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<HSTProposal
   Phase1ID="6942"
   Phase2ID="18225"
   Phase="Phase II"
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   <!--Date: Wed Feb 04 22:51:58 GMT 2026-->
   
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            <ErrorText>The current Call for Proposals is for HST Cycle 34.</ErrorText>
            
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            <SubmissionLog>Assigned ID: 6942

----- Attempting Submission 1 (Thu Jan 08 21:08:32 GMT 2026) -----</SubmissionLog>
            
            <DiagnosticJustification>this is an XMM/HST proposal. I was instructed to slect cycle 33</DiagnosticJustification>
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            <SubmissionComments>With respect to the original text in the proposal, we removed the FLATS for defringing because we realized fringes are not an issue in the wavelength covered by these observations.

We slightly increased the exposure time of the MAMA observations, since we realized there was some extra time available in the first orbit.</SubmissionComments>
            
            <SubmissionCommentsCheckSum>447644107</SubmissionCommentsCheckSum>
            
            <SubmissionLog>----- Attempting Submission 1 (Wed Feb 04 22:51:58 GMT 2026) -----</SubmissionLog>
            
            <Phase2DiagnosticJustification>we believe that the warnings can be ignored but please let us know if there are any concerns. Thanks!</Phase2DiagnosticJustification>
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   <ProposalInformation
      Category="GO"
      SnapPriority="Normal Priority"
      PureParallelProposal="false"
      Cycle="33"
      STScIEditNumber="0">
      
      <Title>Do true Seyfert 2 galaxies truly exist ? The case of NGC 3660</Title>
      
      <Abstract>True Seyfert 2 galaxies are active nuclei with no optical/UV/IR broad emission lines that are simultaneously unabsorbed in X-rays and variable, demonstrating a direct view of the inner nucleus. The detection of optical and UV broad lines in the prototypical Seyfert 2 galaxy NGC 3147 in narrow-slit HST spectra has however questioned the very existence of the population as a whole. We propose here a joint XMM-Newton and HST program on one of the best remaining true Seyfert 2 candidates - NGC 3660 - with the goals of (I) searching for a broad, so far undetected, Halpha  emission line using narrow-slit HST spectroscopy, and (II) deriveing a high quality intrinsic nuclear SED using quasi-simultaneous observations. The program has the potential of settling once and for all the debate on the existence of true Seyfert 2 galaxies in general.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Giovanni"
         LastName="Miniutti"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="13280"
         Institution="Centro de Astrobiologia - CAB"
         Country="ESP"
         State="Madrid"
         Contact="true"
         AdminCoI="CoI: Dr. Marco Chiaberge " />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Marco"
         LastName="Chiaberge"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="6163"
         Institution="Space Telescope Science Institute - ESA - JWST"
         Country="USA"
         State="MD"
         Contact="true"
         AdminUSPI="true" />
      
      <CoInvestigator
         Honorific="Prof."
         FirstName="Stefano"
         LastName="Bianchi"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="8807"
         Institution="Universita di Roma Tre"
         Country="ITA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Alessandro"
         LastName="Capetti"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="3088"
         Institution="Osservatorio Astronomico di Torino"
         Country="ITA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Frederic"
         LastName="Marin"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="18558"
         Institution="Universite de Strasbourg I"
         Country="FRA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Ismael"
         LastName="Garcia Bernete"
         ESAMember="true"
         CSAMember="false"
         Retired="false"
         UniqueID="22036"
         Institution="Centro de Astrobiologia - CAB"
         Country="ESP"
         State="Madrid"
         Contact="false"
         AdminUSPI="false" />
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>In order to achieve our goals, we request narrow-slit optical spectra around H|*| using STIS/CCD and the
G750M grating and optical/UV imaging with STIS/NUV-MAMA. We will use the 52x0.1 arcsec slit to
reduce host galaxy contamination by a factor of |*| 10 with respect to ground based observations and to
increase the contrast of any broad line component against both the stellar continuum and the superimposed
narrow lines, which are mostly produced in the extended (kpc-scale) narrow line region (0.1|*| |*| 25 pc at
z = 0.012). We replicate the highly successful strategy that led to the discovery of a broad H|*| in NGC 3147
(right panel of Fig. 1) by our team. The pointing will be aimed at the host galaxy photocenter. A target
acquisition image with the F28X50LP will be taken to allow recentering on the brightest region, where we
expect the AGN to be located, with exposure of 60 s, appropriate for the expected surface brightness of |*|
15 mag arcsec|*|2. To avoid missing the AGN at the center of the galaxy nucleus, we will obtain 5 spectra,
as done for NGC 3147 (GO15225, PI: Bianchi). The first will be centered at the location derived following
the acquisition image. The following will be taken with a POS-TARG of (+0.1,0.0), (+0.2,0.0), (-0.1,0.0),
(-0.2,0.0).
We performed accurate S/N simulations using the STIS ETC. The stellar continuum within the 0.1|*| slit
is expected to be F|*| |*| 2 |*| 10|*|16 erg cm|*|2 s|*|1 |*|A|*|1, using the information derived from ground based
spectra. The resulting S/N is 11 per resolution element. The broad emission line is expected to have a flux
F(H|*|) |*| 1 |*| 10|*|13 erg cm|*|2 s|*|1 and FWHM|*|3000-6000 km s|*|1 (Bianchi et al 2012). Assuming a FWHM
of 5000 km s|*|1, we expect a S/N of 37 at the peak. We use the 52x01E1 aperture to mitigate CTE losses
and two CR-SPLIT images at each slit position to eliminate cosmic rays. As for the SED measurements, we will utilize
the STIS/NUV-MAMA with the F25SFR2 filter, centered at 2320 |*|A to obtain imaging in the UV. Two
dithered exposures will be obtained with a total exposure time of 300 sec, reaching a point source S/N of 17
for a flux of F|*| |*| 1 |*| 10|*|17 erg cm|*|2 s|*|1 |*|A|*|1. The acquisition image will instead provide a measurement of
the AGN continuum at |*| 7000|*|A. Using the HST APT, our program can be completed within 4 HST orbits</ObservingDescription>
         </Phase2Questions>
      </Questions>
      
      <TeamExpertise>N/A</TeamExpertise>
      
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         ThisCycle2GyroPrimary="4" />
      
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      <Phase1ProposalInformation
         LongTermMonitoring="false"
         Attachment="/Users/marcoc/MyDocuments/Science/Miniutti/NGC3660/98108_001_sj.pdf"
         ProposalSize="VERY SMALL">
         
         <ScientificCategory>Supermassive Black Holes and Active Galaxies</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="AGN host galaxies" />
         
         <ScientificKeyword2
            Keyword="Seyfert galaxies" />
         
         <ScientificKeyword3
            Keyword="Supermassive black holes" />
         
         <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>XMM_NEWTON</PrimaryTac>
            
            <PrimaryProposalId>098108</PrimaryProposalId>
         </PrimarySubmission>
         
         <NoDuplicateProposalSubmissions>false</NoDuplicateProposalSubmissions>
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      <Phase2ProposalInformation
         PCFlag="true"
         ProposalSize="SMALL_CYCLE21">
         
         <Availability>SUPPORTED</Availability>
      </Phase2ProposalInformation>
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         Name="NGC-3660"
         Number="1"
         ReferenceFrame="ICRS"
         ICRS="true"
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         RAPMUnits="MAS_PER_YEAR"
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         DecPMUnits="MAS_PER_YEAR"
         PMNotApplicable="false"
         Epoch="2000"
         AnnualParallax="3.23E-4"
         ProvisionalCoordinates="11 23 32.2781 -08 39 30.73">
         
         <PrimaryCategory>GALAXY</PrimaryCategory>
         
         <PrimaryDescription>
            
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            <Description>SEYFERT</Description>
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         <Extended>YES</Extended>
         
         <Comments>This object was generated by the targetselector and retrieved from the SIMBAD database.

SIMBAD listed proper motion for this target. When retrieving targets with PM from SIMBAD, APT requests the coordinates be calculated with an epoch of the year 2000. Do not modify this epoch. Always review coordinates using the Target Confirmation tool, which graphically displays the PM.</Comments>
         
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            <Equinox>J2000</Equinox>
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         <Equinox>J2000</Equinox>
         
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         NumberOfOrbits="4"
         NumberOfIterations="1"
         TotalOrbits="4"
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         CoordinatedParallel="false"
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               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>6581</Wavelength>
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            <Configuration>
               
               <Config>STIS/NUV-MAMA</Config>
               
               <ScienceMode>Imaging</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>F25SRF2</SpectralElement>
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292.02&#xA;18 Nov 2025&#x9;&#x9;&#x9;282.28 - 292.28&#xA;19 Nov 2025&#x9;&#x9;&#x9;282.54 - 292.54&#xA;20 Nov 2025&#x9;&#x9;&#x9;282.80 - 292.80&#xA;21 Nov 2025&#x9;&#x9;&#x9;283.05 - 293.05&#xA;22 Nov 2025&#x9;&#x9;&#x9;283.29 - 293.29&#xA;23 Nov 2025&#x9;&#x9;&#x9;283.54 - 293.54&#xA;24 Nov 2025&#x9;&#x9;&#x9;283.78 - 293.78&#xA;25 Nov 2025&#x9;&#x9;&#x9;284.01 - 294.01&#xA;26 Nov 2025&#x9;&#x9;&#x9;284.24 - 294.24&#xA;27 Nov 2025&#x9;&#x9;&#x9;284.47 - 294.47&#xA;28 Nov 2025&#x9;&#x9;&#x9;284.70 - 294.70&#xA;29 Nov 2025&#x9;&#x9;&#x9;284.93 - 294.93&#xA;30 Nov 2025&#x9;&#x9;&#x9;285.15 - 295.15&#xA;01 Dec 2025&#x9;&#x9;&#x9;285.37 - 295.37&#xA;02 Dec 2025&#x9;&#x9;&#x9;295.59 - 295.59&#xA;03 Dec 2025&#x9;&#x9;&#x9;285.80 - 295.80&#xA;04 Dec 2025&#x9;&#x9;&#x9;286.02 - 296.02&#xA;05 Dec 2025&#x9;&#x9;&#x9;286.23 - 296.23&#xA;06 Dec 2025&#x9;&#x9;&#x9;286.44 - 296.44&#xA;07 Dec 2025&#x9;&#x9;&#x9;286.65 - 296.65&#xA;08 Dec 2025&#x9;&#x9;&#x9;286.86 - 296.86&#xA;09 Dec 2025&#x9;&#x9;&#x9;287.07 - 297.07&#xA;10 Dec 2025&#x9;&#x9;&#x9;287.27 - 297.27&#xA;11 Dec 2025&#x9;&#x9;&#x9;287.48 - 297.48&#xA;12 Dec 2025&#x9;&#x9;&#x9;287.68 - 297.68&#xA;13 Dec 2025&#x9;&#x9;&#x9;287.89 - 297.89&#xA;14 Dec 2025&#x9;&#x9;&#x9;288.09 - 298.09&#xA;15 Dec 2025&#x9;&#x9;&#x9;288.30 - 298.30&#xA;16 Dec 2025&#x9;&#x9;&#x9;288.50 - 298.50&#xA;17 Dec 2025&#x9;&#x9;&#x9;278.71 - 308.71&#xA;18 Dec 2025&#x9;&#x9;&#x9;278.91 - 308.91&#xA;19 Dec 2025&#x9;&#x9;&#x9;279.11 - 309.11&#xA;20 Dec 2025&#x9;&#x9;&#x9;279.32 - 309.32&#xA;21 Dec 2025&#x9;&#x9;&#x9;279.52 - 309.52&#xA;22 Dec 2025&#x9;&#x9;&#x9;279.73 - 309.73&#xA;23 Dec 2025&#x9;&#x9;&#x9;279.94 - 309.94&#xA;24 Dec 2025&#x9;&#x9;&#x9;280.14 - 310.14&#xA;25 Dec 2025&#x9;&#x9;&#x9;280.35 - 310.35&#xA;26 Dec 2025&#x9;&#x9;&#x9;280.56 - 310.56&#xA;27 Dec 2025&#x9;&#x9;&#x9;272.97 - 318.57&#xA;28 Dec 2025&#x9;&#x9;&#x9;273.08 - 298.08&#x9;308.08 - 318.88&#xA;01 Jan 2026&#x9;&#x9;&#x9;273.54 - 273.54&#xA;10 Jan 2026&#x9;&#x9;&#x9;274.32 - 274.32&#xA;11 Jan 2026&#x9;&#x9;&#x9;274.41 - 274.41&#xA;12 Jan 2026&#x9;&#x9;&#x9;274.66 - 284.66&#xA;13 Jan 2026&#x9;&#x9;&#x9;276.05 - 291.05&#xA;14 Jan 2026&#x9;&#x9;&#x9;276.31 - 296.31&#xA;15 Jan 2026&#x9;&#x9;&#x9;276.58 - 301.58&#xA;16 Jan 2026&#x9;&#x9;&#x9;277.83 - 312.83&#xA;17 Jan 2026&#x9;&#x9;&#x9;278.10 - 323.40&#xA;18 Jan 2026&#x9;&#x9;&#x9;278.39 - 323.69&#xA;19 Jan 2026&#x9;&#x9;&#x9;279.57 - 323.07&#xA;20 Jan 2026&#x9;&#x9;&#x9;279.87 - 323.37&#xA;21 Jan 2026&#x9;&#x9;&#x9;280.17 - 323.67&#xA;22 Jan 2026&#x9;&#x9;&#x9;281.26 - 323.20&#xA;23 Jan 2026&#x9;&#x9;&#x9;281.58 - 323.52&#xA;24 Jan 2026&#x9;&#x9;&#x9;281.90 - 323.84&#xA;28 Jan 2026&#x9;&#x9;&#x9;284.62 - 309.62&#xA;29 Jan 2026&#x9;&#x9;&#x9;285.00 - 324.28&#xA;30 Jan 2026&#x9;&#x9;&#x9;285.39 - 324.67&#xA;31 Jan 2026&#x9;&#x9;&#x9;285.79 - 325.07&#xA;01 Feb 2026&#x9;&#x9;&#x9;285.96 - 325.72&#xA;02 Feb 2026&#x9;&#x9;&#x9;286.39 - 326.15&#xA;03 Feb 2026&#x9;&#x9;&#x9;286.83 - 326.59&#xA;04 Feb 2026&#x9;&#x9;&#x9;287.10 - 327.24&#xA;05 Feb 2026&#x9;&#x9;&#x9;287.58 - 327.72&#xA;06 Feb 2026&#x9;&#x9;&#x9;288.08 - 328.22&#xA;07 Feb 2026&#x9;&#x9;&#x9;288.01 - 329.33&#xA;08 Feb 2026&#x9;&#x9;&#x9;288.55 - 329.87&#xA;09 Feb 2026&#x9;&#x9;&#x9;289.11 - 330.43&#xA;10 Feb 2026&#x9;&#x9;&#x9;288.80 - 331.92&#xA;11 Feb 2026&#x9;&#x9;&#x9;289.42 - 332.54&#xA;12 Feb 2026&#x9;&#x9;&#x9;290.07 - 333.19&#xA;13 Feb 2026&#x9;&#x9;&#x9;289.54 - 335.08&#xA;14 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;18 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;19 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;20 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;21 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;22 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;24 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;25 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;26 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;27 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;28 Feb 2026&#x9;&#x9;&#x9;Date not checked.&#xA;01 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;04 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;05 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;06 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;07 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;08 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;09 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;10 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;11 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;12 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;13 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;14 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;18 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;19 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;20 Mar 2026&#x9;&#x9;&#x9;Date not checked.&#xA;21 Mar 2026&#x9;&#x9;&#x9;019.02 - 024.02&#xA;22 Mar 2026&#x9;&#x9;&#x9;022.97 - 022.97&#xA;22 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;24 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;25 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;26 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;27 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;28 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;29 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;30 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;31 Jul 2026&#x9;&#x9;&#x9;Date not checked.&#xA;01 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;02 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;03 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;04 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;05 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;06 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;07 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;10 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;11 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;12 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;13 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;14 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;18 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;19 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;20 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;21 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;22 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;24 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;25 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;26 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;27 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;28 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;29 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;30 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;31 Aug 2026&#x9;&#x9;&#x9;Date not checked.&#xA;01 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;02 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;03 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;04 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;05 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;06 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;07 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;08 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;09 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;10 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;11 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;12 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;13 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;14 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;18 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;19 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;20 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;21 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;22 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;23 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;24 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;25 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;26 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;27 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;28 Sep 2026&#x9;&#x9;&#x9;Date not checked.&#xA;02 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;03 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;04 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;05 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;06 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;07 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;08 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;09 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;10 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;11 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;12 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;13 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;14 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;15 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;16 Oct 2026&#x9;&#x9;&#x9;Date not checked.&#xA;17 Nov 2026&#x9;&#x9;&#x9;281.95 - 291.95&#xA;18 Nov 2026&#x9;&#x9;&#x9;282.22 - 292.22&#xA;19 Nov 2026&#x9;&#x9;&#x9;282.48 - 292.48&#xA;20 Nov 2026&#x9;&#x9;&#x9;282.73 - 292.73&#xA;21 Nov 2026&#x9;&#x9;&#x9;282.98 - 292.98&#xA;24 Nov 2026&#x9;&#x9;&#x9;293.72 - 293.72&#xA;25 Nov 2026&#x9;&#x9;&#x9;283.95 - 293.95&#xA;26 Nov 2026&#x9;&#x9;&#x9;284.19 - 294.19&#xA;27 Nov 2026&#x9;&#x9;&#x9;284.42 - 294.42&#xA;28 Nov 2026&#x9;&#x9;&#x9;284.64 - 294.64&#xA;29 Nov 2026&#x9;&#x9;&#x9;284.87 - 294.87&#xA;30 Nov 2026&#x9;&#x9;&#x9;285.09 - 295.09&#xA;01 Dec 2026&#x9;&#x9;&#x9;285.31 - 295.31&#xA;02 Dec 2026&#x9;&#x9;&#x9;285.53 - 295.53&#xA;03 Dec 2026&#x9;&#x9;&#x9;285.75 - 295.75&#xA;04 Dec 2026&#x9;&#x9;&#x9;285.96 - 295.96&#xA;05 Dec 2026&#x9;&#x9;&#x9;286.17 - 296.17&#xA;06 Dec 2026&#x9;&#x9;&#x9;286.39 - 296.39&#xA;07 Dec 2026&#x9;&#x9;&#x9;286.60 - 296.60&#xA;08 Dec 2026&#x9;&#x9;&#x9;286.81 - 296.81&#xA;09 Dec 2026&#x9;&#x9;&#x9;287.01 - 297.01&#xA;10 Dec 2026&#x9;&#x9;&#x9;287.22 - 297.22&#xA;11 Dec 2026&#x9;&#x9;&#x9;287.43 - 297.43&#xA;12 Dec 2026&#x9;&#x9;&#x9;287.63 - 297.63&#xA;13 Dec 2026&#x9;&#x9;&#x9;287.84 - 297.84&#xA;14 Dec 2026&#x9;&#x9;&#x9;288.04 - 298.04&#xA;15 Dec 2026&#x9;&#x9;&#x9;288.25 - 298.25&#xA;16 Dec 2026&#x9;&#x9;&#x9;288.45 - 298.45&#xA;17 Dec 2026&#x9;&#x9;&#x9;278.65 - 308.65&#xA;18 Dec 2026&#x9;&#x9;&#x9;278.86 - 308.86&#xA;19 Dec 2026&#x9;&#x9;&#x9;279.06 - 309.06&#xA;20 Dec 2026&#x9;&#x9;&#x9;279.27 - 279.27&#x9;299.27 - 309.27&#xA;21 Dec 2026&#x9;&#x9;&#x9;279.47 - 309.47&#xA;22 Dec 2026&#x9;&#x9;&#x9;279.68 - 309.68&#xA;23 Dec 2026&#x9;&#x9;&#x9;279.88 - 309.88&#xA;24 Dec 2026&#x9;&#x9;&#x9;280.09 - 310.09&#xA;25 Dec 2026&#x9;&#x9;&#x9;280.29 - 310.29&#xA;26 Dec 2026&#x9;&#x9;&#x9;280.50 - 310.50&#xA;27 Dec 2026&#x9;&#x9;&#x9;272.91 - 318.51&#xA;28 Dec 2026&#x9;&#x9;&#x9;273.02 - 318.82&#xA;29 Dec 2026&#x9;&#x9;&#x9;273.14 - 319.14&#xA;30 Dec 2026&#x9;&#x9;&#x9;273.35 - 319.35&#xA;31 Dec 2026&#x9;&#x9;&#x9;273.47 - 319.67&#xA;01 Jan 2027&#x9;&#x9;&#x9;273.49 - 320.09&#xA;02 Jan 2027&#x9;&#x9;&#x9;273.61 - 320.41&#xA;03 Jan 2027&#x9;&#x9;&#x9;273.73 - 303.73&#x9;320.73 - 320.73&#xA;04 Jan 2027&#x9;&#x9;&#x9;273.85 - 293.85&#x9;321.05 - 321.05&#xA;05 Jan 2027&#x9;&#x9;&#x9;273.88 - 278.88&#x9;321.48 - 321.48&#xA;06 Jan 2027&#x9;&#x9;&#x9;321.81 - 321.81&#xA;18 Jan 2027&#x9;&#x9;&#x9;288.31 - 288.31&#xA;19 Jan 2027&#x9;&#x9;&#x9;278.60 - 298.60&#xA;20 Jan 2027&#x9;&#x9;&#x9;279.79 - 304.79&#xA;21 Jan 2027&#x9;&#x9;&#x9;280.09 - 315.09&#xA;22 Jan 2027&#x9;&#x9;&#x9;280.40 - 323.90&#xA;23 Jan 2027&#x9;&#x9;&#x9;281.49 - 323.43&#xA;24 Jan 2027&#x9;&#x9;&#x9;281.82 - 323.76&#xA;25 Jan 2027&#x9;&#x9;&#x9;282.15 - 324.09&#xA;26 Jan 2027&#x9;&#x9;&#x9;283.19 - 323.73&#xA;27 Jan 2027&#x9;&#x9;&#x9;283.54 - 324.08&#xA;28 Jan 2027&#x9;&#x9;&#x9;283.90 - 324.44&#xA;29 Jan 2027&#x9;&#x9;&#x9;284.90 - 324.18&#xA;30 Jan 2027&#x9;&#x9;&#x9;285.29 - 324.57&#xA;31 Jan 2027&#x9;&#x9;&#x9;285.68 - 324.96&#xA;01 Feb 2027&#x9;&#x9;&#x9;285.85 - 325.61&#xA;02 Feb 2027&#x9;&#x9;&#x9;286.28 - 326.04&#xA;03 Feb 2027&#x9;&#x9;&#x9;286.72 - 326.48&#xA;04 Feb 2027&#x9;&#x9;&#x9;286.98 - 327.12&#xA;05 Feb 2027&#x9;&#x9;&#x9;287.46 - 327.60&#xA;06 Feb 2027&#x9;&#x9;&#x9;287.95 - 328.09&#xA;07 Feb 2027&#x9;&#x9;&#x9;287.87 - 329.19&#xA;08 Feb 2027&#x9;&#x9;&#x9;288.41 - 329.73&#xA;09 Feb 2027&#x9;&#x9;&#x9;288.97 - 330.29&#xA;10 Feb 2027&#x9;&#x9;&#x9;288.65 - 331.77&#xA;11 Feb 2027&#x9;&#x9;&#x9;289.26 - 289.26&#x9;324.26 - 332.38&#xA;15 Feb 2027&#x9;&#x9;&#x9;290.82 - 336.36&#xA;16 Feb 2027&#x9;&#x9;&#x9;291.61 - 337.15&#xA;17 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;18 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;19 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;20 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;21 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;22 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;23 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;24 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;25 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;26 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;27 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;28 Feb 2027&#x9;&#x9;&#x9;Date not checked.&#xA;01 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;02 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;03 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;04 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;05 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;06 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;09 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;10 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;11 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;12 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;13 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;14 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;15 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;16 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;17 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;18 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;19 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;20 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;21 Mar 2027&#x9;&#x9;&#x9;Date not checked.&#xA;22 Mar 2027&#x9;&#x9;&#x9;021.98 - 031.98&#xA;23 Mar 2027&#x9;&#x9;&#x9;025.73 - 030.73&#xA;24 Mar 2027&#x9;&#x9;&#x9;029.20 - 029.20&#xA;"
                        Label="Roll Ranges Report"
                        Target="NGC-3660"
                        Coordinates="RA: 11 23 32.2781,  DEC: -08 39 30.73"
                        Prefix="Orient"
                        Units="U3">
                        
                        <StConstraintSchedulingWindows
                           Name="Roll Report Data"
                           Type="Roll Ranges"
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         IsActive="true" />
      
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</HSTProposal>
