParallel="0" />
      
      <TargetOfOpportunityActivations
         NonDisruptive="2" />
      
      <Phase1ProposalInformation
         LongTermMonitoring="false"
         Attachment="/Users/maureen/Research/Observe/chandra25/gctransients/final/27400223_jhoman_sj.pdf"
         ProposalSize="VERY SMALL">
         
         <ScientificCategory>Stellar Populations and the Interstellar Medium</ScientificCategory>
         
         <SecondaryScientificCategory>Stellar Physics and Stellar Types</SecondaryScientificCategory>
         
         <ScientificKeyword1
            Keyword="Globular star clusters" />
         
         <ScientificKeyword2
            Keyword="Interacting binary stars" />
         
         <ScientificKeyword3
            Keyword="Neutron stars" />
         
         <ScientificKeyword4
            Keyword="Transient sources" />
         
         <ProprietaryPeriod
            Default="true">6</ProprietaryPeriod>
         
         <CalibProp>false</CalibProp>
         
         <UvInit>false</UvInit>
         
         <Treasury>false</Treasury>
         
         <MultiCycleTreasury>false</MultiCycleTreasury>
         
         <GoArchival>false</GoArchival>
         
         <HstRomanScience>false</HstRomanScience>
         
         <HWOPrecursorScience>false</HWOPrecursorScience>
         
         <MultiObservatory>true</MultiObservatory>
         
         <MultiObservatoryRole>SECONDARY</MultiObservatoryRole>
         
         <PrimarySubmission>
            
            <PrimaryTac>CHANDRA</PrimaryTac>
            
            <PrimaryProposalId>27400223</PrimaryProposalId>
         </PrimarySubmission>
         
         <NoDuplicateProposalSubmissions>false</NoDuplicateProposalSubmissions>
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      <Phase2ProposalInformation
         PCFlag="true"
         ProposalSize="SMALL_CYCLE21">
         
         <Availability>SUPPORTED</Availability>
      </Phase2ProposalInformation>
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   <Targets>
      
      <FixedTarget
         Name="NGC6440-TRANSIENT"
         Number="1"
         ReferenceFrame="ICRS"
         ICRS="true"
         PMNotApplicable="false"
         Epoch="2000">
         
         <PrimaryCategory>STELLAR CLUSTER</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>GLOBULAR CLUSTER</Description>
         </PrimaryDescription>
         
         <Extended>NO</Extended>
         
         <Comments>Our target is a to-be-identified star in the globular cluster NGC6440. The counterpart that we aim to identify is expected to have a magnitude in F606W m(F435W) &gt;~ 16.</Comments>
         
         <AlternateNames />
         
         <EquatorialPosition
            Value="17 48 52.2240 -20 21 36.86">
            
            <RAUnc
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            <DECUnc
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            <Equinox>J2000</Equinox>
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         Number="2">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>X-RAY TRANSIENT</Description>
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         <Comments>next X-ray transient discovered in a Galactic globular cluster, whose position can only be accurately determined with Chandra</Comments>
         
         <Criteria
            FreeText="false">first trigger of globular-cluster X-ray transient program</Criteria>
         
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            <BroadBandMagnitude
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               Magnitude="19" />
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         Instrument="WFC3"
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         NumberOfOrbits="2"
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277.79&#xA;18 Feb 2026&#x9;&#x9;&#x9;267.72 - 277.72&#xA;19 Feb 2026&#x9;&#x9;&#x9;267.66 - 277.66&#xA;20 Feb 2026&#x9;&#x9;&#x9;267.59 - 277.59&#xA;21 Feb 2026&#x9;&#x9;&#x9;267.52 - 277.52&#xA;22 Feb 2026&#x9;&#x9;&#x9;267.46 - 277.46&#xA;23 Feb 2026&#x9;&#x9;&#x9;267.40 - 277.40&#xA;24 Feb 2026&#x9;&#x9;&#x9;267.33 - 277.33&#xA;25 Feb 2026&#x9;&#x9;&#x9;267.27 - 277.27&#xA;26 Feb 2026&#x9;&#x9;&#x9;267.21 - 277.21&#xA;27 Feb 2026&#x9;&#x9;&#x9;267.15 - 277.15&#xA;28 Feb 2026&#x9;&#x9;&#x9;267.09 - 272.09&#xA;01 Mar 2026&#x9;&#x9;&#x9;267.03 - 267.03&#xA;02 Mar 2026&#x9;&#x9;&#x9;266.97 - 276.97&#xA;03 Mar 2026&#x9;&#x9;&#x9;266.92 - 276.92&#xA;04 Mar 2026&#x9;&#x9;&#x9;266.86 - 276.86&#xA;05 Mar 2026&#x9;&#x9;&#x9;266.80 - 276.80&#xA;06 Mar 2026&#x9;&#x9;&#x9;266.75 - 276.75&#xA;07 Mar 2026&#x9;&#x9;&#x9;266.69 - 276.69&#xA;08 Mar 2026&#x9;&#x9;&#x9;266.64 - 276.64&#xA;09 Mar 2026&#x9;&#x9;&#x9;266.58 - 276.58&#xA;10 Mar 2026&#x9;&#x9;&#x9;266.53 - 276.53&#xA;11 Mar 2026&#x9;&#x9;&#x9;266.47 - 276.47&#xA;12 Mar 2026&#x9;&#x9;&#x9;266.42 - 276.42&#xA;13 Mar 2026&#x9;&#x9;&#x9;266.37 - 276.37&#xA;14 Mar 2026&#x9;&#x9;&#x9;266.31 - 276.31&#xA;15 Mar 2026&#x9;&#x9;&#x9;266.26 - 276.26&#xA;16 Mar 2026&#x9;&#x9;&#x9;266.21 - 276.21&#xA;17 Mar 2026&#x9;&#x9;&#x9;266.15 - 276.15&#xA;18 Mar 2026&#x9;&#x9;&#x9;256.10 - 286.10&#xA;19 Mar 2026&#x9;&#x9;&#x9;256.05 - 286.05&#xA;20 Mar 2026&#x9;&#x9;&#x9;255.99 - 285.99&#xA;21 Mar 2026&#x9;&#x9;&#x9;255.94 - 285.94&#xA;22 Mar 2026&#x9;&#x9;&#x9;255.89 - 285.89&#xA;23 Mar 2026&#x9;&#x9;&#x9;255.83 - 285.83&#xA;24 Mar 2026&#x9;&#x9;&#x9;255.78 - 285.78&#xA;25 Mar 2026&#x9;&#x9;&#x9;255.73 - 285.73&#xA;26 Mar 2026&#x9;&#x9;&#x9;255.67 - 285.67&#xA;30 Mar 2026&#x9;&#x9;&#x9;257.46 - 282.46&#xA;31 Mar 2026&#x9;&#x9;&#x9;247.40 - 277.40&#xA;01 Apr 2026&#x9;&#x9;&#x9;247.25 - 262.25&#xA;02 Apr 2026&#x9;&#x9;&#x9;247.19 - 252.19&#xA;03 Apr 2026&#x9;&#x9;&#x9;246.93 - 246.93&#xA;11 Apr 2026&#x9;&#x9;&#x9;245.36 - 245.36&#xA;12 Apr 2026&#x9;&#x9;&#x9;245.09 - 250.09&#xA;13 Apr 2026&#x9;&#x9;&#x9;244.87 - 254.87&#xA;14 Apr 2026&#x9;&#x9;&#x9;244.81 - 259.81&#xA;15 Apr 2026&#x9;&#x9;&#x9;245.87 - 265.87&#xA;16 Apr 2026&#x9;&#x9;&#x9;245.80 - 275.80&#xA;17 Apr 2026&#x9;&#x9;&#x9;245.73 - 280.73&#xA;18 Apr 2026&#x9;&#x9;&#x9;246.64 - 286.94&#xA;19 Apr 2026&#x9;&#x9;&#x9;246.57 - 291.87&#xA;20 Apr 2026&#x9;&#x9;&#x9;246.50 - 291.80&#xA;21 Apr 2026&#x9;&#x9;&#x9;247.33 - 290.83&#xA;22 Apr 2026&#x9;&#x9;&#x9;247.25 - 290.75&#xA;23 Apr 2026&#x9;&#x9;&#x9;247.17 - 252.17&#xA;26 Apr 2026&#x9;&#x9;&#x9;267.71 - 277.71&#xA;27 Apr 2026&#x9;&#x9;&#x9;248.32 - 288.86&#xA;28 Apr 2026&#x9;&#x9;&#x9;248.24 - 288.78&#xA;29 Apr 2026&#x9;&#x9;&#x9;248.14 - 288.68&#xA;30 Apr 2026&#x9;&#x9;&#x9;248.68 - 287.96&#xA;01 May 2026&#x9;&#x9;&#x9;248.59 - 287.87&#xA;02 May 2026&#x9;&#x9;&#x9;248.49 - 287.77&#xA;03 May 2026&#x9;&#x9;&#x9;248.14 - 287.90&#xA;04 May 2026&#x9;&#x9;&#x9;248.04 - 287.80&#xA;05 May 2026&#x9;&#x9;&#x9;247.93 - 287.69&#xA;06 May 2026&#x9;&#x9;&#x9;247.62 - 287.76&#xA;07 May 2026&#x9;&#x9;&#x9;247.51 - 287.65&#xA;08 May 2026&#x9;&#x9;&#x9;247.38 - 287.52&#xA;09 May 2026&#x9;&#x9;&#x9;246.67 - 287.99&#xA;10 May 2026&#x9;&#x9;&#x9;246.53 - 287.85&#xA;11 May 2026&#x9;&#x9;&#x9;246.39 - 287.71&#xA;12 May 2026&#x9;&#x9;&#x9;246.25 - 287.57&#xA;13 May 2026&#x9;&#x9;&#x9;245.20 - 288.32&#xA;14 May 2026&#x9;&#x9;&#x9;245.04 - 288.16&#xA;15 May 2026&#x9;&#x9;&#x9;244.87 - 287.99&#xA;16 May 2026&#x9;&#x9;&#x9;243.48 - 289.02&#xA;17 May 2026&#x9;&#x9;&#x9;243.30 - 288.84&#xA;18 May 2026&#x9;&#x9;&#x9;243.10 - 288.64&#xA;19 May 2026&#x9;&#x9;&#x9;241.22 - 290.12&#xA;20 May 2026&#x9;&#x9;&#x9;276.00 - 289.90&#xA;23 May 2026&#x9;&#x9;&#x9;267.87 - 267.87&#xA;24 May 2026&#x9;&#x9;&#x9;237.58 - 257.58&#xA;25 May 2026&#x9;&#x9;&#x9;234.10 - 249.10&#xA;26 May 2026&#x9;&#x9;&#x9;233.77 - 243.77&#xA;27 May 2026&#x9;&#x9;&#x9;233.41 - 243.41&#xA;28 May 2026&#x9;&#x9;&#x9;233.02 - 238.02&#xA;29 May 2026&#x9;&#x9;&#x9;232.60 - 237.60&#xA;30 May 2026&#x9;&#x9;&#x9;232.13 - 237.13&#xA;31 May 2026&#x9;&#x9;&#x9;231.62 - 236.62&#xA;01 Jun 2026&#x9;&#x9;&#x9;231.05 - 241.05&#xA;02 Jun 2026&#x9;&#x9;&#x9;230.42 - 245.42&#xA;03 Jun 2026&#x9;&#x9;&#x9;229.71 - 249.71&#xA;04 Jun 2026&#x9;&#x9;&#x9;228.91 - 253.91&#xA;05 Jun 2026&#x9;&#x9;&#x9;228.01 - 258.01&#xA;06 Jun 2026&#x9;&#x9;&#x9;226.96 - 266.96&#xA;07 Jun 2026&#x9;&#x9;&#x9;225.75 - 270.75&#xA;08 Jun 2026&#x9;&#x9;&#x9;224.33 - 279.33&#xA;09 Jun 2026&#x9;&#x9;&#x9;222.64 - 282.64&#xA;10 Jun 2026&#x9;&#x9;&#x9;220.61 - 280.61&#xA;11 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;12 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;13 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;14 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;18 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;19 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;20 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;21 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;22 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 Jun 2026&#x9;&#x9;&#x9;Date not checked.&#xA;24 Jun 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;02 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;03 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;04 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;05 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;06 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;07 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;08 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;09 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;10 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;11 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;12 Dec 2026&#x9;&#x9;&#x9;Date not checked.&#xA;13 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;06 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;07 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;08 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;09 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;10 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;11 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;12 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;13 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;14 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;15 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;16 Jan 2027&#x9;&#x9;&#x9;Date not checked.&#xA;17 Feb 2027&#x9;&#x9;&#x9;267.81 - 277.81&#xA;20 Feb 2027&#x9;&#x9;&#x9;267.61 - 267.61&#xA;21 Feb 2027&#x9;&#x9;&#x9;267.54 - 277.54&#xA;22 Feb 2027&#x9;&#x9;&#x9;267.48 - 277.48&#xA;23 Feb 2027&#x9;&#x9;&#x9;267.41 - 277.41&#xA;24 Feb 2027&#x9;&#x9;&#x9;267.35 - 277.35&#xA;25 Feb 2027&#x9;&#x9;&#x9;267.29 - 277.29&#xA;26 Feb 2027&#x9;&#x9;&#x9;267.23 - 277.23&#xA;27 Feb 2027&#x9;&#x9;&#x9;267.16 - 277.16&#xA;28 Feb 2027&#x9;&#x9;&#x9;267.11 - 277.11&#xA;01 Mar 2027&#x9;&#x9;&#x9;267.05 - 277.05&#xA;02 Mar 2027&#x9;&#x9;&#x9;266.99 - 276.99&#xA;03 Mar 2027&#x9;&#x9;&#x9;266.93 - 276.93&#xA;04 Mar 2027&#x9;&#x9;&#x9;266.87 - 276.87&#xA;05 Mar 2027&#x9;&#x9;&#x9;266.82 - 276.82&#xA;06 Mar 2027&#x9;&#x9;&#x9;266.76 - 276.76&#xA;07 Mar 2027&#x9;&#x9;&#x9;266.71 - 276.71&#xA;08 Mar 2027&#x9;&#x9;&#x9;266.65 - 276.65&#xA;09 Mar 2027&#x9;&#x9;&#x9;266.60 - 276.60&#xA;10 Mar 2027&#x9;&#x9;&#x9;266.54 - 276.54&#xA;11 Mar 2027&#x9;&#x9;&#x9;266.49 - 276.49&#xA;12 Mar 2027&#x9;&#x9;&#x9;266.43 - 276.43&#xA;13 Mar 2027&#x9;&#x9;&#x9;266.38 - 276.38&#xA;14 Mar 2027&#x9;&#x9;&#x9;266.33 - 276.33&#xA;15 Mar 2027&#x9;&#x9;&#x9;266.27 - 276.27&#xA;16 Mar 2027&#x9;&#x9;&#x9;266.22 - 276.22&#xA;17 Mar 2027&#x9;&#x9;&#x9;271.17 - 276.17&#xA;20 Mar 2027&#x9;&#x9;&#x9;266.01 - 276.01&#xA;21 Mar 2027&#x9;&#x9;&#x9;255.95 - 285.95&#xA;22 Mar 2027&#x9;&#x9;&#x9;255.90 - 285.90&#xA;23 Mar 2027&#x9;&#x9;&#x9;255.85 - 285.85&#xA;24 Mar 2027&#x9;&#x9;&#x9;255.79 - 285.79&#xA;25 Mar 2027&#x9;&#x9;&#x9;255.74 - 285.74&#xA;26 Mar 2027&#x9;&#x9;&#x9;255.69 - 285.69&#xA;27 Mar 2027&#x9;&#x9;&#x9;255.63 - 285.63&#xA;28 Mar 2027&#x9;&#x9;&#x9;255.58 - 285.58&#xA;29 Mar 2027&#x9;&#x9;&#x9;247.73 - 293.33&#xA;30 Mar 2027&#x9;&#x9;&#x9;247.57 - 293.37&#xA;31 Mar 2027&#x9;&#x9;&#x9;247.42 - 293.42&#xA;01 Apr 2027&#x9;&#x9;&#x9;247.36 - 293.36&#xA;02 Apr 2027&#x9;&#x9;&#x9;247.20 - 288.40&#xA;03 Apr 2027&#x9;&#x9;&#x9;246.95 - 271.95&#xA;04 Apr 2027&#x9;&#x9;&#x9;246.79 - 256.79&#xA;05 Apr 2027&#x9;&#x9;&#x9;246.63 - 251.63&#xA;06 Apr 2027&#x9;&#x9;&#x9;246.47 - 246.47&#xA;13 Apr 2027&#x9;&#x9;&#x9;244.89 - 244.89&#xA;14 Apr 2027&#x9;&#x9;&#x9;244.82 - 244.82&#xA;15 Apr 2027&#x9;&#x9;&#x9;245.89 - 250.89&#xA;16 Apr 2027&#x9;&#x9;&#x9;245.82 - 255.82&#xA;17 Apr 2027&#x9;&#x9;&#x9;245.75 - 265.75&#xA;18 Apr 2027&#x9;&#x9;&#x9;246.66 - 271.66&#xA;19 Apr 2027&#x9;&#x9;&#x9;246.59 - 276.59&#xA;20 Apr 2027&#x9;&#x9;&#x9;246.52 - 281.52&#xA;21 Apr 2027&#x9;&#x9;&#x9;247.35 - 290.85&#xA;22 Apr 2027&#x9;&#x9;&#x9;247.27 - 290.77&#xA;23 Apr 2027&#x9;&#x9;&#x9;247.19 - 290.69&#xA;24 Apr 2027&#x9;&#x9;&#x9;247.89 - 289.83&#xA;25 Apr 2027&#x9;&#x9;&#x9;247.81 - 289.75&#xA;26 Apr 2027&#x9;&#x9;&#x9;247.73 - 289.67&#xA;27 Apr 2027&#x9;&#x9;&#x9;248.35 - 288.89&#xA;28 Apr 2027&#x9;&#x9;&#x9;248.26 - 288.80&#xA;29 Apr 2027&#x9;&#x9;&#x9;248.17 - 288.71&#xA;30 Apr 2027&#x9;&#x9;&#x9;248.71 - 287.99&#xA;01 May 2027&#x9;&#x9;&#x9;248.61 - 287.89&#xA;02 May 2027&#x9;&#x9;&#x9;248.51 - 287.79&#xA;03 May 2027&#x9;&#x9;&#x9;248.41 - 287.69&#xA;04 May 2027&#x9;&#x9;&#x9;248.06 - 287.82&#xA;05 May 2027&#x9;&#x9;&#x9;247.96 - 287.72&#xA;06 May 2027&#x9;&#x9;&#x9;247.84 - 287.60&#xA;07 May 2027&#x9;&#x9;&#x9;247.54 - 287.68&#xA;08 May 2027&#x9;&#x9;&#x9;247.41 - 287.55&#xA;09 May 2027&#x9;&#x9;&#x9;247.29 - 287.43&#xA;10 May 2027&#x9;&#x9;&#x9;246.57 - 287.89&#xA;14 May 2027&#x9;&#x9;&#x9;255.08 - 285.08&#xA;15 May 2027&#x9;&#x9;&#x9;244.91 - 288.03&#xA;16 May 2027&#x9;&#x9;&#x9;243.53 - 289.07&#xA;17 May 2027&#x9;&#x9;&#x9;243.35 - 288.89&#xA;18 May 2027&#x9;&#x9;&#x9;243.15 - 288.69&#xA;19 May 2027&#x9;&#x9;&#x9;241.27 - 290.17&#xA;20 May 2027&#x9;&#x9;&#x9;241.05 - 289.95&#xA;21 May 2027&#x9;&#x9;&#x9;240.82 - 289.72&#xA;22 May 2027&#x9;&#x9;&#x9;238.20 - 291.86&#xA;23 May 2027&#x9;&#x9;&#x9;237.94 - 291.60&#xA;24 May 2027&#x9;&#x9;&#x9;237.66 - 291.32&#xA;25 May 2027&#x9;&#x9;&#x9;234.18 - 279.18&#xA;26 May 2027&#x9;&#x9;&#x9;233.86 - 263.86&#xA;27 May 2027&#x9;&#x9;&#x9;233.51 - 253.51&#xA;28 May 2027&#x9;&#x9;&#x9;233.13 - 248.13&#xA;29 May 2027&#x9;&#x9;&#x9;232.71 - 242.71&#xA;30 May 2027&#x9;&#x9;&#x9;232.26 - 242.26&#xA;31 May 2027&#x9;&#x9;&#x9;231.76 - 236.76&#xA;01 Jun 2027&#x9;&#x9;&#x9;231.20 - 236.20&#xA;02 Jun 2027&#x9;&#x9;&#x9;230.59 - 240.59&#xA;03 Jun 2027&#x9;&#x9;&#x9;229.90 - 239.90&#xA;04 Jun 2027&#x9;&#x9;&#x9;229.13 - 244.13&#xA;05 Jun 2027&#x9;&#x9;&#x9;228.25 - 248.25&#xA;06 Jun 2027&#x9;&#x9;&#x9;227.24 - 252.24&#xA;07 Jun 2027&#x9;&#x9;&#x9;226.08 - 251.08&#xA;08 Jun 2027&#x9;&#x9;&#x9;224.72 - 254.72&#xA;09 Jun 2027&#x9;&#x9;&#x9;223.11 - 258.11&#xA;10 Jun 2027&#x9;&#x9;&#x9;221.17 - 276.17&#xA;11 Jun 2027&#x9;&#x9;&#x9;218.80 - 278.80&#xA;12 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;13 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;14 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;15 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;16 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;17 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;18 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;19 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;20 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;21 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;22 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;23 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;24 Jun 2027&#x9;&#x9;&#x9;Date not checked.&#xA;"
                        Label="Roll Ranges Report"
                        Target="NGC6440-TRANSIENT"
                        Coordinates="RA: 17 48 52.2240,  DEC: -20 21 36.86"
                        Prefix="Orient"
                        Units="U3">
                        
                        <StConstraintSchedulingWindows
                           Name="Roll Report Data"
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