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<HSTProposal
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   Phase2ID="10891"
   Phase="Phase II"
   AptVersion="Version 15.2.2 ">
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            SubmissionCounter="2"
            SubmissionSuccessCounter="1"
            HasErrors="false"
            Cycle="15"
            IncludeSysInfo="true"
            NotificationAddress="nevans@cfa.harvard.edu"
            AssignedID="10891">
            
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            <SubmissionComments>In this revision we have adopted 0.3 sec for all of the exposures on Polaris A, based on the observations obtained in
August 2005.  We have also added a series of dithered 20-sec observations of the wide companion Polaris B, 
placed at the same location in the FOV as the observations of Polaris A, in order to determine an accurate PSF from
a single star exposed to the same level as Polaris A.</SubmissionComments>
            
            <SubmissionLog>    ----- Submission 1 (Tue May 09 02:53:30 GMT 2006) -----
  Phase II Proposal 10891 (10891) successfully submitted.


----- Submission 2 (Fri Jun 09 21:46:38 GMT 2006) -----
</SubmissionLog>
            
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   <ProposalInformation
      Category="GO"
      PureParallelProposal="false"
      Cycle="15">
      
      <Title>The Dynamical Mass of the Bright Cepheid Polaris</Title>
      
      <Abstract>Cepheid variables are of central importance in Galactic and extragalactic astronomy. They are the primary standard candles for measuring extragalactic distances, and they provide critical tests of stellar-evolution theory. Surprisingly, however, until now there was not a single Cepheid with a purely dynamical measurement of its mass.

Polaris (alpha UMi) is the nearest and brightest of all Cepheids. It offers the unique opportunity to measure the dynamical mass of a Cepheid, because it is in a binary system for which a single-lined spectroscopic orbit is already available. In Cycle 14, we resolved the system in the UV using ACS/HRC, thus providing the first direct detection of the companion, as well as a first approximation to the dynamical mass. In the present proposal we request one HST orbit per year for the next 3 Cycles, in order to refine the visual orbit. Combined with the HST/FGS parallax (see below), this program will provide an accurate mass for the Cepheid (the error should be about 0.5 Msun by Cycle 17), and the only one based purely on dynamical information.  Only HST's combination of high spatial resolution and UV sensitivity can achieve this result. 

The parallax is a key ingredient in the mass determination. In an ongoing multi-year program (GO-9888, GO-10113, GO-10482), we are using the FGS to improve significantly upon the Hipparcos parallax of Polaris.  The continued ACS imaging proposed here will thus provide extremely valuable astrophysical information from a very modest additional investment of observing time.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Nancy"
         MiddleInitial="R."
         LastName="Evans"
         ESAMember="false"
         UniqueID="631"
         AddressVerifiedCycle="15">
         
         <Address
            Institution="Smithsonian Institution Astrophysical Observatory"
            USState="MA"
            Country="USA" />
      </PrincipalInvestigator>
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Howard"
         MiddleInitial="E."
         LastName="Bond"
         ESAMember="false"
         UniqueID="2894"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="15">
         
         <Address
            Institution="Space Telescope Science Institute"
            USState="MD"
            Country="USA" />
      </CoInvestigator>
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Giuseppe"
         LastName="Bono"
         ESAMember="true"
         UniqueID="5732"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="15">
         
         <Address
            Institution="INAF, Osservatorio Astronomico di Roma"
            Country="Italy" />
      </CoInvestigator>
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Margarita"
         LastName="Karovska"
         ESAMember="false"
         UniqueID="1079"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="15">
         
         <Address
            Institution="Smithsonian Institution Astrophysical Observatory"
            USState="MA"
            Country="USA" />
      </CoInvestigator>
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Edmund"
         LastName="Nelan"
         ESAMember="false"
         UniqueID="3260"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="15">
         
         <Address
            Institution="Space Telescope Science Institute"
            USState="MD"
            Country="USA" />
      </CoInvestigator>
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Dimitar"
         MiddleInitial="D."
         LastName="Sasselov"
         ESAMember="false"
         UniqueID="2271"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="15">
         
         <Address
            Institution="Harvard University"
            USState="MA"
            Country="USA" />
      </CoInvestigator>
      
      <CoInvestigator
         Honorific="Dr."
         FirstName="Gail"
         LastName="Schaefer"
         ESAMember="false"
         UniqueID="6641"
         AdminUSPI="false"
         Contact="false">
         
         <Address
            Institution="Space Telescope Science Institute"
            USState="MD"
            Country="USA" />
      </CoInvestigator>
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>The observations with ACS/HRC will consist of a series of 0.3-sec exposures in F220W, with dithering to improve the astrometric accuracy.  At each of 4 dither positions we will obtain 5x0.3 sec exposures, for a grand total of 20 frames. The aim is to resolve the close companion of Polaris, and measure the separation and position angle.  The target will be positioned in the HRC field of view so as to also show the wide companion, Polaris B, which will serve as a check on the position angle measurement.  

We will then move the telescope so as to place the companion Polaris B at the SAME set of 4 dither positions used for Polaris A. At each of the 4 positions we will take 4x20 sec, for a grand total of 16 frames. The purpose of these exposures is for Polaris B to provide a PSF of a single star at the same positions in the field of view used for the very close binary Polaris A, and exposed to the same count level as for Polaris A (since the flux ratio between B and A is 0.015).</ObservingDescription>
            
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            <AdditionalComments />
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         TotalTargets="1"
         Attachment="/klingsor/data1/bond/hstcycle14/polaris/polarispro.pdf">
         
         <ScientificCategory>COOL STARS</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="ASTROMETRY" />
         
         <ScientificKeyword2
            Keyword="COSMOLOGICAL PARAMETERS AND DISTANCE SCALE" />
         
         <ScientificKeyword3
            Keyword="DETACHED BINARIES" />
         
         <ScientificKeyword4
            Keyword="STELLAR EVOLUTION AND MODELS" />
         
         <ScientificKeyword5
            Keyword="VARIABLE AND PULSATING STARS" />
         
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         <Legacy>false</Legacy>
         
         <Theory>false</Theory>
         
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            <Description>F3-F9</Description>
            
            <Description>CEPHEID</Description>
            
            <Description>PULSATING VARIABLE</Description>
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            <Equinox>J2000</Equinox>
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         <ProvisionalDEC>+89 16 0.00</ProvisionalDEC>
         
         <Equinox>J2000</Equinox>
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         ReferenceFrame="ICRS"
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         Epoch="1991.25"
         AnnualParallax="0.00756">
         
         <PrimaryCategory>STAR</PrimaryCategory>
         
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            <Description>F3-F9</Description>
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         <Comments>These coordinates will place Polaris B at the same location in the FOV as Polaris A, as desired.</Comments>
         
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            <AlternateName>ALPHA-UMI-B</AlternateName>
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            <Equinox>J2000</Equinox>
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         <ProvisionalDEC>+00 00 0.00</ProvisionalDEC>
         
         <Equinox>J2000</Equinox>
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               <Config>ACS/HRC</Config>
               
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