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Title: The%20Photometric%20Calibration%20of%20the%20Blanco%20Dark%20Energy%20Survey%20(DES)


1
The Photometric Calibration of the Blanco Dark
Energy Survey (DES)
  • Purpose of Survey
  • Perform a 5000 sq deg griz imaging survey of the
    Southern Galactic Cap in order to
  • Constrain the Dark Energy parameter w to 5
    (stat. errors) in each of 4 complementary
    techniques
  • wP/p (equation of state parameter)
  • Begin to constrain dw/dz
  • Serve as a stepping stone to large-scale,
    next-generation projects (e.g., LSST, SKA, JDEM)
  • New Equipment
  • Replace the prime focus cage on the CTIO Blanco
    4m telescope with a new 2.2 deg FOV optical CCD
    camera
  • Construct instrument 2005-2009
  • Survey Period
  • 30 of the telescope time (525 nights) from
    2009-2014 (September - February)

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3
DES Science
  • Four Probes of Dark Energy
  • Galaxy Cluster counting
  • 20,000 clusters to z1.3 with M gt 2x1014 Msun
  • Weak lensing
  • 300 million galaxies with shape measurements over
    5000 sq deg
  • Spatial clustering of galaxies
  • 300 million galaxies to z 1 and beyond
  • Standard Candles
  • 1900 SNe Ia, z 0.25-0.75

H. Lin
Good all-sky photometry (2 or better) needed
for photometric redshifts (cluster counting, weak
lensing, galaxy clustering) and for good light
curves (SNe Ia).
Photometric redshifts out to z1.3
4
Basic Survey Parameters
Overlap with South Pole Telescope Survey (4000
sq deg)
Survey Area
  • Limiting Magnitudes
  • Galaxies 10s griz 24.6, 24.1, 24.3, 23.9
  • Point sources 5s griz 26.1, 25.6, 25.8, 25.4
  • Observation Strategy
  • 100 sec exposures
  • 2 filters per pointing (typically)
  • gr in dark time
  • iz in bright time
  • Multiple tilings/overlaps to optimize photometric
    calibrations
  • 2 survey tilings/filter/year
  • All-sky photometric accuracy
  • Requirement 2
  • Goal 1

Connector region (800 sq deg)
J. Annis
Overlap with SDSS equatorial Stripe 82 for
calibration (200 sq deg)
Total Area 5000 sq deg
5
The DES Instrument (DECam)
DES Focal Plane The Hex
z band
B. Flaugher
  • 62 2k x 4k image CCDs
  • 520 Mpix
  • 0.27 arcsec/pixel
  • LBL design
  • fully depleted, 250-micron thick CCDs
  • 17 second readout time
  • QEgt 50 at 1000 nm

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7
Photometric Monitoring
  • 10 micron all sky camera
  • Apache Point Observatory (SDSS, ARC3.5m)
  • Whipple Observatory (Pairitel telescope)
  • detects even light cirrus under a full range of
    moon phases (no moon to full moon)
  • Optical All-Sky camera
  • CONCam, TASCA
  • RoboDIMM seeing and flux monitor
  • Provide real-time estimates of sky conditions for
    survey strategy
  • E.g, Should next image be a photometric
    calibration field, a science target, or something
    else?
  • Provide measure of the photometric quality of an
    image
  • E.g., This image was obtained under
    such-and-such conditions is it good enough to be
    used for photometric calibrations?

APO 10 micron all-sky camera
8
Nightly Absolute Calibration
  • (Evolving) Standard Star Observation Strategy
  • Observe 3 standard star fields, each at a
    different airmass (X1-2), between nautical (12)
    and astronomical (18) twilight (evening and
    morning).
  • Observe up to 3 more standard fields (at various
    airmasses) throughout the night
  • Also can observe standard star fields when sky is
    photometric but seeing is too poor for science
    imaging (seeing gt 1.1 arcsec)
  • Use fields with multiple standard stars
  • Keep an eye on the photometricity monitors
  • Absolute Calibration Strategy
  • Calibrate to the DES griz natural system
  • No system response color terms in the photometric
    equations
  • Avoids coupling science images obtained in
    different filters
  • Use ugriz and ugriz standards transformed to
    the DES griz natural system
  • SDSS gri(z) and gri(z) are similar to DES
    gri(z), so transformations should be well behaved
  • Transformations could be done on the fly
  • Similar to the SDSS calibration strategy
  • SDSS photometry is published in the SDSS 2.5m
    telescopes ugriz natural system
  • SDSS photometry is calibrated based upon
    observations of ugriz standard stars by the
    SDSS 0.5m Photometric Telescope (PT)

9
Southern ugriz Standards
  • Smith, Allam, Tucker, Stute, Rodgers, Stoughton
  • 13.5' x 13.5' fields, typically tens of stds. per
    field
  • r 9 - 18, 60 fields, 16,000 standards
  • See talk by J . Allyn Smith
  • stars as bright as r13 can likely be observed by
    DECam with 5 second exposures under conditions
    of poor seeing or with de-focusing (FWHM1.5).

10
SDSS Stripe 82 ugriz Standards
  • Already part of the DES survey strategy.
  • Readily observable at a range of airmasses
    throughout most nights during the DES program.
  • 2.5 wide (compares favorably with DECam's FOV
    (2.2).
  • Good star/galaxy classification to r 21.
  • Value-added catalogue of tertiary standards is
    being made
  • Area of Stripe 82 has been observed by SDSS gt 10x
    under photometric conditions
  • 1 million tertiary SDSS ugriz standards (r
    14.5 - 21)!
  • 4000 per sq deg (on average)
  • Ivezic et al. 2006, in prep.
  • See talk by Zeljko Ivezic

(Others VST OmegaCam stds (Verdoes Kleign)?
SkyMapper stds (Bessell)?)
11
Global Relative CalibrationsHex-to-Hex
Zeropoint Offsets
  • We cover the sky twice per year per filter. This
    is called tiling.
  • It takes 1700 hexes to tile the whole survey
    area

The Hex
Jim Annis DES Collaboration Meeting, May 5-7,
2005
12
Global Relative CalibrationsStar Flats
  • Due to vignetting and stray light, a detectors
    response function differs for point sources and
    extended sources
  • Standard flat fields (domes, twilights, skies)
    may flatten an image sky background well, but not
    the stellar photometry
  • The solution star flats (Manfroid 1995)
  • offset a field (like an open cluster) multiple
    times and fit a spatial function to the magnitude
    differences for matched stars from the different
    exposures
  • can also just observe a well-calibrated field
    once (Manfroid 1996)

U
B
V
R
R
V
I
Manfroid, Selman, Jones 2001, ESO WFI using
dithered exposures (3rd degree polynomial fits)
Koch et al. 2004, ESO WFI star flats based on
SDSS Stripe 82 observations (2nd order polynomial
fits)
13
Global Relative Calibrations Simulation
  • INSTRUMENT MODEL
  • A multiplicative flat field gradient of amplitude
    3 from east to west
  • An additive scattered light pattern with a
    amplitude from the optical axis, 3 at the edge
    of the camera
  • An additive 3 rms scattered light per CCD
  • Solution
  • Simultaneous least squares solution to the
    underlying relative photometry given the
    observations


scaling bar is 0.20 mags to 0.20 mags
Jim Annis DES Collaboration Meeting, May 5-7,
2005
14
Global Absolute Calibration
  • Need
  • one or more spectrophotometric standard stars
    which have been calibrated (directly or
    indirectly) to a NIST standard source
  • an accurately measured total system response for
    each filter passband for at least one CCD
  • filter transmissions, CCD QE, optical throughput,
    atmospheric transmission
  • Calculate the expected photon flux Fexp for each
    std star in each filter passband (synthetic
    photometry)
  • Measure the magnitude for each standard star in
    each filter passband with the BlancoDECam
  • Calculate the zeropoint zp via the relation,
  • 10-0.4(mag zp) Fexp

15
Global Absolute Calibration
  • Filter transmission, CCD QE, and optical
    throughput for the BlancoDECam can be measured
    via a monochromator (but see also Chris Stubbs
    talk on a tunable dye laser system and David
    Burkes talk on LSST calibration)
  • The atmospheric transmission spectrum for CTIO
    has been measured (Stone Baldwin 1983, Baldwin
    Stone 1984, Hamuy et al. 1992, 1994)
  • Several potentially useful spectrophotometric
    standards are available
  • E.g., GD 71, G158-100, GD 50, and G162-66
  • All are HST WD spectrophotometric standards
  • All are visible from CTIO
  • All are V gt 13.0
  • Wont saturate DECam at an exposure time of 5
    seconds (FWHM 1.5arcsec)

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17
Extra Slides
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19
DES Simulations Feed DM Challenges
  • 2004 Level 0 Image Simulations ? DM Challenge 0
    Done!
  • Reformatted SDSS data used to simulate DES images
  • 2005-06 Level 1 Catalog Image Sim. ? DM Chal. 1
    Done!
  • 500 sq. deg. catalog 500 GB of images FNAL and
    UChicago computing used
  • 2006-07 Level 2 Catalog and Image Sim. In
    progress
  • 5000 sq. deg. catalog 5 TB of images
  • FermiGrid MareNostrum SuperComputer (Barcelona)
  • Higher resolution N-body simulation, more
    realistic galaxy properties, and more
    sophisticated atmosphere and instrument models
    (noise, ghosts)
  • Recover input cosmology from catalogs using 4 DES
    key project methods
  • 2007-8 Level 3 Catalog and Image Simulations
  • Suite of full-DES catalogs (i.e., different input
    cosmologies)
  • Synergy with DOE SciDAC proposal (with many DES
    collaborators) to produce large cosmological
    simulations for dark energy studies
  • 1 year of DES imaging data
  • Recovery of input cosmologies from catalogs and
    images
  • Stress test of full data processing system

20
Some Definitions
  • Relative Photometric Calibration
  • m m0 -2.5log(F/F0)
  • the ratio F/F0 is important, not absolute value
    of F0
  • F0 need not be measured directly
  • (F/F0,m0) can be defined arbitrarily (e.g.,
    relative to Vega).
  • Absolute Photometric Calibration
  • connects mags, which are relative by nature, to
    real physical fluxes (e.g., photons/s/m2)
  • answers the question, What is the zeropoint flux
    F0 for mag m0?

21
Is Absolute Calibration Necessaryand/or Useful?
  • Absolute calibration is necessary in order to
    make use of results from models or from other
    experiments, either for input into the current
    experiment or for sanity checks
  • Red Sequence Cluster Finding
  • could in principle be done purely based upon
    relative calibration internal to the DES
    (empirical calibration of red sequence)
  • could lose benefits of modelling with synthetic
    photometry
  • Photo-z's
  • could also, in principle, be done purely based
    upon relative calibration
  • could also lose benefits of modeling with
    synthetic photometry

22
Is Absolute Calibration Necessaryand/or Useful?
  • Type Ia SNe (0.3 lt z lt 0.8)
  • absolute calibration needed to accurately compare
    rest-frame photometry of high-redshift SNe
    against the rest-frame photometry of low-redshift
    SNe within the DES SNe sample
  • strictly speaking, only an absolute color
    calibration is needed
  • the zeropoints for the 4 photometric bands need
    to be the same
  • the zeropoints for the 4 photometric bands can
    all be wrong by the same amount, though
  • see SNAP calibration requirements
  • absolute calibration needed in order to combine
    DES SNIa results with other SNIa experiments,
    which are done in other filter systems
  • Galaxy evolution
  • absolute calibration needed in order to compare
    DES results with those of galaxy evolution models

23
The Absolute Calibration Experiment
  • Assume a perfectly flat relative calibration
    across the full 5000 sq deg of the DES
  • chip-to-chip and tile-to-tile offsets and color
    terms are known perfectly and applied perfectly
    to all the data
  • all that are needed for the absolute calibration
    of the entire survey are the 4 zeropoints one
    for each filter passband to convert the
    measured mags in each passband into a calibrated
    flux with real flux units (e.g., photons/s/m2)

24
The Absolute Calibration Experiment
  • Need
  • one or more spectrophotometric standard stars
    which have been calibrated (directly or
    indirectly) to a NIST std source
  • an accurately measured total system response for
    each filter passband for at least one CCD
  • filter transmissions, CCD QE, optical throughput,
    atmospheric transmission
  • Calculate the expected photon flux Fexp for each
    std star in each filter passband (synthetic
    photometry)
  • Measure the magnitude for each standard star in
    each filter passband with the BlancoDECam
  • Calculate the zeropoint zp via the relation,

    10(-0.4mag zp) Fexp

25
Possible Spectrophotometric Stds
  • Vega
  • V0.03, RA183656.3, DEC384701
  • NIST-calibrated. Too bright! Too far north!
  • BD17 4708
  • V9.47, RA211131.4, DEC180534
  • SDSS fundamental standard. F subdwarf. Too
    bright.
  • G191 B2B
  • V11.77, RA050530.1, DEC524947
  • HST White Dwarf standard. Too bright? Too far
    north!
  • GD 71
  • V13.03, RA055227.5, DEC155317
  • HST White Dwarf standard.
  • P330E
  • V13.01, RA163134.3, DEC300852
  • HST solar analog. A bit northerly.

26
Possible Southern Spectro. Stds.
  • Several potentials in Stone Baldwin, 1983,
    MNRAS, 204, 347
  • G158 -100
  • r'14.691, RA003354.6, DEC-120758.9
  • HST White Dwarf standard.
  • Filippenko Greenstein, 1984 PASP, 96, 530
  • GD 50
  • V14.06, RA034850, DEC-005831
  • HST White Dwarf standard.
  • Stone, 1996 ApJS, 107, 423
  • G162-66
  • V13.0, r'13.227, RA103343, DEC-114139
  • HST White Dwarf standard.
  • Stone, 1996 ApJS, 107, 423

27
The Shutter
  • Spec's from SOAR shutter (A. Walker)
  • 1 percent UNIFORMITY at 1 sec exposure time
  • actual exp. time anywhere on CCD should be no
    more than 1 different from anywhere else at this
    exposure time
  • Shutter exposure time REPEATABILITY better than
    0.005 sec (5 milliseconds)
  • Shutter exposure time ACCURACY should be such
    that the offset from the nominal exposure time
    should be less than 0.05 sec (50 milliseconds)
  • Shutter should allow exposures from 1 sec upwards
  • capability to take shorter exposures (e.g., down
    to 0.2) would be useful as a GOAL, not a
    specification

28
Structure (I)
  • The Photometric Standards Module is basically a
    big least squares solver, fitting the observed
    mags of a set of standard stars to their true
    mags via a simple model (photometric equation).
  • In one of its simplest forms, the photometric
    equation looks like this
  • m minst ? a ? kX (1)
  • m is the standard (true) mag of the standard
    star
  • minst is the instrumental mag, minst
    -2.5log(counts/sec)
  • a is the photometric zeropoint
  • k is the first-order extinction
  • X is the airmass

29
Structure (II)
  • Since we will likely be using standard stars
    which are on a system that closely approximates
    but does not exactly match the DES natural
    system, we will probably want to add an
    instrumental color term to the photometric
    equations
  • m minst ? a ? b(color ? color0) ? kX (2)
  • color is a color index, e.g., (g-r)
  • color0 is a constant indicating the crossing
    color between the DES natural system and the
    standard star photometric system
  • converts standard stars to DES system, and not
    the other way around!
  • use only for standard star observations when
    applying the results to target data, use m
    minst ? a ? kX.
  • follows SDSS photometric calibration strategy

30
Structure (III)
  • Explicit examples for DES filters
  • g ginst ? ag ? bg ( (g-r) ? (g-r)0 ) ?
    kgX (3a)
  • r rinst ? ar ? br ( (g-r) ? (g-r)0 ) ?
    krX (3b)
  • i iinst ? ai ? bi ( (i-z) ? (i-z)0 ) ?
    kiX (3c)
  • z zinst ? az ? bz ( (i-z) ? (i-z)0 ) ?
    kzX (3d)
  • These assume that only two filters will be
    observed each night (either g and r, or i and z).

31
Global Relative Photometry
? CMB style mapping strategy ? y A x N ? y
observations ? Ratios of instrumental star fluxes
between pairs of hexes (62 ccds 1
hex) ? Includes effects of uncorrected flat field
problems and scattered light problems ? x scale
factor map ? Scale factor for a given hex
image ? N noise ? A survey mapping ? 0 if no
overlap ? 1/3 if 2nd, 3rd, tiling overlap ? ½ if
4th, and higher tile overlaps
  • Solutions
  • x W y
  • Simple average coadd
  • Wcoadd AtA -1At
  • Weighted averaging
  • W At N -1 A -1AtN -1
  • N is the noise covariance matrix
  • Minimum variance for Gaussian noise
  • Provides least squares flux scalings
  • That is, the flat map
  • Inverting large matrices (??)
  • Year 1 4 matrices of 6000x4000
  • Year 2 4 matrices of 30,000x8000

Jim Annis, DES Collaboration Meeting, May 5-7,
2005
32
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