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   <!--Date: Mon Jun 25 16:39:57 GMT 2012-->
   
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            <SubmissionLog>Assigned ID: 1003
----- Attempting Submission 1 (Sat Feb 25 00:33:41 GMT 2012) -----
  HST Phase I Proposal 1003 (PTF11kly_HST_PROPOSAL.pdf.apt) successfully submitted.
----- Attempting Submission 2 (Sat Feb 25 00:51:56 GMT 2012) -----
  HST Phase I Proposal 1003 (PTF11kly_HST_PROPOSAL.pdf.apt) successfully submitted.
----- Attempting Submission 3 (Sat Feb 25 00:57:31 GMT 2012) -----
  HST Phase I Proposal 1003 (PTF11kly_HST_PROPOSAL.pdf.apt) successfully submitted.
----- Attempting Submission 4 (Sat Feb 25 00:58:55 GMT 2012) -----</SubmissionLog>
            
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            <SubmissionLog>----- Attempting Submission 1 (Mon Jun 25 16:39:57 GMT 2012) -----</SubmissionLog>
            
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   <ProposalInformation
      Category="GO"
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      Cycle="20"
      STScIEditNumber="0"
      ProposalSize="SMALL">
      
      <Title>Late Time STIS Spectroscopy of the Extremely Nearby Type Ia SN 2011fe</Title>
      
      <Abstract>In the first 2-3 months after the explosion of a Type Ia supernova, the innermost layers of the ejecta are concealed from view by a brilliant pseudo-photosphere.  Observations obtained many months later, when the ejecta become nebular, enable us to peer deep into these layers and probe different explosion physics than is possible earlier on --- but at a cost.  By this point, the supernova has faded dramatically, so only the closest events may be observed.  SN 2011fe is the nearest Type Ia supernova discovered in a quarter century.  We propose to obtain STIS spectroscopy of this remarkable supernova, a year after explosion, and combine these space-based observations with ground-based optical and near-infrared spectroscopy for analysis.  Using the focusing lens of radiative transfer simulations, we will constrain the amount of radioactive nickel produced in the explosion, explore the extent of large-scale hydrodynamical mixing, and reconstruct the abundance stratification of the innermost ejecta.  SN 2011fe represents a unprecedented opportunity to study how Type Ia supernovae explode, and is likely to remain so for decades to come.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Rollin"
         LastName="Thomas"
         ESAMember="false"
         UniqueID="6135"
         Institution="Lawrence Berkeley National Laboratory"
         Country="USA"
         State="CA"
         Contact="true" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Peter"
         MiddleInitial="E."
         LastName="Nugent"
         ESAMember="false"
         UniqueID="4243"
         Institution="Lawrence Berkeley National Laboratory"
         Country="USA"
         State="CA"
         Contact="true"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Eddie"
         LastName="Baron"
         ESAMember="false"
         UniqueID="5883"
         Institution="University of Oklahoma Norman Campus"
         Country="USA"
         State="OK"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Daniel"
         LastName="Kasen"
         ESAMember="false"
         UniqueID="8049"
         Institution="University of California - Berkeley"
         Country="USA"
         State="CA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Mark"
         LastName="Sullivan"
         ESAMember="true"
         UniqueID="5893"
         Institution="University of Oxford"
         Country="GBR"
         State="England"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Eric"
         LastName="Hsiao"
         ESAMember="false"
         UniqueID="8846"
         Institution="Carnegie Institution of Washington"
         Country="USA"
         State="DC"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Mark"
         MiddleInitial="M."
         LastName="Phillips"
         ESAMember="false"
         UniqueID="3669"
         Institution="Carnegie Institution of Washington"
         Country="USA"
         State="DC"
         Contact="false"
         AdminUSPI="false" />
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>Our goal is to obtain ultraviolet spectroscopy of the extremely nearby Type Ia supernova 2011fe in M101 using STIS, 13 months after it reached peak luminosity. We hope our observations can be carried out at the very start of Cycle 20, since the supernova will only continue to fade.  We will combine these observations with complementary, time-coordinated ground-based optical and near-infrared observations, and analyze them together using comprehensive radiative transfer simulations.  Comparing synthetic spectra to late-time observations will allow us to explore the extent of large-scale hydrodynamic mixing during the explosion, constrain the amount of radioactive nickel produced, and reconstruct the multi-dimensional distribution of the innermost ejecta.  Careful examination of nebular phase lines will provide constraints on large-scale explosion asymmetry.  

We plan a total of 10 orbits split into 3 visits.  Our strategy is to maximize S/N we can get in the NUV, but also obtain some optical spectroscopy that can retire risk associated with constraints on ground-based visibility of the target in late September.

The first 2 visits are in the STIS/NUV-MAMA configuration.  The first visit uses 5 orbits, the second uses 4.  We dither along the slit at the end of every few orbits by 11 pixels to reduce the impact of hot pixels.  The third and final visit uses the STIS/CCD G430L and G750L configurations in sequence in a single orbit.  Exposure time and S/N are estimated by rescaling fluxes estimated from an HST spectrum of SN1992A obtained 291 days past peak and using the appropriate online STIS ETC's.  We account for the fact that SN2011fe was over 10 times brighter than SN1992A at peak since it was much closer, and we also account for an additional ~100 days of decline in flux since our observations are later on the light curve of SN2011fe than those of SN1992A.</ObservingDescription>
            
            <RealtimeJustification>Our observations need to come as close to the beginning of Cycle 20 as possible.  If the observations can be scheduled in September, this is not a problem for us at all.  All 3 visits need to be scheduled as close together in time as is feasible.  We understand the MAMA observing constraints prevent those visits from taking place in the same day.</RealtimeJustification>
            
            <CalibrationJustification />
            
            <AdditionalComments />
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         AfterNext2GyroParallel="0" />
      
      <Phase1ProposalInformation
         TotalTargets="1"
         Attachment="/Users/rthomas/project/hst/PTF11kly.pdf">
         
         <ScientificCategory>HOT STARS</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="Radiative Transfer" />
         
         <ScientificKeyword2
            Keyword="Supernova Remnants" />
         
         <ScientificKeyword3
            Keyword="Supernovae" />
         
         <ProprietaryPeriod>12</ProprietaryPeriod>
         
         <CalibProp>false</CalibProp>
         
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         PCFlag="false">
         
         <Availability>SUPPORTED</Availability>
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         Name="SN2011FE"
         Number="1"
         ReferenceFrame="ICRS"
         Redshift="0.0008"
         ProvisionalCoordinates="14 03 5.8104 +54 16 25.39">
         
         <PrimaryCategory>EXT-STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>SUPERNOVA TYPE IA</Description>
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            <AlternateName>PTF11KLY</AlternateName>
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         <Equinox>J2000</Equinox>
         
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               Magnitude="19.5"
               MagnitudeUnc="0.3" />
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         CoordinatedParallel="false"
         TargetOfOpportunity="No"
         CVZ="false"
         Duplication="false">
         
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               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G230L</SpectralElement>
               
               <Wavelength>2376</Wavelength>
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            ObservationRequirements="BETWEEN 01-OCT-2012:00:00:00 AND 31-OCT-2012:00:00:00;" />
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         <SubpatternPatternType>LINE</SubpatternPatternType>
         
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            Number="3"
            Label="MAMA Spectrum"
            TargetName="SN2011FE"
            Config="STIS/NUV-MAMA"
            Opmode="ACCUM"
            Aperture="52X0.2"
            SpElement="G230L"
            Wavelength="2376"
            NumberOfIterations="1"
            EtcRunId="STIS.sp.407505"
            TimePerExposure="3085"
            RealtimeAnalysis="false"
            RequiresUplink="false"
            Expand="false"
            LowSky="false"
            Shadow="false"
            NewAlignment="false"
            NewObset="false"
            NewObsetFullAcq="false"
            SpecialCommand="false">
            
            <MaxDur />
            
            <MinDur />
            
            <Comments />
            
            <InstrumentParameters />
            
            <SubExposures>
               
               <SubExposure
                  OrbitNumber="5" />
            </SubExposures>
         </Exposure>
      </Visit>
      
      <Visit
         Number="02"
         PCSMode="Fine"
         After=""
         Before="03-OCT-2012:00:00:00">
         
         <ToolData>
            
            <ToolDataItem
               Key="OpTimeStamp">
               
               <OpToolDataDate>
                  
                  <Time>1340386653187</Time>
               </OpToolDataDate>
            </ToolDataItem>
            
            <ToolDataItem
               Key="Visit Planner">
               
               <VpVisitData>
                  
                  <StVisitSchedulingWindows
                     Binary="true"
                     UpToDate="true"
                     StSchedulingPCF="1336003200000 0.0 1336046400000 1.0 1338379199000 0.0 1340798400000 1.0 1343131199000 0.0 1343649600000 1.0 1344427199000 0.0 1345550400000 1.0 1345982399000 0.0 1346846400000 1.0 1349179199000 0.0 1396396800000">
                     
                     <StConstraintSchedulingWindows
                        Name="Before"
                        StSchedulingPCF="1336003200000 1.0 1349222400000 0.0 1396396800000" />
                     
                     <StConstraintSchedulingWindows
                        Name="Target Visibility"
                        StSchedulingPCF="1336003200000 0.0 1336046400000 1.0 1338379199000 0.0 1340798400000 1.0 1343131199000 0.0 1343649600000 1.0 1344427199000 0.0 1345550400000 1.0 1345982399000 0.0 1346846400000 1.0 1349179199000 0.0 1350993600000 1.0 1353326399000 0.0 1355745600000 1.0 1357905599000 0.0 1361016000000 1.0 1362657599000 0.0 1365249600000 1.0 1367323199000 0.0 1369224000000 1.0 1371556799000 0.0 1372680000000 1.0 1372852799000 0.0 1373976000000 1.0 1377604799000 0.0 1380024000000 1.0 1382270399000 0.0 1384171200000 1.0 1386071999000 0.0 1388923200000 1.0 1390996799000 0.0 1394193600000 1.0 1395748799000 0.0 1396396800000" />
                     
                     <StConstraintSchedulingWindows
                        Name="Timing link"
                        StSchedulingPCF="1336003200000 0.0 1336046400000 1.0 1338465599000 0.0 1340798400000 1.0 1343217599000 0.0 1343649600000 1.0 1344427199000 0.0 1345550400000 1.0 1345982399000 0.0 1346846400000 1.0 1349179199000 0.0 1396396800000">
                        
                        <AncillaryData
                           Title="Comments"
                           Label="Comments">
                           
                           <String>Timing link suitability includes constraints ([Sequence (01 02 03) within  3.0 days])</String>
                        </AncillaryData>
                     </StConstraintSchedulingWindows>
                     
                     <AncillaryData
                        Title="Comments"
                        Label="Comments">
                        
                        <String>The scheduling data was generated by CASM 20.2.</String>
                        
                        <String>CASM was run in Phase II mode.</String>
                     </AncillaryData>
                  </StVisitSchedulingWindows>
                  
                  <AncillaryData
                     Title="Roll Ranges Report"
                     Label="Roll Ranges Report"
                     Header="  Target: SN2011FE&#xA;  RA: 14 03 5.8130&#xA;  DEC: +54 16 25.36&#xA;  Dates: 5/3/2012 -- 4/2/2014&#xA;&#xA;Day&#x9;Available Roll Ranges (U3 Angles)">
                     
                     <RollRangeChartPanel
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                        StartTime="2012.124"
                        EndTime="2014.92"
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149.48:2012.166 111.24 148.64:2012.167 110.42 147.82:2012.168 126.99 136.99:2012.169 126.17 136.17:2012.170 125.35 135.35:2012.171 124.52 134.52:2012.172 123.69 133.69:2012.173 122.87 132.87:2012.174 122.04 132.04:2012.175 121.22 131.22:2012.176 120.39 130.39:2012.177 119.56 129.56:2012.178 118.73 128.73:2012.179 117.9 127.9:2012.180 117.07 127.07:2012.181 116.23 126.23:2012.182 115.4 125.4:2012.183 114.56 124.56:2012.184 113.72 123.72:2012.185 112.88 122.88:2012.186 112.04 122.04:2012.187 111.19 121.19:2012.188 110.35 120.35:2012.189 109.5 119.5:2012.190 108.64 118.64:2012.191 107.79 117.79:2012.192 106.93 116.93:2012.193 106.07 116.07:2012.194 105.21 115.21:2012.195 104.34 114.34:2012.196 103.47 113.47:2012.197 102.6 112.6:2012.198 101.72 111.72:2012.199 100.84 110.84:2012.200 99.96 109.96:2012.201 99.07 109.07:2012.202 98.18 108.18:2012.203 97.29 107.29:2012.204 96.39 106.39:2012.205 95.49 105.49:2012.206 94.58 104.58:2012.207 93.67 103.67:2012.208 92.76 102.76:2012.209 91.84 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