Title: The%20Photometric%20Calibration%20of%20the%20Blanco%20Dark%20Energy%20Survey%20(DES)
1The 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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3DES 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
4Basic 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
5The 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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7Photometric 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
8Nightly 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)
9Southern 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).
10SDSS 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)?)
11Global 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
12Global 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)
13Global 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
14Global 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
15Global 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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17Extra Slides
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19DES 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
20Some 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?
21Is 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
22Is 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
23The 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)
24The 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
25Possible 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.
26Possible 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
27The 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
28Structure (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
29Structure (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
30Structure (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).
31Global 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
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