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<HSTProposal
   Phase2ID="13466"
   Phase="Phase II"
   AptVersion="Version 22.0.2 ">
   <!--**********************************************************************************************************************-->
   <!--This file is automatically generated and should not be edited by hand. Editing this file directly is at your own risk.-->
   <!--**********************************************************************************************************************-->
   <!--APT Output Product-->
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   <!--APT Version: Version 22.0.2 -->
   <!--Date: Mon Mar 24 17:28:21 GMT 2014-->
   
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            HasErrors="true"
            Cycle="21"
            IncludeSysInfo="true"
            NotificationAddress="ksahu@stsci.edu">
            
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               os.name="Mac OS X"
               os.version="10.8.5"
               java.version="1.7.0_40"
               Runtime.maxMemory="2667"
               linux.distribution="not available"
               linux.version="not available"
               screens="2560x1600" />
            
            <ErrorText>The number of orbits used does not match the number allocated
VISIBILITY OVERRUN</ErrorText>
            
            <SubmissionComments>Visit 1 has already been scheduled, but we found a problem. 
The filter was wrongly specified as F606W in two of the exposures, which I changed to F555W.
We also found that we get more exposures if we replace 170 sec with 200sec since some of the
overheads are hidden! So we replaced  the exposure times, which allowed us one more exposure.
We will greatly appreciate if visit 3 can be executed instead of Visit 1, at this late stage!

The exp times in visit 2 are ancreased to 200sec.</SubmissionComments>
            
            <SubmissionCommentsCheckSum>-612362738</SubmissionCommentsCheckSum>
            
            <SubmissionLog>----- Attempting Submission 2 (Tue Mar 18 18:31:37 GMT 2014) -----
  HST Phase II Proposal 13466 (13466.apt) successfully submitted.

----- Attempting Submission 3 (Tue Mar 18 18:46:48 GMT 2014) -----

----- Attempting Submission 4 (Tue Mar 18 20:44:53 GMT 2014) -----
  HST Phase II Proposal 13466 (13466.apt) successfully submitted.

----- Attempting Submission 5 (Wed Mar 19 15:36:12 GMT 2014) -----
  HST Phase II Proposal 13466 (13466.apt) successfully submitted.

----- Attempting Submission 6 (Wed Mar 19 18:31:35 GMT 2014) -----

----- Attempting Submission 7 (Mon Mar 24 17:28:21 GMT 2014) -----</SubmissionLog>
            
            <Phase2DiagnosticJustification>can visit 1 be replaced with visit 3 please? Thanks.</Phase2DiagnosticJustification>
         </Phase2SubmissionData>
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   <ProposalInformation
      Category="GO"
      PureParallelProposal="false"
      Cycle="21"
      STScIEditNumber="4">
      
      <Title>Determining the Mass of Proxima Centauri through Astrometric Microlensing</Title>
      
      <Abstract>We propose to determine the mass of our nearest neighbor, Proxima Centauri, using the novel technique of astrometric microlensing. Proxima is a dM6e star, with an estimated mass of about 0.12 Msun, lying at a distance of 1.3 pc and having a large proper motion of 3.8 arcsec/yr. In a reprise of the famous 1919 solar eclipse that verified general relativity, Proxima will pass in front of a pair of 18th-magnitude background stars in 2015, affording us two independent opportunities to measure the relativistic deflection. The first passage will occur in May 2015 (impact parameter 1.5 arcsec), and the second in June 2015 (impact parameter 1.4 arcsec). As Proxima passes in front, it will cause a relativistic deflection of the background stars' images by ~0.5 milliarcsec, an amount readily detectable with HST/WFC3.
The gravitational deflection angle depends only upon the distances and relative positions of the stars, and the mass of the lens (Proxima). Since the distance to Proxima is well known from accurate parallax measurements, and the relative stellar positions can be determined precisely before the event, the astrometric measurement offers a unique and direct method to measure the mass of a single, isolated star. We anticipate better than 10% accuracy for the mass determination. The mass of Proxima is of special interest because it is the nearest M dwarf, representing the most common type of star in the Galaxy, for which the mass-luminosity relation is still uncertain at present.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Kailash"
         MiddleInitial="C."
         LastName="Sahu"
         ESAMember="false"
         UniqueID="2253"
         Institution="Space Telescope Science Institute"
         Country="USA"
         State="MD"
         Contact="true" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Howard"
         MiddleInitial="E."
         LastName="Bond"
         ESAMember="false"
         UniqueID="2894"
         Institution="The Pennsylvania State University"
         Country="USA"
         State="PA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Jay"
         LastName="Anderson"
         ESAMember="false"
         UniqueID="3772"
         Institution="Space Telescope Science Institute"
         Country="USA"
         State="MD"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Martin"
         LastName="Dominik"
         ESAMember="true"
         UniqueID="8434"
         Institution="University of St. Andrews"
         Country="GBR"
         State="England"
         Contact="false"
         AdminUSPI="false" />
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>The first epoch observations will be taken in a few different filters (F475W, F555W, F606W, F814W) to better characterize the spectral type of the source. Subsequent observations will be taken mainly in 2 filters (F606W and F814W). We will obtain one short (0.5 sec) exposure to get an unsaturated image of Proxima, in order to register its position. The other exposures will be of 90 to 200 sec durations, so that the source stars will have a S/N &amp; 300 in each exposure. We can obtain about 10 such exposures in each orbit, at 2 dither positions, which would be adequate to achieve the astrometric accuracy required for the project.</ObservingDescription>
            
            <RealtimeJustification />
            
            <CalibrationJustification />
            
            <AdditionalComments />
         </Phase2Questions>
      </Questions>
      
      <Orbits
         ThisCycle2GyroPrimary="2"
         ThisCycle2GyroParallel="0"
         NextCycle2GyroPrimary="2"
         NextCycle2GyroParallel="0"
         AfterNext2GyroPrimary="8"
         AfterNext2GyroParallel="0" />
      
      <Phase1ProposalInformation
         TotalTargets="1"
         Attachment="/Users/ksahu/stprop12/proxima/prox7.pdf"
         ProposalSize="SMALL">
         
         <ScientificCategory>COOL STARS</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="Astrometry" />
         
         <ScientificKeyword2
            Keyword="Gravitational Lensing" />
         
         <ScientificKeyword3
            Keyword="Low-Mass And Cool Stars" />
         
         <ScientificKeyword4
            Keyword="Microlensing" />
         
         <ProprietaryPeriod>12</ProprietaryPeriod>
         
         <CalibProp>false</CalibProp>
         
         <UvInit>false</UvInit>
         
         <ChandraCoord>0.0</ChandraCoord>
         
         <NOAONights>0.0</NOAONights>
         
         <Treasury>false</Treasury>
         
         <MultiCycleTreasury>false</MultiCycleTreasury>
         
         <Theory>false</Theory>
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      <Phase2ProposalInformation
         PCFlag="true"
         ProposalSize="SMALL_CYCLE21">
         
         <Availability>AVAILABLE</Availability>
      </Phase2ProposalInformation>
   </ProposalInformation>
   
   <Targets>
      
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         Name="PROXIMA-CEN-SOURCE"
         Number="1"
         ReferenceFrame="ICRS"
         ProvisionalCoordinates="14 29 42.9485 -62 40 46.16">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>K V-IV</Description>
         </PrimaryDescription>
         
         <Comments>This object was updated to the SOURCE that Proxima-Cen is going to lens. At present, the source and proxima-cen are separated by about 10.5 arcsec, and this separation will slowly decrease to 1.5 arcsec in 2015.</Comments>
         
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         Instrument="WFC3"
         Number="1"
         NumberOfOrbits="1"
         NumberOfIterations="12"
         TotalOrbits="12"
         PureParallel="false"
         CoordinatedParallel="false"
         TargetOfOpportunity="No"
         CVZ="false"
         Duplication="false">
         
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               <Polarimetry>No</Polarimetry>
               
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 :proposal-id 13466
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 :proposal-version -1
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                     <StConstraintSchedulingWindows
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                     <AncillaryData
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                        Label="Comments">
                        
                        <String>The scheduling data was generated by CASM 22.0.</String>
                        
                        <String>CASM was run in Phase II mode.</String>
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                  <AncillaryData
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