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<HSTProposal
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   Phase2ID="11166"
   Phase="Phase II"
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   <!--Date: Wed Nov 25 11:50:15 GMT 2009-->
   
   <ProposalInformation
      Category="GO"
      PureParallelProposal="false"
      Cycle="16"
      STScIEditNumber="3">
      
      <Title>The Mass-dependent Evolution of the Black Hole-Bulge Relations</Title>
      
      <Abstract>In the local universe, the masses of giant black holes  are correlated with the luminosities, masses and velocity dispersions of their host galaxy bulges. This indicates a surprisingly close connection between the evolution of galactic nuclei (on parsec scales) and of stars on kpc scales. A key observational test of proposed explanations for these correlations is to measure how they have evolved over cosmic time. Our ACS imaging of 20 Seyfert 1 galaxies at z=0.37 showed them to have smaller bulges (by a factor of 3) for a given central black hole mass than is found in galaxies in the present-day universe. However, since all our sample galaxies had black hole masses in the range 10^8.0--8.5 Msun, we could only measure the OFFSET in black hole mass to bulge luminosity ratios from the present epoch. By extending this study to black hole masses another factor of 10 lower, we propose to determine the full CORRELATION of black hole mass with host galaxy properties at a lookback time of 4 Gyrs and to test mass-dependency of the evolution. We have selected 14 Seyfert galaxies from SDSS DR5 whose narrow Hbeta emission lines (and estimated nuclear luminosities) imply that they have black hole masses around 10^7 Msuns. We will soon complete our Keck spectroscopic measures of their bulge velocity dispersions.  We need a 1-orbit NICMOS image of each galaxy to separate its nonstellar luminosity from its bulge and disk. This will allow us to make the first determination of the full black hole/bulge relations at z=0.37 (e.g. M-L and M-sigma), as well as a test of whether active galaxies obey the Fundamental Plane relation at that epoch.</Abstract>
      
      <PrincipalInvestigator
         Honorific="Dr."
         FirstName="Jong-Hak"
         LastName="Woo"
         ESAMember="false"
         UniqueID="7147"
         AddressVerifiedCycle="16">
         
         <Address
            Institution="University of California - Santa Barbara"
            USState="CA"
            Country="USA" />
      </PrincipalInvestigator>
      
      <CoInvestigator
         Honorific="Prof."
         FirstName="Tommaso"
         MiddleInitial="L."
         LastName="Treu"
         ESAMember="false"
         UniqueID="7250"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="17">
         
         <Address
            Institution="University of California - Santa Barbara"
            USState="CA"
            Country="USA" />
      </CoInvestigator>
      
      <CoInvestigator
         Honorific="Prof."
         FirstName="Matthew"
         MiddleInitial="A."
         LastName="Malkan"
         ESAMember="false"
         UniqueID="1761"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="17">
         
         <Address
            Institution="University of California - Los Angeles"
            USState="CA"
            Country="USA" />
      </CoInvestigator>
      
      <CoInvestigator
         Honorific="Prof."
         FirstName="Roger"
         MiddleInitial="D."
         LastName="Blandford"
         ESAMember="false"
         UniqueID="217"
         AdminUSPI="false"
         Contact="false"
         AddressVerifiedCycle="17">
         
         <Address
            Institution="Stanford University"
            USState="CA"
            Country="USA" />
      </CoInvestigator>
      
      <Questions>
         
         <Phase2Questions>
            
            <ObservingDescription>Our goal is to obtain high resolution photometry of a sample of 14
Seyfert 1 galaxies at z=0.37+-0.01 for which central black hole masses and
bulge velocity dispersions are obtained from the ground. We need to
determine the luminosity of the bulge and of the central point source,
in order to extend our measurement of the M-L and M-sigma
relationships down to black hole mass ~10^7 solar mass.
We aim for uncertainties on the photometric quantities smaller than
0.2 dex, i.e. small with respect to the intrinsic uncertainty on the virial black 
hole mass estimates (0.4 dex). In addition, we will also derive effective radii
(Re) and effective surface brightnesses (SBe) for the bulges, in order to 
derive their dynamical masses (sigma^2 Re) and probe the evolution of relationships
involving more than one variable.   

Strategy

The following strategy is based on our previous successful experience (Cycle 13).

Camera. NIC-2 on NICMOS is the camera of choice, providing
superior sensitivity to the NIC-1 camera at the low surface brightness
levels needed to do bulge/disk decomposition, and better PSF sampling
than NIC-3. PSF sampling will be further improved by obtaining
dithered exposures with semi-integer pixel offsets (4 positions per
pixel). This will also enable robust cosmic ray/defects removal. Note
that the contrast between the central point source and the host galaxy
in our sample is far more favorable than in other HST studies of QSOs
hosts, where the AGN typically outshines the galaxy by a factor of 10
or more. Furthermore going to longer wavelength improves the contrast,
since the host is redder than the nucleus. Therefore, in our case the
modelling of the wings of the PSF is not nearly as crucial to obtain
accurate parameters for the host galaxy. The residual PSF related
uncertainties are estimated as described below.

Filter. To minimize the size of the PSF, and preserving high
sensitivity, we select the F110W filter. This filter is close in
wavelength to the rest frame 5100\AA\ continuum -- used to estimate
the size of the broad line region.

Exposure time. The depth of the observations is chosen to
obtain data of comparable quality to the ones we have obtained in Cycle 13
(adequate to meet our goals). Based on our previous extensive 
experience with structural parameters of distant bulges and AGN 
(e.g. Hunt et al.\ 1999; Treu et al. 2001), and confirmed by our study 
from Cycle 13 data (Treu et al. 2007), the limiting factor is the signal 
to noise at the relatively low surface brightness typical of the disk and 
the outer bulge. The typical surface brightness of the outer bulge
region is I=22 mag arcsec$^{-2}$ , corresponding to F110W$\sim$20.8 mag 
arcsec$^{-2}$ (Vega). According to the NICMOS ETC, surface brightness
I=22 mag arcsec$^{-2}$ gives signal-to-noise ratio of 10 per 1x1 pixel
area in 2300s using the F110W filter (i.e. one orbit per pointing, 4
exposures per pointing and related overhead), which is adequate for
our goals. The same exposures will yield extremely high
signal-to-noise ratio detection (S/N$&gt;200$) of the central point
source, allowing for accurate determination of its luminosity, and the
wings of the PSF. NICMOS-PSF with the F110W filter is ~50% larger than ACS-PSF
in optical bands. However, stellar-to-AGN flux ratio is higher in near IR than optical.
Thus, we will be able to resolve host galaxy bulges.</ObservingDescription>
            
            <RealtimeJustification />
            
            <CalibrationJustification />
            
            <AdditionalComments />
         </Phase2Questions>
      </Questions>
      
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         ThisCycle2GyroParallel="0"
         NextCycle2GyroPrimary="0"
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         AfterNext2GyroPrimary="0"
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         Attachment="/usr/local/APT/APT175/C:\usr\local\APT\APT1721\C:\Users\jhwoo\ARCHIVE\PROPOSAL\HST07\NIC\BHSZv16z37v10.pdf">
         
         <ScientificCategory>AGN/QUASARS</ScientificCategory>
         
         <ScientificKeyword1
            Keyword="Black Holes" />
         
         <ScientificKeyword2
            Keyword="Galaxy Formation And Evolution" />
         
         <ScientificKeyword3
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         <ScientificKeyword4
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         <Survey>false</Survey>
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                        <String>CASM was run in Phase II mode.</String>
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(Tic-Obset
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(Tic-Orbit
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                     <StConstraintSchedulingWindows
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                     <StConstraintSchedulingWindows
                        Name="Abs Orient (30.00 66.00)(120.00 156.00)(210.00 246.00)(300.00 336.00)"
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                     <StConstraintSchedulingWindows
                        Name="Combined Roll Restriction"
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                     <StConstraintSchedulingWindows
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                     <AncillaryData
                        Title="Comments"
                        Label="Comments">
                        
                        <String>The scheduling data was generated by CASM 17.2.</String>
                        
                        <String>CASM was run in Phase II mode.</String>
                     </AncillaryData>
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                  <AncillaryData
                     Title="Roll Ranges Report"
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         <Comments />
         
         <ExecutionDate>1199220633000</ExecutionDate>
         
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 :proposal-id 11166
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(Tic-Obset
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(Tic-Orbit
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(Tic-Obset
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(Tic-Obset
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(Tic-Orbit
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               <MaxDur />
               
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               <Comments />
               
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                  </AncillaryData>
               </VpVisitData>
            </ToolDataItem>
         </ToolData>
         
         <Comments>This is a repeat of visit 14.</Comments>
         
         <ExecutionDate>1217590014000</ExecutionDate>
         
         <ExecutionRoll>212.8204928099666</ExecutionRoll>
         
         <TicData>
            
            <TicFileString>(Tic-Visit
 :proposal-id 11166
 :visit-id "94"
 :proposal-version -1
 :trans-version "20090130"
 :date "05-Jun-2009 18:33:42.0"
 :trans-errors '(:WARNINGS 4 :ERRORS 0 :HEALTH-AND-SAFETY 0
                 :FATAL-ERRORS 0 :CONTINUABLE-FATALS 0)
 :number-of-orbits 1
 :saa-model "23"
 :si-bright-earth-limb-angle 20.0
 :data-volume 83920
 :tdrss-contact-duration 0
 :coron NIL
 )

(Tic-Obset
 :proposal-id 11166
 :visit-id "94"
 :obset-id "94"
 :pcs-mode "FGS"
 )

(Tic-Orbit
 :proposal-id 11166
 :visit-id "94"
 :orbit-number 1
 :pcs-time 355
 :si-vis-utilization 2734
 :al-overhead-at-end 0
 :internal-dur-at-end 131
 :dark-offset NIL
 :dark-utilization 0
 :max-dark-utilization 1920
 :low-sky "N"
 :pcs-visibility 3132
 :pcs-gap 0
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            <TicDataCurrent>true</TicDataCurrent>
            
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            <TicNumOverruns>0</TicNumOverruns>
         </TicData>
         
         <GuidingTolerance>
            
            <Angle />
         </GuidingTolerance>
         
         <SeqWithin>
            
            <VisitList />
         </SeqWithin>
         
         <OnHoldComments />
         
         <ExposureGroup
            Type="Pattern"
            Pattern="1">
            
            <Exposure
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               TargetName="SDSS-J211531.68-072627.5"
               Config="NIC2"
               Opmode="MULTIACCUM"
               Aperture="NIC2"
               SpElement="F110W"
               NumberOfIterations="1"
               TimePerExposure="DEF"
               RealtimeAnalysis="false"
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               Expand="false"
               LowSky="false"
               Shadow="false"
               GSAcqScenario="BASE1TNS"
               NewAlignment="false"
               NewObset="false"
               NewObsetFullAcq="false"
               SpecialCommand="false">
               
               <MaxDur />
               
               <MinDur />
               
               <Comments />
               
               <InstrumentParameters
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               <SubExposures>
                  
                  <SubExposure
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                     OrbitNumber="1" />
                  
                  <SubExposure
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                  <SubExposure
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                     OrbitNumber="1" />
                  
                  <SubExposure
                     PrimaryPatternPosition="4"
                     OrbitNumber="1" />
               </SubExposures>
            </Exposure>
         </ExposureGroup>
      </Visit>
   </Visits>
</HSTProposal>

