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            <SubmissionLog>Assigned ID: 6916

----- Attempting Submission 1 (Wed Aug 27 23:13:44 GMT 2025) -----
HST Phase I Proposal 6916  successfully submitted.
Receipt: # 6916-1</SubmissionLog>
            
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            <SubmissionLog>----- Attempting Submission 1 (Tue Sep 09 22:20:17 GMT 2025) -----
HST Phase II Proposal 18192  successfully submitted.
Receipt: # 18192-1

----- Attempting Submission 2 (Wed Dec 03 00:32:27 GMT 2025) -----</SubmissionLog>
            
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      Category="GO"
      SnapPriority="Normal Priority"
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      Cycle="33"
      STScIEditNumber="0">
      
      <Title>Dual Fe Ka peaks in MCG-03-34-64 - a close merger pair in the local Universe?</Title>
      
      <Abstract>ACIS imaging of the nearby Seyfert MCG-03-34-64 has revealed two spatially-resolved peaks of luminous
Fe Ka line emission, coincident with radio peaks, comprising a candidate dual AGN. If confirmed, this
merger pair - at a separation of just 100 pc - would be the closest dual nuclei detected in multi waveband
analysis to date. Establishment of close nuclear pairs offers critical model constraints for galaxy/AGN
co-evolution. However, a single nucleus plus shocked gas provides an alternative model for the data. We
request 200 ks of ACIS-S time (4x the existing exposure), supported by 2 orbits of HST STIS, to confirm
the statistical significance and origin of the Fe Ka peaks and confidently parameterize this important system.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="T."
         MiddleInitial="Jane"
         LastName="Turner"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="4739"
         Institution="Eureka Scientific Inc."
         Country="USA"
         State="CA"
         Contact="true" />
      
      <CoInvestigator
         FirstName="Steven"
         MiddleInitial="B."
         LastName="Kraemer"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="19372"
         Institution="Catholic University of America"
         Country="USA"
         State="DC"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="James"
         MiddleInitial="N."
         LastName="Reeves"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="13742"
         Institution="Catholic University of America"
         Country="USA"
         State="DC"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Valentina"
         LastName="Braito"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="9137"
         Institution="Catholic University of America"
         Country="USA"
         State="DC"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Anna"
         LastName="Trindade Falcao"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="20812"
         Institution="NASA Goddard Space Flight Center / ORAU"
         Country="USA"
         State="MD"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Henrique"
         MiddleInitial="R."
         LastName="Schmitt"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="2977"
         Institution="Naval Research Laboratory"
         Country="USA"
         State="DC"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Lea"
         MiddleInitial="Marie"
         LastName="Feuillet"
         ESAMember="false"
         CSAMember="false"
         Retired="false"
         UniqueID="45969"
         Institution="Catholic University of America"
         Country="USA"
         State="DC"
         Contact="false"
         AdminUSPI="false" />
      
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            <ObservingDescription>In order to map the spatially-resolved kinematics of the NLR emission-line gas, we request a STIS G430M
spectrum of [O III] 5007|*| through the 0:200 - 5200 slit. With this, we will achieve a velocity resolution
of |*| 60 km/, which is ideal for separating distinct kinematic components and measuring accurate velocity
dispersions for each component. The slit will be oriented to cover the bright knots of [O III] present
in the archival ACS narrow-band image, with a |*|20 deg tolerance. Based on the [OIII] image, the peak
[OIII] fluxes are similar corresponding to a surface brightness of 2|*|10|*|13 erg s|*|1 cm|*|2 arcsec|*|2, while the
wings have surface brightness 5|*|10|*|14 erg s|*|1 cm|*|2 arcsec|*|2 and the fainter regions have surface brightness
3|*|10|*|15 erg s|*|1 cm|*|2 arcsec|*|2. Using the STIS ETC, and the NGC 1068 spectrum (to represent a Seyfert
2) normalized to the [O III] line with an integration of 40 minutes and the 0:200 |*| 5200 slit, we will achieve a
SNR = 75, 33, 3.5 for the 3 regions defined by the 3 [O III] knots. Therefore, we require one orbit for the
G430M spectrum.
In order to constrain the ionization mechanisms for the optical emission-line gas, we request a G430L
spectrum with the same slit and orientation used for the G430M. We base our exposure request on the need
to obtain useful S/N for [Ne V] 3426|*|, which, based on the archival ESO-VLT X-Shooter spectra, has a
flux 10% that of the integrated [O III] emission, corresponding to a surface brightness of |*| 4 |*| 10|*|13 erg
s|*|1 cm|*|2 arcsec|*|2. Using the ETC, we determine that in a 40 minute exposure we will obtain a SNR |*| 7.5
at the average surface brightness, and SNR |*| 3 at 1:5 |*| 10|*|13 erg s|*|1 cm|*|2 arcsec|*|2. The [O II] 3727|*| ,
[Ne III] 3869|*| , and [O III] 5007 |*| lines are all su|*|ciently bright to map the ionization structure of the
NLR with the proposed data, at a slightly lower S/N than that detailed for [O III], above. We require one
orbit for the G430L spectrum. For each spectrum, we will obtain three sub exposures at slightly di|*|erent
positions along the slit to facilitate the removal of cosmic rays and hot pixels on the CCD images. We will
obtain these exposures near the top of the chip (the E1 position) to minimize CTE loss.</ObservingDescription>
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      <TeamExpertise>Our team have extensive experience in the analysis, interpretation and publication of X-ray spectral data (Turner,Reeves, Braito, Trindade Falcao) and UV and optical data (Kraemer, Schmitt, Trindade Falcao, Feullit) and radio data (Schmitt, Feullit). The PI has authored 200 publications in refereed journals.

For the proposed project we will use publicly available models with  ftools, CIAO and XSPEC  software for the data analysis. 

All co-investigators will be involved in the interpretation and publication of the results.</TeamExpertise>
      
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         <ScientificCategory>Supermassive Black Holes and Active Galaxies</ScientificCategory>
         
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         <ScientificKeyword2
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         <NoDuplicateProposalSubmissions>true</NoDuplicateProposalSubmissions>
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322.26&#xA;09 Mar 2026&#x9;&#x9;&#x9;281.28 - 322.60&#xA;10 Mar 2026&#x9;&#x9;&#x9;281.64 - 322.96&#xA;11 Mar 2026&#x9;&#x9;&#x9;281.12 - 324.24&#xA;12 Mar 2026&#x9;&#x9;&#x9;281.52 - 324.64&#xA;13 Mar 2026&#x9;&#x9;&#x9;281.93 - 325.05&#xA;14 Mar 2026&#x9;&#x9;&#x9;281.16 - 326.70&#xA;15 Mar 2026&#x9;&#x9;&#x9;281.62 - 327.16&#xA;16 Mar 2026&#x9;&#x9;&#x9;282.11 - 327.65&#xA;17 Mar 2026&#x9;&#x9;&#x9;280.94 - 329.84&#xA;18 Mar 2026&#x9;&#x9;&#x9;281.49 - 330.39&#xA;19 Mar 2026&#x9;&#x9;&#x9;282.07 - 330.97&#xA;20 Mar 2026&#x9;&#x9;&#x9;280.31 - 333.97&#xA;21 Mar 2026&#x9;&#x9;&#x9;280.97 - 334.63&#xA;22 Mar 2026&#x9;&#x9;&#x9;281.67 - 301.67&#x9;331.67 - 335.33&#xA;25 Mar 2026&#x9;&#x9;&#x9;290.95 - 295.95&#xA;26 Mar 2026&#x9;&#x9;&#x9;281.90 - 341.90&#xA;27 Mar 2026&#x9;&#x9;&#x9;282.94 - 342.94&#xA;28 Mar 2026&#x9;&#x9;&#x9;284.07 - 344.07&#xA;29 Mar 2026&#x9;&#x9;&#x9;285.30 - 345.30&#xA;30 Mar 2026&#x9;&#x9;&#x9;286.66 - 346.66&#xA;31 Mar 2026&#x9;&#x9;&#x9;288.16 - 343.16&#xA;01 Apr 2026&#x9;&#x9;&#x9;289.81 - 344.81&#xA;02 Apr 2026&#x9;&#x9;&#x9;291.66 - 341.66&#xA;03 Apr 2026&#x9;&#x9;&#x9;293.72 - 338.72&#xA;04 Apr 2026&#x9;&#x9;&#x9;296.03 - 336.03&#xA;05 Apr 2026&#x9;&#x9;&#x9;298.64 - 338.64&#xA;06 Apr 2026&#x9;&#x9;&#x9;301.60 - 326.60&#xA;07 Apr 2026&#x9;&#x9;&#x9;304.95 - 304.95&#xA;18 Dec 2026&#x9;&#x9;&#x9;282.92 - 292.92&#xA;19 Dec 2026&#x9;&#x9;&#x9;283.09 - 293.09&#xA;20 Dec 2026&#x9;&#x9;&#x9;283.26 - 293.26&#xA;21 Dec 2026&#x9;&#x9;&#x9;283.42 - 293.42&#xA;22 Dec 2026&#x9;&#x9;&#x9;283.58 - 283.58&#xA;23 Dec 2026&#x9;&#x9;&#x9;283.74 - 288.74&#xA;24 Dec 2026&#x9;&#x9;&#x9;283.90 - 293.90&#xA;25 Dec 2026&#x9;&#x9;&#x9;284.05 - 294.05&#xA;26 Dec 2026&#x9;&#x9;&#x9;284.21 - 294.21&#xA;27 Dec 2026&#x9;&#x9;&#x9;284.36 - 294.36&#xA;28 Dec 2026&#x9;&#x9;&#x9;284.51 - 294.51&#xA;29 Dec 2026&#x9;&#x9;&#x9;284.65 - 294.65&#xA;30 Dec 2026&#x9;&#x9;&#x9;284.80 - 294.80&#xA;11 Jan 2027&#x9;&#x9;&#x9;286.45 - 291.45&#xA;12 Jan 2027&#x9;&#x9;&#x9;286.58 - 296.58&#xA;13 Jan 2027&#x9;&#x9;&#x9;286.72 - 296.72&#xA;14 Jan 2027&#x9;&#x9;&#x9;286.85 - 296.85&#xA;15 Jan 2027&#x9;&#x9;&#x9;286.98 - 296.98&#xA;16 Jan 2027&#x9;&#x9;&#x9;277.12 - 307.12&#xA;17 Jan 2027&#x9;&#x9;&#x9;277.25 - 307.25&#xA;18 Jan 2027&#x9;&#x9;&#x9;277.38 - 282.38&#x9;297.38 - 307.38&#xA;19 Jan 2027&#x9;&#x9;&#x9;277.51 - 307.51&#xA;20 Jan 2027&#x9;&#x9;&#x9;277.65 - 307.65&#xA;21 Jan 2027&#x9;&#x9;&#x9;277.78 - 307.78&#xA;22 Jan 2027&#x9;&#x9;&#x9;277.91 - 307.91&#xA;23 Jan 2027&#x9;&#x9;&#x9;278.05 - 308.05&#xA;24 Jan 2027&#x9;&#x9;&#x9;278.18 - 308.18&#xA;25 Jan 2027&#x9;&#x9;&#x9;278.32 - 308.32&#xA;26 Jan 2027&#x9;&#x9;&#x9;270.65 - 316.25&#xA;27 Jan 2027&#x9;&#x9;&#x9;270.69 - 316.49&#xA;28 Jan 2027&#x9;&#x9;&#x9;270.73 - 316.73&#xA;29 Jan 2027&#x9;&#x9;&#x9;270.87 - 316.87&#xA;30 Jan 2027&#x9;&#x9;&#x9;270.91 - 317.11&#xA;31 Jan 2027&#x9;&#x9;&#x9;270.85 - 317.45&#xA;01 Feb 2027&#x9;&#x9;&#x9;270.89 - 317.69&#xA;02 Feb 2027&#x9;&#x9;&#x9;270.94 - 317.94&#xA;03 Feb 2027&#x9;&#x9;&#x9;270.98 - 318.18&#xA;04 Feb 2027&#x9;&#x9;&#x9;270.93 - 318.53&#xA;05 Feb 2027&#x9;&#x9;&#x9;270.98 - 318.78&#xA;06 Feb 2027&#x9;&#x9;&#x9;270.93 - 319.13&#xA;07 Feb 2027&#x9;&#x9;&#x9;270.99 - 319.39&#xA;08 Feb 2027&#x9;&#x9;&#x9;270.94 - 319.74&#xA;09 Feb 2027&#x9;&#x9;&#x9;270.90 - 320.10&#xA;10 Feb 2027&#x9;&#x9;&#x9;270.90 - 320.42&#xA;11 Feb 2027&#x9;&#x9;&#x9;271.06 - 320.58&#xA;12 Feb 2027&#x9;&#x9;&#x9;272.36 - 319.62&#xA;13 Feb 2027&#x9;&#x9;&#x9;272.53 - 319.79&#xA;17 Feb 2027&#x9;&#x9;&#x9;274.22 - 319.52&#xA;18 Feb 2027&#x9;&#x9;&#x9;275.31 - 305.31&#xA;19 Feb 2027&#x9;&#x9;&#x9;275.50 - 290.50&#x9;319.00 - 319.00&#xA;20 Feb 2027&#x9;&#x9;&#x9;275.69 - 285.69&#x9;319.19 - 319.19&#xA;21 Feb 2027&#x9;&#x9;&#x9;276.67 - 276.67&#x9;316.67 - 318.61&#xA;22 Feb 2027&#x9;&#x9;&#x9;318.82 - 318.82&#xA;06 Mar 2027&#x9;&#x9;&#x9;280.80 - 280.80&#xA;07 Mar 2027&#x9;&#x9;&#x9;281.11 - 291.11&#xA;08 Mar 2027&#x9;&#x9;&#x9;280.85 - 295.85&#xA;09 Mar 2027&#x9;&#x9;&#x9;281.19 - 301.19&#xA;10 Mar 2027&#x9;&#x9;&#x9;281.55 - 306.55&#xA;11 Mar 2027&#x9;&#x9;&#x9;281.02 - 316.02&#xA;12 Mar 2027&#x9;&#x9;&#x9;281.41 - 324.53&#xA;13 Mar 2027&#x9;&#x9;&#x9;281.82 - 281.82&#xA;14 Mar 2027&#x9;&#x9;&#x9;281.05 - 281.05&#xA;16 Mar 2027&#x9;&#x9;&#x9;281.98 - 301.98&#xA;17 Mar 2027&#x9;&#x9;&#x9;280.81 - 329.71&#xA;18 Mar 2027&#x9;&#x9;&#x9;281.35 - 330.25&#xA;19 Mar 2027&#x9;&#x9;&#x9;281.92 - 330.82&#xA;20 Mar 2027&#x9;&#x9;&#x9;280.14 - 333.80&#xA;21 Mar 2027&#x9;&#x9;&#x9;280.79 - 334.45&#xA;22 Mar 2027&#x9;&#x9;&#x9;281.49 - 335.15&#xA;23 Mar 2027&#x9;&#x9;&#x9;282.23 - 335.89&#xA;24 Mar 2027&#x9;&#x9;&#x9;279.86 - 339.86&#xA;25 Mar 2027&#x9;&#x9;&#x9;280.72 - 340.72&#xA;26 Mar 2027&#x9;&#x9;&#x9;281.65 - 341.65&#xA;27 Mar 2027&#x9;&#x9;&#x9;282.67 - 342.67&#xA;28 Mar 2027&#x9;&#x9;&#x9;283.77 - 343.77&#xA;29 Mar 2027&#x9;&#x9;&#x9;284.97 - 344.97&#xA;30 Mar 2027&#x9;&#x9;&#x9;286.30 - 346.30&#xA;31 Mar 2027&#x9;&#x9;&#x9;287.76 - 347.76&#xA;01 Apr 2027&#x9;&#x9;&#x9;289.37 - 349.37&#xA;02 Apr 2027&#x9;&#x9;&#x9;291.17 - 351.17&#xA;03 Apr 2027&#x9;&#x9;&#x9;293.17 - 348.17&#xA;04 Apr 2027&#x9;&#x9;&#x9;295.41 - 345.41&#xA;05 Apr 2027&#x9;&#x9;&#x9;297.94 - 342.94&#xA;06 Apr 2027&#x9;&#x9;&#x9;300.80 - 340.80&#xA;07 Apr 2027&#x9;&#x9;&#x9;304.05 - 339.05&#xA;08 Apr 2027&#x9;&#x9;&#x9;307.74 - 337.74&#xA;"
                        Label="Roll Ranges Report"
                        Target="MCG-03-34-064"
                        Coordinates="RA: 13 22 24.4583,  DEC: -16 43 42.48"
                        Prefix="Orient"
                        Units="U3">
                        
                        <StConstraintSchedulingWindows
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1807049872729 1.0 300.8:340.8 1807136272729 1.0 304.05:339.05 1807222672729 1.0 307.74:337.74 1807228800000 0.0 1807228800001" />
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 :date "09-Sep-2025 18:10:23.0"
 :trans-errors '(:WARNINGS 0 :ERRORS 0 :HEALTH-AND-SAFETY 0
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 :proposal-id 18192
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 :orbit-number 2
 :pcs-time 380
 :si-vis-utilization 2425
 :al-overhead-at-end 0
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 :max-dark-utilization 1920
 :low-sky "N"
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