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<HSTProposal
   Phase1ID="236"
   Phase2ID="14246"
   Phase="Phase II"
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   <!--Date: Wed Nov 11 15:57:14 GMT 2015-->
   
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            <SubmissionLog>Assigned ID: 236

----- Attempting Submission 1 (Thu Apr 09 19:11:08 GMT 2015) -----
HST Phase I Proposal 236 (gies.apt) successfully submitted.
Receipt: # 236-1</SubmissionLog>
            
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            <SubmissionComments>Dear Nolan and Denise, 

I have revised again the Phase II proposal for GO 14246.
Here are the changes:

- I increased the ACQ/IMAGE exposures to reach a S/N=40.

- I set Buffer time = exposure time to ensure full read of the buffers. 

- I adjusted the science exposures to fit in the allotted orbits. 

Cheers, Doug</SubmissionComments>
            
            <SubmissionCommentsCheckSum>-889433495</SubmissionCommentsCheckSum>
            
            <SubmissionLog>----- Attempting Submission 1 (Wed Jul 15 19:15:38 GMT 2015) -----
HST Phase II Proposal 14246 (gies.apt) successfully submitted.
Receipt: # 14246-1

----- Attempting Submission 2 (Wed Nov 04 17:14:56 GMT 2015) -----
HST Phase II Proposal 14246 (gies.apt) successfully submitted.
Receipt: # 14246-2

----- Attempting Submission 3 (Wed Nov 11 15:57:14 GMT 2015) -----</SubmissionLog>
            
            <Phase2DiagnosticJustification>APT crashed when attempting this operation. 
I did inspect images and confirmed the coordinates.</Phase2DiagnosticJustification>
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   <ProposalInformation
      Category="GO"
      PureParallelProposal="false"
      Cycle="23"
      STScIEditNumber="0">
      
      <Title>The Fastest Rotating Stars</Title>
      
      <Abstract>The VLT FLAMES Survey of the massive stars in the Tarantula Nebula region 
of the LMC has led to the discovery of the two fastest rotating stars: 
VFTS 102 and 285 with V sin i = 610 and 609 km/sec.  These two O-dwarfs 
may be single stars born with extraordinarily high angular momentum or 
they may have been spun up in a binary system by mass transfer or merger.
Extreme rotators like these suffer gravity darkening that makes their 
equatorial regions cooler than the polar zones, so that the equatorial 
parts close to the limb contribute less flux and create narrower lines. 
We show how HST/COS spectroscopy of the far-ultraviolet spectra can 
be used with the optical rotational line broadening to estimate this 
gravity darkening effect and to determine the ratios of equatorial to 
critical rotation velocity for these two stars.  This ratio is key to 
describing the bipolar winds of rapidly rotating stars, and the COS 
spectra will record the important wind lines in the FUV for comparison 
with models of asymmetric winds.  The COS spectra will yield estimates 
of the stellar masses, radii, rotation rates, and abundances that will 
help us assess the origin and destiny of these remarkable stars in 
particular and massive rotating stars in general.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Douglas"
         MiddleInitial="R."
         LastName="Gies"
         ESAMember="false"
         Retired="false"
         UniqueID="765"
         Institution="Georgia State University Research Foundation"
         Country="USA"
         State="GA"
         Contact="true" />
      
      <CoInvestigator
         Honorific="Mr."
         FirstName="Zhao"
         LastName="Guo"
         ESAMember="false"
         Retired="false"
         UniqueID="17681"
         Institution="Georgia State University Research Foundation"
         Country="USA"
         State="GA"
         Contact="false"
         AdminUSPI="false" />
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>We propose to obtain COS observations of the FUV spectrum of VFTS 102 and 285 using
the G130M grating to cover most of the range from 1150 to 1450 with a resolving power of
18,000 (although we may make a modest reduction in resolving power by spectral smoothing
in the data analysis stage to increase the signal-to-noise ratio). Our primary goal is to obtain
cross-correlation functions of the FUV photospheric lines with model spectra. Numerical
tests with model spectra indicate that we can estimate the FWHM of the cross-correlation
function to better than 5% accuracy (comparable to the optical measurements of V sin i;
Ramirez-Agudelo et al. 2013) with a signal-to-noise ratio of S/N = 10 per resolution element,
so our goal is to obtain a S/N = 10 at 1310 in a single visit to each target. This S/N is also
adequate for our investigation of the line morphology of the wind lines of Si III 1206, 
N V 1240, and Si IV 1400. 

We used the COS ETC and assumed that the spectral energy distributions are given by 
reddened versions of Castelli &amp; Kurucz model spectra for the spectral classifications 
of the two targets. The model spectra were normalized using the UIT B1 magnitudes 
(effective wavelength = 1521 Angstroms) of the targets from Parker et al. (1998, 
AJ, 116, 180) and B-V colors from Evans et al. (2011), and the extinctions were 
estimated using intrinsic colors from Wegner (1994) and a ratio of total-to-
selective extinction of R = 3.41 (LMC average). The COS ETC gave exposure times of
4500 and 440 seconds for VFTS 102 and 285, respectively (the latter being hotter and less
reddened).  Following the example in the Instrument Handbook, we would obtain this result
through several exposures at each of four FP-POS spectral offsets and two or three CENWAVE 
positions in order to fill in the gap in spectral coverage between the two COS detectors.  
All these exposures would be made in standard TIME-TAG mode.

We estimate that there are 54 minutes of visibility per orbit for the declination of both
targets (delta = -69 deg). In the first orbit, we require 3 minutes for acquisition, 
5 minutes for COS FUV acquisition and search, 2 minutes for PEAKXD cross dispersion peakup, 
and 5 minutes for PEAKD peakup in the dispersion direction. This leaves 39 minutes for science
exposures. In succeeding orbits, we need 4 minutes for re-acquisition, yielding a net of 50
minutes for science exposure. Thus, for the fainter target, VFTS 102, we are requesting
three orbits (with 4, 4, and 4 sub-exposures for each of 3 CENWAVE positions; this will
require orbits 1, 2, and 3, respectively).  We can obtain all the sub-exposures 
(four  in each of 2 CENWAVE positions) in a single orbit for the brighter target, VFTS 285.

Dr. Hugues Sana kindly provided F275W AB magnitudes for both stars based upon 
unpublished HST observations:
m(F275W) = 15.044 for VFTS-102
m(F275W) = 14.013 for VFTS-285
The COS ETC calculations using these estimates led to exposure times that are a 
factor of 3.1 and 3.9 times lower for VFTS-102 and VFTS-285, repectively, than given above.
Given this uncertainty, the BUFFER-TIME estimates were lowered by these factors 
(and the recommended 2/3) from the ETC calculations in order to be sure the 
buffers do not reach full capicity.</ObservingDescription>
         </Phase2Questions>
      </Questions>
      
      <Orbits
         ThisCycle2GyroPrimary="4" />
      
      <Phase1ProposalInformation
         Attachment="/nfs/morgan4/gies/TeX/NASA/HST_VFTS/gies.pdf"
         ProposalSize="SMALL">
         
         <ScientificCategory>HOT STARS</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="Main Sequence Stars" />
         
         <ScientificKeyword2
            Keyword="Massive Stars" />
         
         <ScientificKeyword3
            Keyword="Stellar Evolution And Models" />
         
         <ScientificKeyword4
            Keyword="Winds/Outflows/Mass-Loss" />
         
         <ScientificKeyword5
            Keyword="Young Star Clusters In External Galaxies" />
         
         <ProprietaryPeriod
            Default="true">12</ProprietaryPeriod>
         
         <CalibProp>false</CalibProp>
         
         <UvInit>true</UvInit>
         
         <Treasury>false</Treasury>
         
         <MultiCycleTreasury>false</MultiCycleTreasury>
      </Phase1ProposalInformation>
      
      <Phase2ProposalInformation
         PCFlag="false"
         ProposalSize="SMALL_CYCLE21">
         
         <Availability>SUPPORTED</Availability>
      </Phase2ProposalInformation>
   </ProposalInformation>
   
   <Targets>
      
      <FixedTarget
         Name="VFTS-102"
         Number="1"
         ReferenceFrame="ICRS"
         RAPMValue="-0.1"
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-1.3"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000.0"
         AnnualParallax="0."
         ProvisionalCoordinates="05 37 39.2480 -69 09 51.04">
         
         <PrimaryCategory>EXT-STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>MAIN SEQUENCE O</Description>
         </PrimaryDescription>
         
         <Extended>NO</Extended>
         
         <Comments>This object was generated by the targetselector and retrieved from the SIMBAD database.
UIT m(B1)=14.55
F(1521)=5.5E-15 erg/s/cm^2/Angstrom</Comments>
         
         <AlternateNames>
            
            <AlternateName>UCAC4-105-014018</AlternateName>
            
            <AlternateName>2MASS-J05373924-6909510</AlternateName>
         </AlternateNames>
         
         <EquatorialPosition
            Value="05 37 39.2400 -69 09 51.12">
            
            <RAUnc
               Secs="0.01" />
            
            <DECUnc
               Arcsec="0.1" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="15.70"
               MagnitudeUnc="0.10" />
            
            <OtherFluxes>E(B-V)=0.63+/-0.10</OtherFluxes>
         </Fluxes>
      </FixedTarget>
      
      <FixedTarget
         Name="VFTS-285"
         Number="2"
         ReferenceFrame="ICRS"
         RAPMValue="-0.40"
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-0.23"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000.0"
         AnnualParallax="0"
         ProvisionalCoordinates="05 38 17.3400 -69 05 42.14">
         
         <PrimaryCategory>EXT-STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>MAIN SEQUENCE O</Description>
         </PrimaryDescription>
         
         <Extended>NO</Extended>
         
         <Comments>This object was generated by the targetselector and retrieved from the SIMBAD database.
UIT m(B1)=12.66 
F(1521)=3.1E-14 erg/s/cm^2/Angstrom
Note that target VFTS-285 has a close companion VFTS-290 that is 
similar in brightness at a separation of 4 arcsec.</Comments>
         
         <AlternateNames>
            
            <AlternateName>2MASS-J05381736-6905425</AlternateName>
            
            <AlternateName>UCAC4-105-014155</AlternateName>
         </AlternateNames>
         
         <EquatorialPosition
            Value="05 38 17.3400 -69 05 42.14">
            
            <RAUnc
               Secs="0.02" />
            
            <DECUnc
               Arcsec="0.3" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="15.63"
               MagnitudeUnc="0.10" />
            
            <OtherFluxes>E(B-V)=0.23+/-0.10</OtherFluxes>
         </Fluxes>
      </FixedTarget>
   </Targets>
   
   <Observations>
      
      <Observation
         TargetName="VFTS-102"
         Instrument="COS"
         Number="1"
         NumberOfOrbits="3"
         NumberOfIterations="1"
         TotalOrbits="3"
         PureParallel="false"
         CoordinatedParallel="false"
         TargetOfOpportunity="No"
         CVZ="false"
         Duplication="false">
         
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            <Configuration>
               
               <Config>COS/FUV</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G130M</SpectralElement>
               
               <Wavelength>1309</Wavelength>
            </Configuration>
         </Configurations>
         
         <ObservationRequirements
            NoConstraints="true" />
         
         <AladinPhase1Requirements
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            Aperture="PSA/BOA"
            MosaicHeight=""
            MosaicWidth=""
            MosaicTileOverlap="10.0"
            AladinOrientationAngle="">
            
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            <AladinPhase1SubExposure0
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               CopyNumber="0"
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         <SuitabilityResults
            DaysHigh="0"
            DaysHighMed="0"
            DaysLowMed="0"
            DaysLow="0"
            OrbitsPerDay="0.0"
            ObservationRequirements="NOCONSTRAINTS" />
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         NumberOfOrbits="1"
         NumberOfIterations="1"
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         PureParallel="false"
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               <Wavelength>1309</Wavelength>
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   </Observations>
   
   <Patterns />
   
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      <Visit
         Number="01"
         Label="VFTS-102"
         Status="implementation"
         After=""
         Before="">
         
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                        <String>CASM was run in Phase II mode.</String>
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         <Exposure
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         <Exposure
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      <Visit
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         Label="VFTS-285"
         Status="implementation"
         After=""
         Before="">
         
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                  <Time>1447257080076</Time>
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                     <AncillaryData
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                        <String>The scheduling data was generated by CASM 23.2.</String>
                        
                        <String>CASM was run in Phase II mode.</String>
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