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<HSTProposal
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            <SubmissionLog>Assigned ID: 2656

----- Attempting Submission 1 (Thu Jan 27 19:48:01 GMT 2022) -----
HST Phase I Proposal 2656  successfully submitted.
Receipt: # 2656-1

----- Attempting Submission 2 (Mon Jan 31 14:44:27 GMT 2022) -----</SubmissionLog>
            
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----- Attempting Submission 2 (Mon Apr 18 14:52:34 GMT 2022) -----
HST Phase II Proposal 16921  successfully submitted.
Receipt: # 16921-2

----- Attempting Submission 3 (Wed May 18 17:54:48 GMT 2022) -----

----- Attempting Submission 4 (Fri Jul 08 20:52:43 GMT 2022) -----</SubmissionLog>
            
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      <Title>Enabling a First in a Lifetime Multi-Wavelength Gas and Dust Coma Characterization of the Centaur 39P/Oterma</Title>
      
      <Abstract>Centaurs are the dynamical intermediary between the more distant and thermally pristine Trans-Neptunian Objects (TNOs) with the more processed and active Jupiter-Family Comets (JFCs). In the Centaur region between Neptune and Jupiter the thermal activation of many cosmogonically abundant volatile species occurs driving comae activity. Investigations of these distant comae provide salient data to test models of the solar system's formation. To date thorough Centaur gas comae characterizations are prohibitive due to instrumental sensitivity limitations, however the newly launched James Webb Space Telescope (JWST) will provide the sensitivities necessary to probe Centaur gas comae. Six Centaurs have been approved for JWST Cycle 1 gas comae characterizations [McKay et al. 2021] with additional contemporaneously acquired dust comae observations from other observatories. Of the six JWST Centaur targets 39P/Oterma is predicted to be beyond suitable characterization through ground-based assets during the Cycle 1 NIRSpec observations. We request 2 HST orbits during Cycle 29 (Jul. - Aug. 2022) of WFC3-UVIS imaging to contemporaneously characterize the dust coma of the Centaur 39P/Oterma during scheduled Cycle 1 JWST NIRSpec gas coma characterization. The tight, stable, and well characterized WFC3 PSF in combination with HST's sensitivity to low surface brightness provide the only observational platform currently available to detect and isolate the flux from 39P's dust coma from its nucleus contribution. If a suitable ramp up of comae activity occurs before the scheduled JWST observations we will forgo the HST observations, instead utilizing ground-based assets.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Charles"
         LastName="Schambeau"
         ESAMember="false"
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         Retired="false"
         UniqueID="17643"
         Institution="University of Central Florida Board of Trustees"
         Country="USA"
         State="FL"
         Contact="true" />
      
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         Honorific="Dr."
         FirstName="Adam"
         LastName="McKay"
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         UniqueID="17898"
         Institution="American University"
         Country="USA"
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      <CoInvestigator
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         FirstName="Eva"
         LastName="Lilly"
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         Retired="false"
         UniqueID="39206"
         Institution="Planetary Science Institute"
         Country="USA"
         State="AZ"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Yanga"
         LastName="Fernandez"
         ESAMember="false"
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         Retired="false"
         UniqueID="6718"
         Institution="University of Central Florida Board of Trustees"
         Country="USA"
         State="FL"
         Contact="false"
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      <CoInvestigator
         FirstName="Olga"
         LastName="Harrington Pinto"
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         Institution="University of Central Florida Board of Trustees"
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         MiddleInitial="Richard"
         LastName="Kareta"
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         UniqueID="41561"
         Institution="Lowell Observatory"
         Country="USA"
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            <ObservingDescription>We will use two orbits of HST/WFC3 to observe the active Centaur 39P/Oterma's dust coma color and morphology to complement its Cycle 1 JWST NIRSpec IFU Prism gas coma characterization. Due to the variable nature of comae activities it is important to schedule the HST observations as close as possible to the JWST observations to ensure a direct comparison of the time variable coma environment. We will acquire imaging data in WFC3-UVIS in the F475W (SDSS g), F625W (SDSS r), and F775W (SDSS i) filters in order to compare to ensemble studies of comes and Centaurs that commonly use the SDSS gri or BVRI systems. The ephemeris uncertainty of 39P is low (approximately 1 arcsecond) so we choose to use the UVIS-M1K1C-SUB subarray (40 arcsecond FOV) to allow more images to be acquired before buffer dumps. 

The coma surface brightness during the JWST and HST observations is not know a priori so we base out exposure times to achieve a S/N of &gt; 50 for each of the filters. A total integration of g (20 minutes), r (15 minutes) and i (23 minutes) is planned to achieve the desired S/N. The telescope will be dithered between individual exposures to mitigate effects of bad pixels and for the removal of cosmic rays. The detector pixels will not be binned retaining the native 0.04 arcseconds per pixel resolution.</ObservingDescription>
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      <TeamExpertise>Dr. Charles Schambeau has expertise in HST data reduction for the WFC3-UVIS instrument. He is an expert in analyzing broadband imaging of cometary and Centaur comae and the modeling effort of our program. He has 4 papers published in the past 6 years related to this research. Dr. Adam McKay is the PI of the JWST program and will perform the NIRSpec spectral analysis for gas comae measurements. Additionally, Dr. Eva Lilly (Schunova), Dr. Teddy Kareta, Ms. Olga Harrington-Pinto, and Dr. Yanga Fernandez are experts in the analysis and interpretation of comet and Centaur comae and their activation mechanisms.</TeamExpertise>
      
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         <ScientificCategory>Solar System Astronomy</ScientificCategory>
         
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266.27&#xA;05 Sep 2022&#x9;&#x9;&#x9;224.86 - 266.18&#xA;06 Sep 2022&#x9;&#x9;&#x9;224.75 - 266.07&#xA;07 Sep 2022&#x9;&#x9;&#x9;223.74 - 266.86&#xA;08 Sep 2022&#x9;&#x9;&#x9;223.63 - 266.75&#xA;09 Sep 2022&#x9;&#x9;&#x9;223.51 - 266.63&#xA;10 Sep 2022&#x9;&#x9;&#x9;222.17 - 267.71&#xA;11 Sep 2022&#x9;&#x9;&#x9;222.03 - 267.57&#xA;12 Sep 2022&#x9;&#x9;&#x9;220.21 - 269.11&#xA;13 Sep 2022&#x9;&#x9;&#x9;220.06 - 268.96&#xA;14 Sep 2022&#x9;&#x9;&#x9;219.89 - 268.79&#xA;15 Sep 2022&#x9;&#x9;&#x9;217.34 - 271.00&#xA;16 Sep 2022&#x9;&#x9;&#x9;217.15 - 270.81&#xA;17 Sep 2022&#x9;&#x9;&#x9;216.95 - 270.61&#xA;18 Sep 2022&#x9;&#x9;&#x9;213.56 - 273.56&#xA;19 Sep 2022&#x9;&#x9;&#x9;213.32 - 273.32&#xA;20 Sep 2022&#x9;&#x9;&#x9;213.06 - 273.06&#xA;21 Sep 2022&#x9;&#x9;&#x9;212.77 - 272.77&#xA;22 Sep 2022&#x9;&#x9;&#x9;212.46 - 272.46&#xA;23 Sep 2022&#x9;&#x9;&#x9;212.11 - 272.11&#xA;24 Sep 2022&#x9;&#x9;&#x9;211.72 - 271.72&#xA;25 Sep 2022&#x9;&#x9;&#x9;211.28 - 271.28&#xA;26 Sep 2022&#x9;&#x9;&#x9;210.77 - 270.77&#xA;27 Sep 2022&#x9;&#x9;&#x9;210.20 - 270.20&#xA;28 Sep 2022&#x9;&#x9;&#x9;209.53 - 211.53&#x9;227.53 - 269.53&#xA;29 Sep 2022&#x9;&#x9;&#x9;230.75 - 268.75&#xA;30 Sep 2022&#x9;&#x9;&#x9;232.81 - 267.81&#xA;01 Oct 2022&#x9;&#x9;&#x9;206.66 - 266.66&#xA;02 Oct 2022&#x9;&#x9;&#x9;205.24 - 265.24&#xA;03 Oct 2022&#x9;&#x9;&#x9;203.41 - 263.41&#xA;04 Oct 2022&#x9;&#x9;&#x9;200.98 - 260.98&#xA;05 Oct 2022&#x9;&#x9;&#x9;197.61 - 257.61&#xA;06 Oct 2022&#x9;&#x9;&#x9;192.65 - 252.65&#xA;07 Oct 2022&#x9;&#x9;&#x9;184.79 - 215.79&#x9;233.79 - 244.79&#xA;09 Oct 2022&#x9;&#x9;&#x9;230.00 - 138.00&#xA;10 Oct 2022&#x9;&#x9;&#x9;227.00 - 130.00&#xA;11 Oct 2022&#x9;&#x9;&#x9;087.20 - 124.20&#xA;12 Oct 2022&#x9;&#x9;&#x9;072.04 - 120.04&#xA;13 Oct 2022&#x9;&#x9;&#x9;063.38 - 116.38&#xA;14 Oct 2022&#x9;&#x9;&#x9;058.01 - 114.01&#xA;15 Oct 2022&#x9;&#x9;&#x9;054.41 - 114.41&#xA;16 Oct 2022&#x9;&#x9;&#x9;051.83 - 111.83&#xA;17 Oct 2022&#x9;&#x9;&#x9;049.91 - 109.91&#xA;18 Oct 2022&#x9;&#x9;&#x9;048.42 - 074.42&#x9;106.42 - 108.42&#xA;19 Oct 2022&#x9;&#x9;&#x9;047.23 - 065.23&#xA;20 Oct 2022&#x9;&#x9;&#x9;046.26 - 068.26&#x9;106.26 - 106.26&#xA;21 Oct 2022&#x9;&#x9;&#x9;045.46 - 105.46&#xA;22 Oct 2022&#x9;&#x9;&#x9;044.77 - 104.77&#xA;23 Oct 2022&#x9;&#x9;&#x9;044.19 - 104.19&#xA;24 Oct 2022&#x9;&#x9;&#x9;043.68 - 103.68&#xA;25 Oct 2022&#x9;&#x9;&#x9;043.23 - 103.23&#xA;26 Oct 2022&#x9;&#x9;&#x9;042.83 - 102.83&#xA;27 Oct 2022&#x9;&#x9;&#x9;042.48 - 102.48&#xA;28 Oct 2022&#x9;&#x9;&#x9;042.16 - 102.16&#xA;29 Oct 2022&#x9;&#x9;&#x9;041.87 - 101.87&#xA;30 Oct 2022&#x9;&#x9;&#x9;041.61 - 101.61&#xA;31 Oct 2022&#x9;&#x9;&#x9;041.37 - 101.37&#xA;01 Nov 2022&#x9;&#x9;&#x9;044.32 - 097.98&#xA;02 Nov 2022&#x9;&#x9;&#x9;044.11 - 097.77&#xA;03 Nov 2022&#x9;&#x9;&#x9;043.93 - 097.59&#xA;04 Nov 2022&#x9;&#x9;&#x9;046.13 - 095.03&#xA;05 Nov 2022&#x9;&#x9;&#x9;045.97 - 094.87&#xA;06 Nov 2022&#x9;&#x9;&#x9;047.50 - 093.04&#xA;07 Nov 2022&#x9;&#x9;&#x9;047.35 - 092.89&#xA;08 Nov 2022&#x9;&#x9;&#x9;047.22 - 092.76&#xA;09 Nov 2022&#x9;&#x9;&#x9;048.30 - 091.42&#xA;10 Nov 2022&#x9;&#x9;&#x9;048.18 - 091.30&#xA;11 Nov 2022&#x9;&#x9;&#x9;048.07 - 091.19&#xA;12 Nov 2022&#x9;&#x9;&#x9;048.86 - 090.18&#xA;13 Nov 2022&#x9;&#x9;&#x9;048.76 - 090.08&#xA;14 Nov 2022&#x9;&#x9;&#x9;048.67 - 076.67&#xA;15 Nov 2022&#x9;&#x9;&#x9;052.16 - 066.16&#xA;16 Nov 2022&#x9;&#x9;&#x9;049.07 - 066.07&#xA;17 Nov 2022&#x9;&#x9;&#x9;048.99 - 089.13&#xA;18 Nov 2022&#x9;&#x9;&#x9;049.10 - 088.86&#xA;19 Nov 2022&#x9;&#x9;&#x9;049.03 - 088.79&#xA;20 Nov 2022&#x9;&#x9;&#x9;049.19 - 088.47&#xA;21 Nov 2022&#x9;&#x9;&#x9;049.12 - 088.40&#xA;22 Nov 2022&#x9;&#x9;&#x9;049.05 - 088.33&#xA;23 Nov 2022&#x9;&#x9;&#x9;048.36 - 088.90&#xA;24 Nov 2022&#x9;&#x9;&#x9;048.29 - 088.83&#xA;25 Nov 2022&#x9;&#x9;&#x9;048.23 - 088.77&#xA;26 Nov 2022&#x9;&#x9;&#x9;047.47 - 089.41&#xA;27 Nov 2022&#x9;&#x9;&#x9;047.42 - 089.36&#xA;28 Nov 2022&#x9;&#x9;&#x9;047.36 - 089.30&#xA;29 Nov 2022&#x9;&#x9;&#x9;046.53 - 090.03&#xA;30 Nov 2022&#x9;&#x9;&#x9;046.48 - 089.98&#xA;01 Dec 2022&#x9;&#x9;&#x9;046.43 - 089.93&#xA;02 Dec 2022&#x9;&#x9;&#x9;045.48 - 090.78&#xA;03 Dec 2022&#x9;&#x9;&#x9;045.44 - 090.74&#xA;04 Dec 2022&#x9;&#x9;&#x9;045.39 - 090.69&#xA;05 Dec 2022&#x9;&#x9;&#x9;044.37 - 091.63&#xA;06 Dec 2022&#x9;&#x9;&#x9;044.33 - 091.59&#xA;07 Dec 2022&#x9;&#x9;&#x9;044.29 - 091.55&#xA;08 Dec 2022&#x9;&#x9;&#x9;043.12 - 092.64&#xA;09 Dec 2022&#x9;&#x9;&#x9;043.08 - 092.60&#xA;10 Dec 2022&#x9;&#x9;&#x9;043.20 - 092.40&#xA;11 Dec 2022&#x9;&#x9;&#x9;043.37 - 084.37&#xA;12 Dec 2022&#x9;&#x9;&#x9;043.53 - 067.53&#xA;13 Dec 2022&#x9;&#x9;&#x9;043.60 - 064.60&#xA;14 Dec 2022&#x9;&#x9;&#x9;043.76 - 091.56&#xA;15 Dec 2022&#x9;&#x9;&#x9;043.83 - 091.43&#xA;16 Dec 2022&#x9;&#x9;&#x9;044.00 - 091.20&#xA;17 Dec 2022&#x9;&#x9;&#x9;044.07 - 091.07&#xA;18 Dec 2022&#x9;&#x9;&#x9;044.14 - 090.94&#xA;19 Dec 2022&#x9;&#x9;&#x9;044.21 - 090.81&#xA;20 Dec 2022&#x9;&#x9;&#x9;044.38 - 090.58&#xA;21 Dec 2022&#x9;&#x9;&#x9;044.46 - 090.46&#xA;22 Dec 2022&#x9;&#x9;&#x9;044.43 - 090.43&#xA;23 Dec 2022&#x9;&#x9;&#x9;044.50 - 090.30&#xA;24 Dec 2022&#x9;&#x9;&#x9;044.58 - 090.18&#xA;25 Dec 2022&#x9;&#x9;&#x9;044.65 - 090.05&#xA;26 Dec 2022&#x9;&#x9;&#x9;044.64 - 090.02&#xA;27 Dec 2022&#x9;&#x9;&#x9;044.71 - 089.91&#xA;28 Dec 2022&#x9;&#x9;&#x9;044.68 - 089.88&#xA;29 Dec 2022&#x9;&#x9;&#x9;044.76 - 089.76&#xA;30 Dec 2022&#x9;&#x9;&#x9;044.74 - 089.74&#xA;31 Dec 2022&#x9;&#x9;&#x9;044.72 - 089.72&#xA;01 Jan 2023&#x9;&#x9;&#x9;044.70 - 089.70&#xA;02 Jan 2023&#x9;&#x9;&#x9;044.68 - 089.68&#xA;03 Jan 2023&#x9;&#x9;&#x9;044.76 - 089.56&#xA;04 Jan 2023&#x9;&#x9;&#x9;062.14 - 072.14&#xA;05 Jan 2023&#x9;&#x9;&#x9;062.12 - 072.12&#xA;06 Jan 2023&#x9;&#x9;&#x9;062.10 - 072.10&#xA;07 Jan 2023&#x9;&#x9;&#x9;062.09 - 072.09&#xA;08 Jan 2023&#x9;&#x9;&#x9;062.07 - 071.07&#xA;09 Jan 2023&#x9;&#x9;&#x9;062.06 - 065.06&#xA;10 Jan 2023&#x9;&#x9;&#x9;062.04 - 071.04&#xA;11 Jan 2023&#x9;&#x9;&#x9;062.02 - 072.02&#xA;12 Jan 2023&#x9;&#x9;&#x9;062.01 - 072.01&#xA;13 Jan 2023&#x9;&#x9;&#x9;061.99 - 071.99&#xA;14 Jan 2023&#x9;&#x9;&#x9;061.98 - 071.98&#xA;15 Jan 2023&#x9;&#x9;&#x9;061.96 - 071.96&#xA;16 Jan 2023&#x9;&#x9;&#x9;061.95 - 071.95&#xA;17 Jan 2023&#x9;&#x9;&#x9;061.94 - 071.94&#xA;18 Jan 2023&#x9;&#x9;&#x9;061.92 - 071.92&#xA;19 Jan 2023&#x9;&#x9;&#x9;061.91 - 071.91&#xA;20 Jan 2023&#x9;&#x9;&#x9;061.90 - 071.90&#xA;21 Jan 2023&#x9;&#x9;&#x9;061.89 - 071.89&#xA;22 Jan 2023&#x9;&#x9;&#x9;061.87 - 071.87&#xA;23 Jan 2023&#x9;&#x9;&#x9;061.86 - 071.86&#xA;24 Jan 2023&#x9;&#x9;&#x9;061.85 - 071.85&#xA;25 Jan 2023&#x9;&#x9;&#x9;061.84 - 071.84&#xA;26 Jan 2023&#x9;&#x9;&#x9;061.83 - 071.83&#xA;27 Jan 2023&#x9;&#x9;&#x9;061.82 - 071.82&#xA;28 Jan 2023&#x9;&#x9;&#x9;061.81 - 071.81&#xA;29 Jan 2023&#x9;&#x9;&#x9;061.80 - 071.80&#xA;30 Jan 2023&#x9;&#x9;&#x9;061.79 - 071.79&#xA;31 Jan 2023&#x9;&#x9;&#x9;061.77 - 071.77&#xA;01 Feb 2023&#x9;&#x9;&#x9;061.77 - 071.77&#xA;02 Feb 2023&#x9;&#x9;&#x9;061.76 - 071.76&#xA;03 Feb 2023&#x9;&#x9;&#x9;061.75 - 071.75&#xA;04 Feb 2023&#x9;&#x9;&#x9;061.74 - 071.74&#xA;05 Feb 2023&#x9;&#x9;&#x9;061.73 - 071.73&#xA;06 Feb 2023&#x9;&#x9;&#x9;061.72 - 071.72&#xA;07 Feb 2023&#x9;&#x9;&#x9;061.71 - 071.71&#xA;08 Feb 2023&#x9;&#x9;&#x9;061.70 - 071.70&#xA;09 Feb 2023&#x9;&#x9;&#x9;061.69 - 071.69&#xA;10 Feb 2023&#x9;&#x9;&#x9;061.68 - 071.68&#xA;11 Feb 2023&#x9;&#x9;&#x9;061.67 - 071.67&#xA;12 Feb 2023&#x9;&#x9;&#x9;061.66 - 071.66&#xA;"
                        Label="Roll Ranges Report"
                        Target="39P"
                        Coordinates=""
                        Prefix="Orient"
                        Units="U3">
                        
                        <StConstraintSchedulingWindows
                           Name="Roll Report Data"
                           Type="Roll Ranges"
                           StSchedulingPCF="1657399953378 1.0 242.85:252.85 1657486353378 1.0 242.83:252.83 1657572753378 1.0 242.82:252.82 1657659153378 1.0 225.41:270.21 1657745553378 1.0 225.3:270.3 1657831953378 1.0 225.28:270.28 1657918353378 1.0 225.27:270.27 1658004753378 1.0 225.25:270.25 1658091153378 1.0 225.23:270.23 1658177553378 1.0 225.22:270.22 1658263953378 1.0 225.1:270.3 1658350353378 1.0 225.08:270.28 1658436753378 1.0 224.98:270.36 1658523153378 1.0 224.95:270.35 1658609553378 1.0 224.83:270.43 1658695953378 1.0 224.81:270.41 1658782353378 1.0 224.69:270.49 1658868753378 1.0 224.56:270.56 1658955153378 1.0 224.54:270.54 1659041553378 1.0 224.42:270.62 1659127953378 1.0 224.19:270.79 1659214353378 1.0 224.07:270.87 1659300753378 1.0 223.94:270.94 1659387153378 1.0 223.82:271.02 1659473553378 1.0 223.59:271.19 1659559953378 1.0 223.46:271.26 1659646353378 1.0 223.23:271.43 1659732753378 1.0 229.1:271.5 1659819153378 1.0 235.07:271.47 1659905553379 1.0 226.83:271.63 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1.0 223.63:266.75 1662756753379 1.0 223.51:266.63 1662843153379 1.0 222.17:267.71 1662929553379 1.0 222.03:267.57 1663015953379 1.0 220.21:269.11 1663102353379 1.0 220.06:268.96 1663188753379 1.0 219.89:268.79 1663275153379 1.0 217.34:271.0 1663361553379 1.0 217.15:270.81 1663447953379 1.0 216.95:270.61 1663534353379 1.0 213.56:273.56 1663620753379 1.0 213.32:273.32 1663707153379 1.0 213.06:273.06 1663793553379 1.0 212.77:272.77 1663879953379 1.0 212.46:272.46 1663966353379 1.0 212.11:272.11 1664052753379 1.0 211.72:271.72 1664139153379 1.0 211.28:271.28 1664225553379 1.0 210.77:270.77 1664311953379 1.0 210.2:270.2 1664398353379 1.0 209.53:211.53:227.53:269.53 1664484753379 1.0 230.75:268.75 1664571153379 1.0 232.81:267.81 1664657553379 1.0 206.66:266.66 1664743953379 1.0 205.24:265.24 1664830353379 1.0 203.41:263.41 1664916753379 1.0 200.98:260.98 1665003153379 1.0 197.61:257.61 1665089553379 1.0 192.65:252.65 1665175953379 1.0 184.79:215.79:233.79:244.79 1665187200000 0.0 230.0:138.0 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