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<HSTProposal
   Phase1ID="7231"
   Phase2ID="18427"
   Phase="Phase II"
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   <!--Date: Fri Aug 07 19:48:57 GMT 2026-->
   
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            <SubmissionLog>----- Attempting Submission 1 (Fri Aug 07 19:35:00 GMT 2026) -----</SubmissionLog>
            
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            <SubmissionLog>Assigned ID: 7231

----- Attempting Submission 1 (Wed Apr 15 22:52:39 GMT 2026) -----
HST Phase I Proposal 7231  successfully submitted.
Receipt: # 7231-1</SubmissionLog>
            
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   <ProposalInformation
      Category="GO"
      SnapPriority="Normal Priority"
      PureParallelProposal="false"
      Cycle="34"
      STScIEditNumber="0">
      
      <Title>Post-periastron Evolution of  Ejecta and Jet-precession in the R Aqr Symbiotic System</Title>
      
      <Abstract>We propose HST/WFC3 observations of the interacting symbiotic system R Aqr, as a followup to the HST archival observations obtained during the recent periastron (with the next periastron expected in about 40 years). Our principal goal is to use the HST unique high-angular resolution UV-optical imaging capability to obtain a detailed post-periastron time-lapse study of the new ejecta and jet/counter-jet propagation, and especially of the jet evolution and precession, at scales close to the binary itself, about 5 AU, to the extended jet-interaction region within 4000 AU from the central binary.  The results will have a great impact on the understanding of other wind accreting, jet-producing systems (e.g., interacting binaries, YSOs, PN, AGN), whose close accreting and jet-forming  environments cannot be currently resolved.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Margarita"
         LastName="Karovska"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="1079"
         Institution="Smithsonian Institution Astrophysical Observatory"
         Country="USA"
         State="MA"
         Contact="true" />
      
      <CoInvestigator
         Honorific="Mr."
         FirstName="Warren"
         MiddleInitial="J."
         LastName="Hack"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="2883"
         Institution="Eureka Scientific Inc."
         Country="USA"
         State="CA"
         Contact="false"
         AdminUSPI="false" />
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>We request a total of 6 orbits, in 2 visits, scheduled within a couple of weeks from each other. The HST high-angular resolution in the spectral regions (filters) that we selected is critical for achieving the science goals of this project. It is very important to have the images at different filters obtained close in time because the R Aqr periastron related outburst and jet structures evolve rapidly, The visits need to be scheduled as close together as possible to keep the orientation as similar as possible due to the HST orbit. This will minimize the errors in combining the exposures and allow us to recover the highest angular-resolution possible to study the origin of the jet of this active system.

We also prefer that the observations are scheduled during Spring-Summer 2027 when the Mira is in the vicinity of (or at) its optical minimum (June-July 2027). The primary component should have a magnitude of V less than 10.5 mag based on the 2023-2026 light curves. This period around the Mira-star minimum starts roughly in April-2027 and goes through September 2027. This will allow the secondary and faint emission components in the core of this system to remain visible without the effects of saturation from the primary. 

The variable nature of the emission from R Aqr will require us to monitor the light curve and spectra closely, using ground based photometry and spectroscopy. Depending on when the observations are scheduled, we may need to adjust the exposures accordingly; specifically, in the month before the actual observations are taken.

We plan to carry out most of the HST WFC3/UVIS imaging of R Aqr using the 4-point dither mode in several filters centered on spectral lines and the nearby continuum. This approach will allow us to reach 0.025''/pixel, and will also assist in cosmic ray removal. Combining the dithered images will result in improvement of the sampling of the PSF and will allow us to further enhance the (nominal 0.04'') resolution using deconvolution techniques such as Richardson-Lucy or EMC2 reaching 0.025''. This will nearly double the number of pixels covering the regions of interest. We also plan several long exposures to image the fainter outer lobes (about 20 arcseconds from the center) and determine their morphology and evolution when compared to the archival HST observations in the past decade. Most of the selected filters were used previously, including in the 2023 WFC3/UVIS observations. This will allow direct comparison and study of the dynamical evolution and proper motions of individual structures (inner jet, knots and blobs, outburst structures etc.).

The images obtained in the spectral lines will provide information on the ionization state, temperature, and density of the gas. The full list of filters we plan to use can be found in the original Phase 1 proposal description. The F343N filter, for example, will provide the [NeV] line intensity and indicate whether temperatures significantly higher than $10^5$ K are present. The Mg II$\lambda$2800\AA\ line has a resonant scattering component and will provide information on the ionization state of the gas. The [OII]$\lambda$3726\AA\ line serves as a density indicator. Furthermore, the [SII]$\lambda$6731\AA/H$\alpha$ ratio will allow us to identify shocked vs. ionized gas emission. The [O III]4363\AA/5007\AA\ ratio gives the temperature which further constrains the shock speed and the ionizing spectrum. The F658N filter will provide an estimate of the [NII] emission and will allow us to calculate the [S II]/[N II] ratio, while also providing density diagnostics where the ratio gets suppressed in the inner regions of R Aqr. The H$\alpha$/H$\beta$ ratio will map the intrinsic reddening, i.e. dust regions/shells along the jet and counter-jet, and perpendicularly to the jet (eg, in the orbital plane).

The exposure times used in this proposal are based on the online WFC3 ETC calculations as verified by the 2023 WFC3 observations of R Aqr. We optimize the efficiency of the observing time by using subarray readouts (1024x1024 readout) to minimize the overheads, while still providing a &gt;=40''x 40'' field of view. Our observations also include post-flash exposure in order to partially remediate the effects of charge-transfer inefficiency due to the age of the detector. 
This proposal was generated using the latest APT based on the desired exposure times to avoid saturation and on the use of dither patterns, and makes the most efficient use of the observing time. 

A reduced gyro mode will not have any significant impact as long as the target is in the HST field-of-regard when the observations need to be taken. This will not require any explicit roll constraints for our observations.</ObservingDescription>
         </Phase2Questions>
      </Questions>
      
      <TeamExpertise>The expertise of our team is complementary (multiwavelength observations and analysis, and theoretical modeling) which will allow us to achieve the goals of our proposal.

PI Dr. Margarita Karovska: Scientific expertise in multiwavelength observational studies and modeling of
interacting binaries including symbiotic systems. High-resolution imaging expertise (including deconvolution
techniques) allowing to achieve maximum resolution (e.g., previous HST, Chandra and VLA observations)
including of symbiotics (R Aqr, CH Cyg, Mira), Planetary Nebulae, and  AGN/quasars and other interacting systems.

(Co-I Warren Hack: Expertise in HST imaging software and data processing expertise (e.g., primary developer of the
Drizzlepac package). He has been applying novel dithered-images combination techniques and PSF simulations,
allowing to reach the finest resolution achievable with the HST (e.g., previous HST studies of symbiotics R
Aqr, CH Cyg, Mira, HM Sge).</TeamExpertise>
      
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      <Phase1ProposalInformation
         LongTermMonitoring="false"
         Attachment="/System/Volumes/Data/solaris/user1/sherwin/18427/E:\data\SCI\R Aqr\proposals\cycle34_2026\Cycle34_raqr_precessionSJ.pdf"
         ProposalSize="VERY SMALL">
         
         <ScientificCategory>Stellar Physics and Stellar Types</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="Binary stars / Trinary stars" />
         
         <ScientificKeyword2
            Keyword="Evolved stars" />
         
         <ScientificKeyword3
            Keyword="Stellar accretion disks" />
         
         <ScientificKeyword4
            Keyword="Stellar jets" />
         
         <ScientificKeyword5
            Keyword="Variable stars" />
         
         <ProprietaryPeriod
            Default="true">6</ProprietaryPeriod>
         
         <CalibProp>false</CalibProp>
         
         <UvInit>true</UvInit>
         
         <Treasury>false</Treasury>
         
         <MultiCycleTreasury>false</MultiCycleTreasury>
         
         <GoArchival>false</GoArchival>
         
         <HstRomanScience>false</HstRomanScience>
         
         <HWOPrecursorScience>false</HWOPrecursorScience>
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      <Phase2ProposalInformation
         PCFlag="true"
         ProposalSize="SMALL_CYCLE21">
         
         <Availability>SUPPORTED</Availability>
      </Phase2ProposalInformation>
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      <FixedTarget
         Name="V-R-AQR"
         Number="1"
         ReferenceFrame="ICRS"
         ICRS="true"
         PMNotApplicable="false"
         ProvisionalCoordinates="23 43 49.4616 -15 17 4.20">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>ACCRETION DISK</Description>
            
            <Description>INTERACTING BINARY</Description>
            
            <Description>JET</Description>
            
            <Description>SYMBIOTIC STAR</Description>
         </PrimaryDescription>
         
         <Comments>This object was generated by the targetselector and retrieved from the SIMBAD database.</Comments>
         
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            <RAUnc
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            <DECUnc
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            <Equinox>J2000</Equinox>
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         <Equinox>J2000</Equinox>
         
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               Magnitude="10"
               MagnitudeUnc="3.0" />
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         NumberOfOrbits="6"
         NumberOfIterations="1"
         TotalOrbits="6"
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            DaysHighMed="0"
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         <CoordinateFrame>POS-TARG</CoordinateFrame>
         
         <Purpose>DITHER</Purpose>
         
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         <PointSpacing>0.145</PointSpacing>
         
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         <Sub-Pattern>false</Sub-Pattern>
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                        Name="&lt;a href=&quot;https://apst.stsci.edu/apt/external/help/documentation/Target-Visibility.html&quot;&gt;Target Visibility&lt;/a&gt;"
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                           <String>Timing link suitability includes constraints ([02 After 01 by at most 14.0 days])</String>
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                     <AncillaryData
                        Title="Comments"
                        Label="Comments">
                        
                        <String>The scheduling data was generated by CASM 34.2.</String>
                        
                        <String>CASM was run in Phase II mode.</String>
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                     Title="Roll Ranges Report"
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012.92&#xD;&#xA;27 Sep 2026&#x9;&#x9;&#x9;355.08 - 010.08&#xD;&#xA;28 Sep 2026&#x9;&#x9;&#x9;357.09 - 007.09&#xD;&#xA;29 Sep 2026&#x9;&#x9;&#x9;358.95 - 003.95&#xD;&#xA;30 Sep 2026&#x9;&#x9;&#x9;000.68 - 000.68&#xD;&#xA;05 Nov 2026&#x9;&#x9;&#x9;035.73 - 035.73&#xD;&#xA;06 Nov 2026&#x9;&#x9;&#x9;035.28 - 035.28&#xD;&#xA;07 Nov 2026&#x9;&#x9;&#x9;035.60 - 035.60&#xD;&#xA;08 Nov 2026&#x9;&#x9;&#x9;035.91 - 035.91&#xD;&#xA;09 Nov 2026&#x9;&#x9;&#x9;035.32 - 035.32&#xD;&#xA;17 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;18 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;19 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;20 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;21 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;22 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;23 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;24 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;25 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;26 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;27 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;28 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;01 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;02 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;03 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;04 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;05 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;06 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;07 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;08 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;09 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;10 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;11 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;12 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;13 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;14 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;15 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;16 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;17 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;18 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;19 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;20 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;21 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;22 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;23 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;24 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;10 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;11 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;12 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;13 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;14 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;15 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;16 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;17 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;18 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;19 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;20 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;21 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;22 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;23 Apr 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;11 May 2027&#x9;&#x9;&#x9;233.98 - 243.98&#xD;&#xA;12 May 2027&#x9;&#x9;&#x9;234.25 - 244.25&#xD;&#xA;13 May 2027&#x9;&#x9;&#x9;234.52 - 244.52&#xD;&#xA;14 May 2027&#x9;&#x9;&#x9;234.78 - 244.78&#xD;&#xA;15 May 2027&#x9;&#x9;&#x9;235.03 - 245.03&#xD;&#xA;16 May 2027&#x9;&#x9;&#x9;235.28 - 245.28&#xD;&#xA;17 May 2027&#x9;&#x9;&#x9;235.53 - 245.53&#xD;&#xA;18 May 2027&#x9;&#x9;&#x9;235.78 - 245.78&#xD;&#xA;19 May 2027&#x9;&#x9;&#x9;236.02 - 246.02&#xD;&#xA;20 May 2027&#x9;&#x9;&#x9;236.26 - 246.26&#xD;&#xA;21 May 2027&#x9;&#x9;&#x9;236.49 - 246.49&#xD;&#xA;22 May 2027&#x9;&#x9;&#x9;236.72 - 246.72&#xD;&#xA;23 May 2027&#x9;&#x9;&#x9;236.95 - 246.95&#xD;&#xA;24 May 2027&#x9;&#x9;&#x9;237.18 - 247.18&#xD;&#xA;25 May 2027&#x9;&#x9;&#x9;237.40 - 247.40&#xD;&#xA;26 May 2027&#x9;&#x9;&#x9;237.63 - 247.63&#xD;&#xA;27 May 2027&#x9;&#x9;&#x9;237.85 - 247.85&#xD;&#xA;28 May 2027&#x9;&#x9;&#x9;238.06 - 248.06&#xD;&#xA;29 May 2027&#x9;&#x9;&#x9;238.28 - 248.28&#xD;&#xA;30 May 2027&#x9;&#x9;&#x9;238.50 - 248.50&#xD;&#xA;31 May 2027&#x9;&#x9;&#x9;238.71 - 248.71&#xD;&#xA;01 Jun 2027&#x9;&#x9;&#x9;238.92 - 248.92&#xD;&#xA;02 Jun 2027&#x9;&#x9;&#x9;239.13 - 249.13&#xD;&#xA;03 Jun 2027&#x9;&#x9;&#x9;239.34 - 249.34&#xD;&#xA;04 Jun 2027&#x9;&#x9;&#x9;239.55 - 249.55&#xD;&#xA;05 Jun 2027&#x9;&#x9;&#x9;239.76 - 249.76&#xD;&#xA;06 Jun 2027&#x9;&#x9;&#x9;239.97 - 249.97&#xD;&#xA;07 Jun 2027&#x9;&#x9;&#x9;240.17 - 250.17&#xD;&#xA;08 Jun 2027&#x9;&#x9;&#x9;240.38 - 250.38&#xD;&#xA;09 Jun 2027&#x9;&#x9;&#x9;240.59 - 250.59&#xD;&#xA;10 Jun 2027&#x9;&#x9;&#x9;240.79 - 250.79&#xD;&#xA;11 Jun 2027&#x9;&#x9;&#x9;241.00 - 251.00&#xD;&#xA;12 Jun 2027&#x9;&#x9;&#x9;231.20 - 261.20&#xD;&#xA;16 Jun 2027&#x9;&#x9;&#x9;232.03 - 242.03&#xD;&#xA;17 Jun 2027&#x9;&#x9;&#x9;232.23 - 262.23&#xD;&#xA;18 Jun 2027&#x9;&#x9;&#x9;232.44 - 262.44&#xD;&#xA;19 Jun 2027&#x9;&#x9;&#x9;232.65 - 262.65&#xD;&#xA;20 Jun 2027&#x9;&#x9;&#x9;232.86 - 262.86&#xD;&#xA;21 Jun 2027&#x9;&#x9;&#x9;233.07 - 263.07&#xD;&#xA;22 Jun 2027&#x9;&#x9;&#x9;225.48 - 271.08&#xD;&#xA;23 Jun 2027&#x9;&#x9;&#x9;225.59 - 271.39&#xD;&#xA;24 Jun 2027&#x9;&#x9;&#x9;225.80 - 271.60&#xD;&#xA;25 Jun 2027&#x9;&#x9;&#x9;225.92 - 271.92&#xD;&#xA;26 Jun 2027&#x9;&#x9;&#x9;226.13 - 272.13&#xD;&#xA;27 Jun 2027&#x9;&#x9;&#x9;226.25 - 272.45&#xD;&#xA;28 Jun 2027&#x9;&#x9;&#x9;226.27 - 272.87&#xD;&#xA;29 Jun 2027&#x9;&#x9;&#x9;226.39 - 273.19&#xD;&#xA;30 Jun 2027&#x9;&#x9;&#x9;226.52 - 273.52&#xD;&#xA;01 Jul 2027&#x9;&#x9;&#x9;226.65 - 273.85&#xD;&#xA;02 Jul 2027&#x9;&#x9;&#x9;226.67 - 274.27&#xD;&#xA;03 Jul 2027&#x9;&#x9;&#x9;226.81 - 274.61&#xD;&#xA;04 Jul 2027&#x9;&#x9;&#x9;226.84 - 275.04&#xD;&#xA;05 Jul 2027&#x9;&#x9;&#x9;226.98 - 275.38&#xD;&#xA;06 Jul 2027&#x9;&#x9;&#x9;227.02 - 267.02&#xD;&#xA;07 Jul 2027&#x9;&#x9;&#x9;227.06 - 257.06&#xD;&#xA;08 Jul 2027&#x9;&#x9;&#x9;227.31 - 252.31&#xD;&#xA;09 Jul 2027&#x9;&#x9;&#x9;227.40 - 252.40&#xD;&#xA;14 Jul 2027&#x9;&#x9;&#x9;230.83 - 250.83&#xD;&#xA;15 Jul 2027&#x9;&#x9;&#x9;231.11 - 256.11&#xD;&#xA;16 Jul 2027&#x9;&#x9;&#x9;231.39 - 261.39&#xD;&#xA;17 Jul 2027&#x9;&#x9;&#x9;232.58 - 267.58&#xD;&#xA;18 Jul 2027&#x9;&#x9;&#x9;232.88 - 272.88&#xD;&#xA;19 Jul 2027&#x9;&#x9;&#x9;233.18 - 276.68&#xD;&#xA;20 Jul 2027&#x9;&#x9;&#x9;234.27 - 276.21&#xD;&#xA;21 Jul 2027&#x9;&#x9;&#x9;234.59 - 276.53&#xD;&#xA;22 Jul 2027&#x9;&#x9;&#x9;234.92 - 276.86&#xD;&#xA;23 Jul 2027&#x9;&#x9;&#x9;235.25 - 277.19&#xD;&#xA;24 Jul 2027&#x9;&#x9;&#x9;236.29 - 276.83&#xD;&#xA;25 Jul 2027&#x9;&#x9;&#x9;236.64 - 277.18&#xD;&#xA;26 Jul 2027&#x9;&#x9;&#x9;237.01 - 277.55&#xD;&#xA;27 Jul 2027&#x9;&#x9;&#x9;238.01 - 277.29&#xD;&#xA;28 Jul 2027&#x9;&#x9;&#x9;238.39 - 277.67&#xD;&#xA;29 Jul 2027&#x9;&#x9;&#x9;238.78 - 278.06&#xD;&#xA;30 Jul 2027&#x9;&#x9;&#x9;238.95 - 278.71&#xD;&#xA;31 Jul 2027&#x9;&#x9;&#x9;239.37 - 279.13&#xD;&#xA;01 Aug 2027&#x9;&#x9;&#x9;239.81 - 279.57&#xD;&#xA;02 Aug 2027&#x9;&#x9;&#x9;240.26 - 280.02&#xD;&#xA;03 Aug 2027&#x9;&#x9;&#x9;240.53 - 280.67&#xD;&#xA;04 Aug 2027&#x9;&#x9;&#x9;241.02 - 281.16&#xD;&#xA;05 Aug 2027&#x9;&#x9;&#x9;241.52 - 281.66&#xD;&#xA;06 Aug 2027&#x9;&#x9;&#x9;266.45 - 282.77&#xD;&#xA;10 Aug 2027&#x9;&#x9;&#x9;242.87 - 257.87&#x9;277.87 - 285.99&#xD;&#xA;11 Aug 2027&#x9;&#x9;&#x9;243.51 - 286.63&#xD;&#xA;12 Aug 2027&#x9;&#x9;&#x9;244.19 - 287.31&#xD;&#xA;13 Aug 2027&#x9;&#x9;&#x9;243.68 - 289.22&#xD;&#xA;14 Aug 2027&#x9;&#x9;&#x9;244.43 - 289.97&#xD;&#xA;15 Aug 2027&#x9;&#x9;&#x9;245.21 - 290.75&#xD;&#xA;16 Aug 2027&#x9;&#x9;&#x9;244.35 - 293.25&#xD;&#xA;17 Aug 2027&#x9;&#x9;&#x9;245.22 - 294.12&#xD;&#xA;18 Aug 2027&#x9;&#x9;&#x9;246.14 - 295.04&#xD;&#xA;19 Aug 2027&#x9;&#x9;&#x9;247.11 - 296.01&#xD;&#xA;20 Aug 2027&#x9;&#x9;&#x9;245.76 - 299.42&#xD;&#xA;21 Aug 2027&#x9;&#x9;&#x9;246.86 - 300.52&#xD;&#xA;22 Aug 2027&#x9;&#x9;&#x9;248.02 - 301.68&#xD;&#xA;23 Aug 2027&#x9;&#x9;&#x9;246.09 - 306.09&#xD;&#xA;24 Aug 2027&#x9;&#x9;&#x9;247.42 - 307.42&#xD;&#xA;25 Aug 2027&#x9;&#x9;&#x9;248.83 - 298.83&#xD;&#xA;26 Aug 2027&#x9;&#x9;&#x9;250.35 - 285.35&#xD;&#xA;27 Aug 2027&#x9;&#x9;&#x9;251.98 - 271.98&#xD;&#xA;28 Aug 2027&#x9;&#x9;&#x9;253.72 - 263.72&#xD;&#xA;29 Aug 2027&#x9;&#x9;&#x9;255.60 - 255.60&#xD;&#xA;15 Sep 2027&#x9;&#x9;&#x9;314.91 - 314.91&#xD;&#xA;16 Sep 2027&#x9;&#x9;&#x9;319.28 - 329.28&#xD;&#xA;17 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;18 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;19 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;20 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;21 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;22 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;23 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;24 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;25 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;26 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;27 Sep 2027&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;28 Sep 2027&#x9;&#x9;&#x9;356.59 - 016.59&#xD;&#xA;29 Sep 2027&#x9;&#x9;&#x9;358.48 - 013.48&#xD;&#xA;30 Sep 2027&#x9;&#x9;&#x9;000.25 - 010.25&#xD;&#xA;01 Oct 2027&#x9;&#x9;&#x9;001.89 - 006.89&#xD;&#xA;02 Oct 2027&#x9;&#x9;&#x9;003.43 - 003.43&#xD;&#xA;07 Nov 2027&#x9;&#x9;&#x9;035.52 - 035.52&#xD;&#xA;08 Nov 2027&#x9;&#x9;&#x9;035.83 - 035.83&#xD;&#xA;09 Nov 2027&#x9;&#x9;&#x9;035.24 - 035.24&#xD;&#xA;10 Nov 2027&#x9;&#x9;&#x9;035.54 - 035.54&#xD;&#xA;11 Nov 2027&#x9;&#x9;&#x9;035.84 - 035.84&#xD;&#xA;12 Nov 2027&#x9;&#x9;&#x9;035.15 - 035.15&#xD;&#xA;19 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;20 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;21 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;22 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;23 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;24 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;25 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;26 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;27 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;28 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;29 Feb 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;01 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;02 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;03 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;04 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;05 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;06 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;07 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;08 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;09 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;10 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;11 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;12 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;13 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;14 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;15 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;16 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;17 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;18 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;19 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;20 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;21 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;22 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;23 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;24 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;25 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;26 Mar 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;12 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;13 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;14 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;15 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;16 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;17 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;18 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;19 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;20 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;21 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;22 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;23 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;24 Apr 2028&#x9;&#x9;&#x9;Date not checked.&#xD;&#xA;"
                        Label="Roll Ranges Report"
                        Target="V-R-AQR"
                        Coordinates="RA: 23 43 49.4634,  DEC: -15 17 4.18"
                        Prefix="Orient"
                        Units="U3">
                        
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                           Type="Roll Ranges"
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 :trans-version "20260618"
 :date "24-Jul-2026 12:57:47.0"
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(Tic-Obset
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(Tic-Orbit
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