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<HSTProposal
   Phase1ID="642"
   Phase2ID="12938"
   Phase="Phase II"
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   <!--Date: Tue Jul 10 20:14:32 GMT 2012-->
   
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            NotificationAddress="dieterich@chara.gsu.edu"
            AssignedID="642">
            
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            <SubmissionComments />
            
            <SubmissionLog>Assigned ID: 642
----- Attempting Submission 1 (Fri Feb 24 20:03:39 GMT 2012) -----</SubmissionLog>
            
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            <SubmissionComments>Hi Beth
Here is my phase II!
This program has some tricky schedulling, as we are trying to align the stis long slit along the axis of binaries that
move significantly on the scale of one HST cycle. I used thevisit planer to get the widest possible windows,
and I have also included a table of ORIENT angles under the comments for each visit. 

The one tricky observation will be GJ1081, visit 5. The binary separation is ony ~0.1" and delta mag is ~2.
I hope to be able to deconvolve the spectra using symmetry arguments, but it will be difficult. Do you have any
thoughts on the feasibility of it? if it is hopeless we could try occulting the primary and obtaining a spectrum 
of the secondary, though that would not really meet the science goals of this program.

Thanks for your help!
Serge</SubmissionComments>
            
            <SubmissionLog>----- Attempting Submission 1 (Tue Jul 10 20:14:32 GMT 2012) -----</SubmissionLog>
            
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   <ProposalInformation
      Category="GO"
      PureParallelProposal="false"
      Cycle="20"
      STScIEditNumber="0"
      ProposalSize="SMALL">
      
      <Title>Probing Fundamental Stellar Parameters with HST/STIS Spectroscopy of M Dwarf Binaries</Title>
      
      <Abstract>We propose to obtain spatially resolved intermediate resolution HST/STIS spectra of
six M dwarf binaries ranging in spectral type from M2V to M8V and in mass from 0.40
to 0.074 Solar Masses. All binaries have previously had their orbits mapped by HST/FGS,
leading to individual dynamical masses with a precision &lt; 5%. The last fifteen years have
seen the development of sophisticated theoretical models for the interior structure, evolution,
and atmospheric properties of low mass stars. These models have thus far been difficult to
test in a holistic manner due to the complex interplay of the variables effective temperature,
mass, age, surface gravity, and metallicity. Fortunately these parameters are now measurable
directly via comparisons with synthetically generated spectra, as has been successfully
demonstrated by various studies. By assuming co-evolution and equal metallicity for the components
of a binary system with known masses, we will be able to test model spectra and constrain the
modeling of fundamental structural, evolutionary, and atmospheric parameters throughout most of the
M dwarf spectral class. The proposed observations are part of the PI's thesis effort to better
characterize M dwarfs and objects near the hydrogen burning mass limit.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Mr."
         FirstName="Sergio"
         MiddleInitial="B."
         LastName="Dieterich"
         ESAMember="false"
         UniqueID="8679"
         Institution="Georgia State University Research Foundation"
         Country="USA"
         State="GA"
         Contact="true" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Todd"
         MiddleInitial="J."
         LastName="Henry"
         ESAMember="false"
         UniqueID="3064"
         Institution="Georgia State University Research Foundation"
         Country="USA"
         State="GA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Russel"
         MiddleInitial="J"
         LastName="White"
         ESAMember="false"
         UniqueID="3665"
         Institution="Georgia State University Research Foundation"
         Country="USA"
         State="GA"
         Contact="false"
         AdminUSPI="false" />
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Wei-Chun"
         LastName="Jao"
         ESAMember="false"
         UniqueID="8041"
         Institution="Georgia State University Research Foundation"
         Country="USA"
         State="GA"
         Contact="false"
         AdminUSPI="false" />
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>We propose to obtain intermediate resolution (R~6,000) optical
spectroscopy of point source binaries with separations ranging from
0.2" to 1.0" using the STIS CCD, the G750M
grating, and the 0.2" long slit. The observational goal is to
obtain spatially resolved spectra with a resolution sufficient to
measure the equivalent widths of several indicators of temperature,
gravity, and metallicity occurring throughout the red optical
range. The next highest resolution red optical grating, G750L, has a
dispersion of 4.92 Ang/pixel, and is therefore not suitable to
measure the equivalent width of fine features such as absorption lines
due to alkali metals and H emission.  We plan on observing both
components simultaneously by orienting  HST so as to align the
slit with the binary axis. All primary
targets are bright enough that they can be acquired through the
standard STIS acquisition procedure, without requiring an offset
from a brighter nearby star. Based on the FGS measurements used
to calculate the orbits, our orbital solutions can predict position
angles with residuals &lt;1.0D.  If we assure that the primary
star is centered in the 0.2" slit by performing a peakup after
coarse acquisition, requiring that a secondary 1.0" away from the
primary be placed within the central 2/4 of the slit yields a position
angle tolerance of 3D, which is much larger than the residuals
of our orbital solutions. Also, because 1.0" is an
upper limit for separations, the alignment tolerance will be
greater than 3.0D in most cases. Upon acquisition we will take an
image of the binary as viewed through the slit without the grating to
measure the precise centering of both components. This image will
allow us to estimate what fraction of the flux from each component is
going through the slit, and thus allow us to establish a relative flux
calibration for the spectra.  The G750M grating has a narrow spectral
range of only 570 Angstroms, and therefore several standard tilt positions
have been configured in order to increase spectral coverage. We
propose to use the seven reddest tilt positions, providing continuous
coverage from 6,482 Ang. to 10,137 Ang. On the blue end, this range
covers the important Halpha 6563 and Li 6708
lines. On the red end, the region around 1 micron contains several
gravity sensitive FeH bands that are difficult to study from Earth due
to telluric H2O absorption. In order to save time while assuring
uniform quality, we will optimize the exposure time in each grating
tilt to provide a signal-to-noise of at least 20 for that spectral
region. For our faintest target, GJ1245C, the ETC predicts a total
exposure time of ~19min, with the longest (bluest) exposure
lasting ~7 minutes and the shortest (reddest) exposure lasting
~45s. Because the overheads are the same regardless of target
brightness and because each target must use an integer number of
orbits, brighter targets will be exposed to a signal-to-noise
significantly higher than 20 at no additional time cost to the
program. The standard tilt positions have a small coverage overlap
that will provide spectrum continuity and facilitate flux
calibration. Because we are observing in red optical wavelengths, it
will be necessary to obtain fringe flats at each tilt position. The
need to tilt the grating to seven different positions during the
observation makes the overheads for this program relatively
high. According to the  STIS Instrument Handbook, Chapter 9,
tables 9.1 and 9.2, each tilt will require a 7 minute overhead,
including the time necessary to obtain fringe flats. Adding up the
time required for guide star acquisition,  STIS acquisition,
peakup, slit imaging, and grating tilts results in 74 minutes of
overhead per visit. Therefore each visit will have to be carried out
over two orbits. By performing the overheads associated with three of
the grating tilts during occultation, and considering the time
required for re-acquisition, each orbit is left with ~15 min of
exposure time, which is slightly more than what is needed to obtain
the minimum desired signal-to-noise on the faintest target. The
overhead time required for this program may seem high, however it is
important to consider that each visit is effectively observing two
independent astrophysical sources, therefore making it a one orbit per
source program.</ObservingDescription>
            
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            <CalibrationJustification />
            
            <AdditionalComments />
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      <Orbits
         ThisCycle2GyroPrimary="12"
         ThisCycle2GyroParallel="0"
         NextCycle2GyroPrimary="0"
         NextCycle2GyroParallel="0"
         AfterNext2GyroPrimary="0"
         AfterNext2GyroParallel="0" />
      
      <Phase1ProposalInformation
         TotalTargets="1"
         Attachment="/nfs/morgan/users/dieterich/hst.cycle20.dir/it.pdf">
         
         <ScientificCategory>COOL STARS</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="Atmospheres And Chromospheres" />
         
         <ScientificKeyword2
            Keyword="Detached Binaries" />
         
         <ScientificKeyword3
            Keyword="Main Sequence Stars" />
         
         <ScientificKeyword4
            Keyword="Stellar Evolution And Models" />
         
         <ScientificKeyword5
            Keyword="Very Low Mass Stars And Brown Dwarfs" />
         
         <ProprietaryPeriod>12</ProprietaryPeriod>
         
         <CalibProp>false</CalibProp>
         
         <ChandraCoord>0.0</ChandraCoord>
         
         <NOAONights>0.0</NOAONights>
         
         <Treasury>false</Treasury>
         
         <MultiCycleTreasury>false</MultiCycleTreasury>
         
         <Theory>false</Theory>
         
         <LargeProgram>false</LargeProgram>
      </Phase1ProposalInformation>
      
      <Phase2ProposalInformation
         PCFlag="false">
         
         <Availability>SUPPORTED</Availability>
      </Phase2ProposalInformation>
   </ProposalInformation>
   
   <Targets>
      
      <FixedTarget
         Name="GJ22AC"
         Number="1"
         ReferenceFrame="ICRS"
         RAPMValue="1738.21"
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-224.11"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000"
         AnnualParallax="0.09935"
         ProvisionalCoordinates="00 32 29.4000 +67 14 8.00">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>COMPOSITE SPECTRAL TYPE</Description>
            
            <Description>LOW MASS COMPANION</Description>
            
            <Description>M V-IV</Description>
         </PrimaryDescription>
         
         <Comments />
         
         <AlternateNames />
         
         <EquatorialPosition
            Value="00 32 29.4330 +67 14 8.41">
            
            <RAUnc
               Arcsec="0.1" />
            
            <DECUnc
               Arcsec="0.1" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <TargetConfirmationChartIsUpToDate />
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="10.5"
               MagnitudeUnc="0.04" />
            
            <OtherFluxes>R~9.6</OtherFluxes>
         </Fluxes>
      </FixedTarget>
      
      <FixedTarget
         Name="G250-29AB"
         Number="2"
         ReferenceFrame="ICRS"
         RAPMValue="495.89"
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-989.85"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000"
         AnnualParallax="0.09589"
         ProvisionalCoordinates="06 54 4.0000 +60 52 18.35">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>COMPOSITE SPECTRAL TYPE</Description>
            
            <Description>LOW MASS COMPANION</Description>
            
            <Description>M V-IV</Description>
         </PrimaryDescription>
         
         <Comments />
         
         <AlternateNames>
            
            <AlternateName>LHS221</AlternateName>
         </AlternateNames>
         
         <EquatorialPosition
            Value="06 54 4.2374 +60 52 18.36">
            
            <RAUnc
               Arcsec="0.1" />
            
            <DECUnc
               Arcsec="0.1" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <TargetConfirmationChartIsUpToDate />
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="10.95"
               MagnitudeUnc="0.03" />
            
            <OtherFluxes>R = 10.0, I = 9.2</OtherFluxes>
         </Fluxes>
      </FixedTarget>
      
      <FixedTarget
         Name="GJ1081AB"
         Number="3"
         ReferenceFrame="ICRS"
         RAPMValue="60"
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-360"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000"
         AnnualParallax="0.0652"
         ProvisionalCoordinates="05 33 19.1300 +44 48 58.80">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>COMPOSITE SPECTRAL TYPE</Description>
            
            <Description>LOW MASS COMPANION</Description>
            
            <Description>M V-IV</Description>
         </PrimaryDescription>
         
         <Comments />
         
         <AlternateNames />
         
         <EquatorialPosition
            Value="05 33 19.1300 +44 48 58.80">
            
            <RAUnc
               Arcsec="0.1" />
            
            <DECUnc
               Arcsec="0.1" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <TargetConfirmationChartIsUpToDate />
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="12.21"
               MagnitudeUnc="0.05" />
            
            <OtherFluxes>R=11.2, I=9.8</OtherFluxes>
         </Fluxes>
      </FixedTarget>
      
      <FixedTarget
         Name="GJ469AB"
         Number="4"
         ReferenceFrame="ICRS"
         RAPMValue="-632.02"
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-257.34"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000"
         AnnualParallax="0.07585"
         ProvisionalCoordinates="12 28 57.5800 +08 25 31.90">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>COMPOSITE SPECTRAL TYPE</Description>
            
            <Description>LOW MASS COMPANION</Description>
            
            <Description>M V-IV</Description>
         </PrimaryDescription>
         
         <Comments />
         
         <AlternateNames />
         
         <EquatorialPosition
            Value="12 28 57.5800 +08 25 31.87">
            
            <RAUnc
               Arcsec="0.1" />
            
            <DECUnc
               Arcsec="0.1" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <TargetConfirmationChartIsUpToDate />
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="12.06"
               MagnitudeUnc="0.05" />
            
            <OtherFluxes>R=10.86, I=9.32</OtherFluxes>
         </Fluxes>
      </FixedTarget>
      
      <FixedTarget
         Name="GJ234AB"
         Number="5"
         ReferenceFrame="ICRS"
         RAPMValue="705.28 "
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-611.92"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000"
         AnnualParallax="0.24232"
         ProvisionalCoordinates="06 29 24.0000 -02 48 0.00">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>COMPOSITE SPECTRAL TYPE</Description>
            
            <Description>LOW MASS COMPANION</Description>
            
            <Description>M V-IV</Description>
         </PrimaryDescription>
         
         <Comments />
         
         <AlternateNames />
         
         <EquatorialPosition
            Value="06 29 23.4070 -02 48 50.27">
            
            <RAUnc
               Arcsec="0.1" />
            
            <DECUnc
               Arcsec="0.1" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <TargetConfirmationChartIsUpToDate />
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="11.09"
               MagnitudeUnc="0.03" />
            
            <OtherFluxes>R=9.77, I=8.05</OtherFluxes>
         </Fluxes>
      </FixedTarget>
      
      <FixedTarget
         Name="GJ1245AC"
         Number="6"
         ReferenceFrame="ICRS"
         RAPMValue="397"
         RAPMUnits="MAS_PER_YEAR"
         DecPMValue="-482"
         DecPMUnits="MAS_PER_YEAR"
         Epoch="2000"
         AnnualParallax="0.220"
         ProvisionalCoordinates="19 53 54.9000 +44 24 54.00">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
         <PrimaryDescription>
            
            <Description>COMPOSITE SPECTRAL TYPE</Description>
            
            <Description>LOW MASS COMPANION</Description>
            
            <Description>M V-IV</Description>
         </PrimaryDescription>
         
         <Comments />
         
         <AlternateNames />
         
         <EquatorialPosition
            Value="19 53 54.4320 +44 24 54.15">
            
            <RAUnc
               Arcsec="0.1" />
            
            <DECUnc
               Arcsec="0.1" />
            
            <Equinox>J2000</Equinox>
         </EquatorialPosition>
         
         <Equinox>J2000</Equinox>
         
         <TargetConfirmationChartIsUpToDate />
         
         <Fluxes>
            
            <BroadBandMagnitude
               Band="V"
               Magnitude="13.41"
               MagnitudeUnc="0.03" />
            
            <OtherFluxes>R=11.1, I=9.78</OtherFluxes>
         </Fluxes>
      </FixedTarget>
   </Targets>
   
   <Observations>
      
      <Observation
         TargetName="GJ22AC"
         Instrument="STIS"
         Number="1"
         NumberOfOrbits="2"
         NumberOfIterations="1"
         TotalOrbits="2"
         PureParallel="false"
         CoordinatedParallel="false"
         TargetOfOpportunity="No"
         CVZ="false"
         Duplication="false">
         
         <Configurations>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>6768</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>7283</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>7795</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>8311</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>8825</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>9336</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>9851</Wavelength>
            </Configuration>
         </Configurations>
         
         <ObservationRequirements
            NoConstraints="false"
            Shadow="false"
            LowSky="false"
            SameOrient="false"
            ImprovedScheduling="true" />
         
         <AladinPhase1Requirements
            Detector="STIS/CCD"
            Aperture="1st-order"
            MosaicHeight=""
            MosaicWidth=""
            MosaicTileOverlap="10.0"
            AladinOrientationAngle="">
            
            <CoordinatedParallels />
            
            <AladinPhase1SubExposure0
               PrimaryPatternPosition="0"
               CopyNumber="0"
               IsDeleteAcceptable="false"
               PosTargX="0.0"
               PosTargY="0.0" />
         </AladinPhase1Requirements>
         
         <SuitabilityResults
            DaysHigh="0"
            DaysHighMed="0"
            DaysLowMed="0"
            DaysLow="0"
            OrbitsPerDay="0.0" />
      </Observation>
      
      <Observation
         TargetName="G250-29AB"
         Instrument="STIS"
         Number="2"
         NumberOfOrbits="2"
         NumberOfIterations="1"
         TotalOrbits="2"
         PureParallel="false"
         CoordinatedParallel="false"
         TargetOfOpportunity="No"
         CVZ="false"
         Duplication="false">
         
         <Configurations>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>6768</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>7283</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>7795</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>8311</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>8825</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>9336</Wavelength>
            </Configuration>
            
            <Configuration>
               
               <Config>STIS/CCD</Config>
               
               <ScienceMode>Spectroscopic</ScienceMode>
               
               <Coronography>No</Coronography>
               
               <Polarimetry>No</Polarimetry>
               
               <SpectralElement>G750M</SpectralElement>
               
               <Wavelength>9851</Wavelength>
            </Configuration>
         </Configurations>
         
         <ObservationRequirements
            NoConstraints="true" />
         
         <AladinPhase1Requirements
            Detector="STIS/CCD"
            Aperture="1st-order"
            MosaicHeight=""
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   <Datasets />
   
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                        <String>The scheduling data was generated by CASM 20.2.</String>
                        
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         <Comments>Note from PI (Sergio Dieterich, dieterich@chara.gsu.edu)

The purpose of this observation is to obtain simultaneous long slit spectroscopy for both components of a binary star by aligning the binary's
separation axis to the STIS long slit.  The binary's position angle moves 25 degrees during cycle 20. I have used the visit planer to select the 
ORIENT/date combination that seems easier to schedule, but any combination meeting the following table will acheieve the science.
Feel free to change ORIENT and date to any other match in the table if it makes life easier.
In the table, ORIENT1 and ORIENT2 are different by 180 degrees.

PLEASE MAKE SURE THE ORIENT AT THE TIME OF OBSERVATION IS WITHIN THE +- TOLERANCE LISTED IN THE LAST COLUMN. 


#   YEAR    MONTH     DAY    SEPARATION ORIENT1    ORIENT2    ORIENT_TOLERANCE
    2012    AUG      10      0.523      220.5      40.5       5.45
    2012    AUG      22      0.522      221.0      41.0       5.46
    2012    SEP       2      0.521      221.5      41.5       5.47
    2012    SEP      14      0.520      222.0      42.0       5.48
    2012    SEP      26      0.519      222.5      42.5       5.50
    2012    OCT       7      0.518      223.0      43.0       5.51
    2012    OCT      19      0.516      223.5      43.5       5.52
    2012    OCT      30      0.515      224.0      44.0       5.53
    2012    NOV      11      0.514      224.5      44.5       5.54
    2012    NOV      22      0.513      225.0      45.0       5.56
    2012    DEC       4      0.512      225.5      45.5       5.57
    2012    DEC      15      0.510      226.0      46.0       5.59
    2012    DEC      27      0.509      226.5      46.5       5.60
    2013    JAN       7      0.507      227.0      47.0       5.62
    2013    JAN      18      0.506      227.5      47.5       5.63
    2013    JAN      30      0.504      228.1      48.1       5.65
    2013    FEB      10      0.503      228.6      48.6       5.67
    2013    FEB      22      0.501      229.1      49.1       5.68
    2013    MAR       6      0.500      229.6      49.6       5.70
    2013    MAR      17      0.498      230.2      50.2       5.72
    2013    MAR      29      0.496      230.7      50.7       5.74
    2013    APR       9      0.495      231.3      51.3       5.76
    2013    APR      21      0.493      231.8      51.8       5.78
    2013    MAY       2      0.491      232.3      52.3       5.80
    2013    MAY      14      0.489      232.9      52.9       5.82
    2013    MAY      25      0.487      233.5      53.5       5.85
    2013    JUN       6      0.485      234.0      54.0       5.87
    2013    JUN      17      0.484      234.6      54.6       5.89
    2013    JUN      29      0.482      235.2      55.2       5.92
    2013    JUL      10      0.480      235.7      55.7       5.94
    2013    JUL      22      0.477      236.3      56.3       5.97
    2013    AUG       2      0.475      236.9      56.9       5.99
    2013    AUG      14      0.473      237.5      57.5       6.02
    2013    AUG      25      0.471      238.1      58.1       6.05
    2013    SEP       6      0.469      238.7      58.7       6.08
    2013    SEP      17      0.467      239.3      59.3       6.11
    2013    SEP      29      0.464      239.9      59.9       6.13
    2013    OCT      10      0.462      240.5      60.5       6.17
    2013    OCT      22      0.460      241.2      61.2       6.20
    2013    NOV       2      0.457      241.8      61.8       6.23
    2013    NOV      14      0.455      242.4      62.4       6.26
    2013    NOV      25      0.452      243.1      63.1       6.29
    2013    DEC       7      0.450      243.7      63.7       6.33
    2013    DEC      18      0.447      244.4      64.4       6.36
    2013    DEC      30      0.445      245.0      65.0       6.40

orient1 range 220 to 245
orient2 range 40  to 65</Comments>
         
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            </SubExposures>
         </Exposure>
         
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            Label="tilt 2 flat"
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            TimePerExposure="DEF"
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         </Exposure>
         
         <Exposure
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            Label="GJ22AC tilt 3"
            TargetName="GJ22AC"
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            Opmode="ACCUM"
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            SpElement="G750M"
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            Label="tilt 3 flat"
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         <Exposure
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            Label="GJ22AC tilt 4"
            TargetName="GJ22AC"
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            SpElement="G750M"
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         <Exposure
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            Label="tilt 4 flat"
            TargetName="CCDFLAT"
            Config="STIS/CCD"
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         <Exposure
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            Label="GJ22AC tilt 5"
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            Wavelength="8825"
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            Label="GJ22AC tilt 6"
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            Label="tilt 6 flat"
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            Config="STIS/CCD"
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            Label="GJ22AC tilt 7"
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                  ActualTime="160.5"
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      </Visit>
      
      <Visit
         Number="02"
         Label="G250-29AB"
         After=""
         Before="">
         
         <ToolData>
            
            <ToolDataItem
               Key="OpTimeStamp">
               
               <OpToolDataDate>
                  
                  <Time>1341947646220</Time>
               </OpToolDataDate>
            </ToolDataItem>
            
            <ToolDataItem
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               <OpToolDataString>
                  
                  <Value>/tmp/OPVisit2346853499052041831.xml</Value>
               </OpToolDataString>
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            <ToolDataItem
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               <VpVisitData>
                  
                  <StVisitSchedulingWindows
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                     UpToDate="true"
                     StSchedulingPCF="1343606400000 0.0 1358208000000 1.0 1358769599000 0.0 1396396800000">
                     
                     <StConstraintSchedulingWindows
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                        StSchedulingPCF="1343606400000 0.0 1356998400000 1.0 1359676800000 0.0 1396396800000" />
                     
                     <StConstraintSchedulingWindows
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                     <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
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                     Label="Roll Ranges Report"
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         <Comments>Note from PI (Sergio Dieterich, dieterich@chara.gsu.edu)

The purpose of this observation is to obtain simultaneous long slit spectroscopy for both components of a binary star by aligning the binary's
separation axis to the STIS long slit.  The binary's position angle moves ~9 degrees during cycle 20. I have used the visit planer to select the 
ORIENT/date combination that seems easier to schedule, but any combination meeting the following table will acheieve the science.
Feel free to change ORIENT and date to any other match in the table if it makes life easier.
In the table, ORIENT1 and ORIENT2 are different by 180 degrees.

PLEASE MAKE SURE THE ORIENT AT THE TIME OF OBSERVATION IS WITHIN THE +- TOLERANCE LISTED IN THE LAST COLUMN. 

#   YEAR    MONTH     DAY  SEPARATION  ORIENT1     ORIENT2   ORIENT_TOLERANCE
    2012    AUG       9      0.517      323.4      143.4       5.5
    2012    AUG      19      0.517      323.2      143.2       5.5
    2012    AUG      29      0.517      323.1      143.1       5.5
    2012    SEP       8      0.517      322.9      142.9       5.5
    2012    SEP      18      0.517      322.8      142.8       5.5
    2012    SEP      28      0.517      322.6      142.6       5.5
    2012    OCT       8      0.517      322.5      142.5       5.5
    2012    OCT      18      0.517      322.3      142.3       5.5
    2012    OCT      28      0.517      322.2      142.2       5.5
    2012    NOV       7      0.517      322.0      142.0       5.5
    2012    NOV      17      0.516      321.8      141.8       5.5
    2012    NOV      27      0.516      321.7      141.7       5.5
    2012    DEC       7      0.516      321.5      141.5       5.5
    2012    DEC      16      0.515      321.4      141.4       5.5
    2012    DEC      26      0.515      321.2      141.2       5.5
    2013    JAN       6      0.515      321.1      141.1       5.5
    2013    JAN      16      0.514      320.9      140.9       5.5
    2013    JAN      25      0.514      320.7      140.7       5.5
    2013    FEB       4      0.513      320.6      140.6       5.5
    2013    FEB      14      0.513      320.4      140.4       5.5
    2013    FEB      24      0.512      320.3      140.3       5.5
    2013    MAR       6      0.512      320.1      140.1       5.5
    2013    MAR      16      0.511      320.0      140.0       5.5
    2013    MAR      26      0.511      319.8      139.8       5.5
    2013    APR       5      0.510      319.6      139.6       5.5
    2013    APR      15      0.509      319.5      139.5       5.6
    2013    APR      25      0.509      319.3      139.3       5.6
    2013    MAY       5      0.508      319.2      139.2       5.6
    2013    MAY      15      0.507      319.0      139.0       5.6
    2013    MAY      25      0.506      318.8      138.8       5.6
    2013    JUN       4      0.506      318.7      138.7       5.6
    2013    JUN      13      0.505      318.5      138.5       5.6
    2013    JUN      23      0.504      318.3      138.3       5.6
    2013    JUL       3      0.503      318.2      138.2       5.6
    2013    JUL      13      0.502      318.0      138.0       5.6
    2013    JUL      23      0.501      317.8      137.8       5.6
    2013    AUG       2      0.500      317.7      137.7       5.7
    2013    AUG      12      0.499      317.5      137.5       5.7
    2013    AUG      22      0.498      317.3      137.3       5.7
    2013    SEP       1      0.497      317.2      137.2       5.7
    2013    SEP      11      0.496      317.0      137.0       5.7
    2013    SEP      21      0.495      316.8      136.8       5.7
    2013    OCT       1      0.494      316.7      136.7       5.7
    2013    OCT      11      0.493      316.5      136.5       5.7
    2013    OCT      21      0.492      316.3      136.3       5.8
    2013    OCT      31      0.490      316.2      136.2       5.8
    2013    NOV       9      0.489      316.0      136.0       5.8
    2013    NOV      19      0.488      315.8      135.8       5.8
    2013    NOV      30      0.487      315.6      135.6       5.8
    2013    DEC       9      0.485      315.5      135.5       5.8
    2013    DEC      19      0.484      315.3      135.3       5.8
    2013    DEC      29      0.483      315.1      135.1       5.9

orient1 range 315 to 323
orient2 range 135 to 143</Comments>
         
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         <Exposure
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            Label="G250-29AB tilt 6"
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            Label="G250-29AB tilt 7"
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         <Exposure
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      </Visit>
      
      <Visit
         Number="03"
         Label="GJ234AB"
         After=""
         Before="">
         
         <ToolData>
            
            <ToolDataItem
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               <OpToolDataDate>
                  
                  <Time>1341948493056</Time>
               </OpToolDataDate>
            </ToolDataItem>
            
            <ToolDataItem
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               <OpToolDataString>
                  
                  <Value>/tmp/OPVisit8928777793026199025.xml</Value>
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            <ToolDataItem
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               <VpVisitData>
                  
                  <StVisitSchedulingWindows
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                     <StConstraintSchedulingWindows
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                     <StConstraintSchedulingWindows
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                     <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>
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                  <AncillaryData
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         <Comments>Note from PI (Sergio Dieterich, dieterich@chara.gsu.edu)

The purpose of this observation is to obtain simultaneous long slit spectroscopy for both components of a binary star by aligning the binary's
separation axis to the STIS long slit.  The binary's position angle moves ~9 degrees during cycle 20. I have used the visit planer to select the 
ORIENT/date combination that seems easier to schedule, but any combination meeting the following table will acheieve the science.
Feel free to change ORIENT and date to any other match in the table if it makes life easier.
In the table, ORIENT1 and ORIENT2 are different by 180 degrees.

PLEASE MAKE SURE THE ORIENT AT THE TIME OF OBSERVATION IS WITHIN THE +- TOLERANCE LISTED IN THE LAST COLUMN. 

#   YEAR    MONTH    DAY  SEPARATION  ORIENT1   ORIENT2  ORIENT_TOLERANCE
    2012    AUG       9      0.71      203.7      23.7       4.0
    2012    AUG      20      0.71      204.6      24.6       4.0
    2012    SEP       1      0.71      205.6      25.6       3.9
    2012    SEP      13      0.71      206.5      26.5       3.9
    2012    SEP      25      0.71      207.4      27.4       3.9
    2012    OCT       6      0.71      208.3      28.3       3.9
    2012    OCT      18      0.72      209.2      29.2       3.9
    2012    OCT      30      0.72      210.1      30.1       3.9
    2012    NOV      11      0.72      211.0      31.0       3.9
    2012    NOV      23      0.72      211.9      31.9       3.9
    2012    DEC       5      0.72      212.8      32.8       3.9
    2012    DEC      16      0.72      213.6      33.6       3.9
    2012    DEC      28      0.73      214.5      34.5       3.9
    2013    JAN       9      0.73      215.4      35.4       3.9
    2013    JAN      21      0.73      216.3      36.3       3.8
    2013    FEB       2      0.73      217.1      37.1       3.8
    2013    FEB      13      0.73      218.0      38.0       3.8
    2013    FEB      25      0.74      218.8      38.8       3.8
    2013    MAR       9      0.74      219.7      39.7       3.8
    2013    MAR      21      0.74      220.5      40.5       3.8
    2013    APR       2      0.74      221.4      41.4       3.8
    2013    APR      13      0.74      222.2      42.2       3.8
    2013    APR      25      0.74      223.1      43.1       3.8
    2013    MAY       7      0.75      223.9      43.9       3.8
    2013    MAY      19      0.75      224.7      44.7       3.8
    2013    MAY      31      0.75      225.6      45.6       3.7
    2013    JUN      12      0.75      226.4      46.4       3.7
    2013    JUN      23      0.75      227.2      47.2       3.7
    2013    JUL       5      0.75      228.0      48.0       3.7
    2013    JUL      17      0.75      228.8      48.8       3.7
    2013    JUL      29      0.76      229.6      49.6       3.7
    2013    AUG      10      0.76      230.5      50.5       3.7
    2013    AUG      21      0.76      231.3      51.3       3.7
    2013    SEP       2      0.76      232.1      52.1       3.7
    2013    SEP      14      0.76      232.9      52.9       3.7
    2013    SEP      26      0.76      233.7      53.7       3.7
    2013    OCT       7      0.76      234.5      54.5       3.7
    2013    OCT      20      0.76      235.3      55.3       3.7
    2013    OCT      31      0.76      236.1      56.1       3.7
    2013    NOV      12      0.76      236.9      56.9       3.7
    2013    NOV      24      0.76      237.7      57.7       3.7
    2013    DEC       6      0.76      238.5      58.5       3.7
    2013    DEC      17      0.76      239.3      59.3       3.7
    2013    DEC      29      0.76      240.1      60.1       3.7</Comments>
         
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         <Comments>Note from PI (Sergio Dieterich, dieterich@chara.gsu.edu)

The purpose of this observation is to obtain simultaneous long slit spectroscopy for both components of a binary star by aligning the binary's
separation axis to the STIS long slit.  The binary's position angle moves ~34 degrees during cycle 20. I have used the visit planer to select the ORIENT/date combination that seems easier to schedule, but any combination meeting the following table will acheieve the science.
Feel free to change ORIENT and date  to any other match in the table if it makes life easier.
In the table, ORIENT1 and ORIENT2 are different by 180 degrees.

PLEASE MAKE SURE THE ORIENT AT THE TIME OF OBSERVATION IS WITHIN THE +- TOLERANCE LISTED IN THE LAST COLUMN. 


#   YEAR    MONTH     DAY  SEPARATION  ORIENT1  ORIENT2    PA_TOLERANCE
    2012    AUG       2      0.681      41.0      221.0       4.1
    2012    AUG      14      0.678      40.3      220.3       4.2
    2012    AUG      26      0.676      39.5      219.5       4.2
    2012    SEP       8      0.673      38.8      218.8       4.2
    2012    SEP      21      0.671      38.1      218.1       4.2
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         <Comments>Note from PI (Sergio Dieterich, dieterich@chara.gsu.edu)

The purpose of this observation is to obtain simultaneous long slit spectroscopy for both components of a binary star by aligning the binary's
separation axis to the STIS long slit.  The binary's position angle moves during cycle 20. I have used the visit planer to select the ORIENT/date combination that seems easier to schedule, but any combination meeting the following table will acheieve the science.
Feel free to change ORIENT and date  to any other match in the table if it makes life easier.
In the table, ORIENT1 and ORIENT2 are different by 180 degrees.

PLEASE MAKE SURE THE ORIENT AT THE TIME OF OBSERVATION IS WITHIN THE +- TOLERANCE LISTED IN THE LAST COLUMN.

#   YEAR    MONTH    DAY SEPARATION    ORIENT1    ORIENT2     PA_TOLERANCE
    2012    OCT       7      0.12      77.64      257.6       22.0
    2012    OCT      15      0.12      77.43      257.4       22.3
    2012    OCT      23      0.11      77.22      257.2       22.6
    2012    OCT      31      0.11      76.99      256.9       23.0
    2012    NOV       9      0.11      76.76      256.7       23.3
    2012    NOV      17      0.11      76.53      256.5       23.7
    2012    NOV      25      0.11      76.28      256.2       24.0
    2012    DEC       3      0.10      76.03      256.0       24.4
    2012    DEC      11      0.10      75.76      255.7       24.8
    2012    DEC      19      0.10      75.49      255.4       25.2
    2012    DEC      27      0.10      75.20      255.2       25.6
    2013    JAN       4      0.10      74.91      254.9       26.0
    2013    JAN      13      0.10      74.60      254.6       26.5
    2013    JAN      21     0.098      74.28      254.2       26.9
    2013    JAN      29     0.096      73.95      253.9       27.4
    2013    FEB       6     0.094      73.61      253.6       27.9
    2013    FEB      14     0.092      73.25      253.2       28.4
    2013    FEB      22     0.090      72.87      252.8       28.9
    2013    MAR       2     0.088      72.48      252.4       29.5
    2013    MAR      10     0.086      72.07      252.0       30.0
    2013    MAR      18     0.084      71.63      251.6       30.6
    2013    MAR      26     0.082      71.18      251.1       31.2
    2013    APR       3     0.080      70.70      250.7       31.9
    2013    APR      12     0.078      70.20      250.2       32.5
    2013    APR      20     0.076      69.68      249.6       33.2
    2013    APR      28     0.074      69.12      249.1       33.9
    2013    MAY       6     0.072      68.54      248.5       34.6
    2013    MAY      14     0.070      67.92      247.9       35.4
    2013    MAY      22     0.068      67.27      247.2       36.2
    2013    MAY      30     0.066      66.57      246.5       37.0
    2013    JUN       7     0.064      65.83      245.8       37.9
    2013    JUN      15     0.062      65.05      245.0       38.8
    2013    JUN      23     0.060      64.21      244.2       39.7
    2013    JUL       1     0.058      63.31      243.3       40.6
    2013    JUL       9     0.056      62.36      242.3       41.6
    2013    JUL      18     0.054      61.32      241.3       42.7
    2013    JUL      26     0.052      60.22      240.2       43.7
    2013    AUG       3     0.050      59.02      239.0       44.8
    2013    AUG      11     0.048      57.73      237.7       45.9
    2013    AUG      19     0.046      56.33      236.3       47.1
    2013    AUG      27     0.044      54.80      234.8       48.3
    2013    SEP       4     0.042      53.16      233.1       49.5
    2013    SEP      12     0.040      51.34      231.3       50.7
    2013    SEP      21     0.038      49.38      229.3       52.0
    2013    SEP      29     0.037      47.21      227.2       53.3
    2013    OCT       7     0.035      44.83      224.8       54.6
    2013    OCT      15     0.033      42.22      222.2       55.9
    2013    OCT      23     0.032      39.36      219.3       57.1
    2013    OCT      31     0.030      36.19      216.1       58.3
    2013    NOV       8     0.029      32.71      212.7       59.5
    2013    NOV      16     0.028      28.91      208.9       60.6
    2013    NOV      24     0.026      24.76      204.7       61.7
    2013    DEC       2     0.025      20.25      200.2       62.6
    2013    DEC      11     0.025      15.40      195.4       63.3
    2013    DEC      19     0.024      10.27      190.2       64.0
    2013    DEC      27     0.023      4.884      184.8       64.4</Comments>
         
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      </Visit>
      
      <Visit
         Number="06"
         Label="GJ469AB"
         Schedulability="100"
         After=""
         Before="">
         
         <ToolData>
            
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               <OpToolDataDate>
                  
                  <Time>1341950388052</Time>
               </OpToolDataDate>
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                  <StVisitSchedulingWindows
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                     <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>
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                  </StVisitSchedulingWindows>
                  
                  <AncillaryData
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         <Comments>Note from PI (Sergio Dieterich, dieterich@chara.gsu.edu)

The purpose of this observation is to obtain simultaneous long slit spectroscopy for both components of a binary star by aligning the binary's
separation axis to the STIS long slit.  The binary's position angle moves during cycle 20. I have used the visit planer to select the ORIENT/date combination that seems easier to schedule, but any combination meeting the following table will acheieve the science.
Feel free to change ORIENT and date  to any other match in the table if it makes life easier.
In the table, ORIENT1 and ORIENT2 are different by 180 degrees.

PLEASE MAKE SURE THE ORIENT AT THE TIME OF OBSERVATION IS WITHIN THE +- TOLERANCE LISTED IN THE LAST COLUMN.

#   YEAR  MONTH   DAY SEP"      ORIENT1   ORIENT2    ORIENT_TOLERANCE
    2012    AUG       5      0.208      25.4     205.4       13.49
    2012    AUG      14      0.206      24.9     204.9       13.60
    2012    AUG      22      0.204      24.4     204.4       13.72
    2012    AUG      31      0.202      24.0     204.0       13.84
    2012    SEP       8      0.201      23.4     203.4       13.96
    2012    SEP      17      0.199      22.9     202.9       14.08
    2012    SEP      26      0.197      22.4     202.4       14.20
    2012    OCT       4      0.195      21.9     201.9       14.33
    2012    OCT      12      0.193      21.3     201.3       14.46
    2012    OCT      21      0.191      20.8     200.8       14.59
    2012    OCT      30      0.190      20.2     200.2       14.73
    2012    NOV       7      0.188      19.6     199.6       14.86
    2012    NOV      15      0.186      19.0     199.0       15.00
    2012    NOV      24      0.184      18.5     198.5       15.14
    2012    DEC       3      0.182      17.8     197.8       15.28
    2012    DEC      11      0.181      17.2     197.2       15.43
    2012    DEC      19      0.179      16.6     196.6       15.57
    2012    DEC      28      0.177      15.9     195.9       15.72
    2013    JAN       6      0.175      15.3     195.3       15.87
    2013    JAN      14      0.174      14.6     194.6       16.02
    2013    JAN      22      0.172      13.9     193.9       16.18
    2013    JAN      31      0.170      13.2     193.2       16.33
    2013    FEB       9      0.168      12.5     192.5       16.49
    2013    FEB      17      0.167      11.8     191.8       16.65
    2013    FEB      25      0.165      11.0     191.0       16.81
    2013    MAR       6      0.163      10.3     190.3       16.97
    2013    MAR      15      0.162      9.53     189.5       17.14
    2013    MAR      23      0.160      8.74     188.7       17.30
    2013    APR       1      0.158      7.93     187.9       17.47
    2013    APR       9      0.157      7.11     187.1       17.63
    2013    APR      18      0.155      6.26     186.2       17.80
    2013    APR      26      0.154      5.40     185.4       17.97
    2013    MAY       5      0.152      4.53     184.5       18.14
    2013    MAY      13      0.151      3.63     183.6       18.31
    2013    MAY      22      0.149      2.72     182.7       18.48
    2013    MAY      30      0.148      1.79     181.7       18.65
    2013    JUN       8      0.146      0.84     180.8       18.82
    2013    JUN      16      0.145    359.87     179.8       18.98
    2013    JUN      25      0.143    358.89     178.8       19.15
    2013    JUL       3      0.142    357.88     177.8       19.32
    2013    JUL      12      0.141    356.86     176.8       19.48
    2013    JUL      20      0.140    355.82     175.8       19.64
    2013    JUL      29      0.138    354.76     174.7       19.81
    2013    AUG       6      0.137    353.68     173.6       19.96
    2013    AUG      15      0.136    352.59     172.5       20.12
    2013    AUG      23      0.135    351.47     171.4       20.27
    2013    SEP       1      0.134    350.33     170.3       20.42
    2013    SEP       9      0.133    349.18     169.1       20.56
    2013    SEP      18      0.132    348.01     168.0       20.70
    2013    SEP      27      0.131    346.83     166.8       20.83
    2013    OCT       5      0.130    345.62     165.6       20.96
    2013    OCT      13      0.129    344.40     164.4       21.09
    2013    OCT      22      0.128    343.17     163.1       21.20
    2013    OCT      31      0.128    341.92     161.9       21.32
    2013    NOV       8      0.127    340.66     160.6       21.42
    2013    NOV      16      0.126    339.38     159.3       21.52
    2013    NOV      25      0.126    338.09     158.0       21.61
    2013    DEC       4      0.125    336.79     156.7       21.69
    2013    DEC      12      0.125    335.48     155.4       21.76
    2013    DEC      20      0.124    334.16     154.1       21.82
    2013    DEC      29      0.124    332.83     152.8       21.88</Comments>
         
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