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Relative measurements with Synoptic surveys Photometry & Astrometry. Eran Ofek Weizmann Institute. Talk Layout. Motivation and science case Relative photometry Limiting factors Methods Linear regression Relative astrometry Effects and limiting factors
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Relative measurements with Synoptic surveys Photometry & Astrometry Eran Ofek Weizmann Institute
Talk Layout Motivation and science case Relative photometry Limiting factors Methods Linear regression Relative astrometry Effects and limiting factors Methods and results
Motivation Relative photometry Light curves Spectral energy distribution Precision driver: small variations Relative astrometry Proper motions, parallax, binarity Photometry and astrometry have much in common
Light curves Some eclipsing M-dwarfs in PTF
Asteroids rotation Poolishok et al. 2012
Asteroids rotation Poolishok et al. 2012
Photometry How? Aperture photometry e.g., phot, SExtrator PSF photometry e.g., daophot, dophot Galaxy fitting e.g., GalFit Absolute (Calibrated) Relative
Photometry Aperture photometry Summing the intensity within an aperture Complications: Subtracting the background Interpolating Optimal aperture Centering
Aperture photometry Interpolating Solution: Bickerton & Lupton 2013 Fraction of light
Aperture photometry Optimal aperture S/N Aper Radius [pix]
Aperture photometry Biases Fraction of light S/N S/N S/N Biases may influence photometry, mainly At the faint end (e.g., due to uncertainty in position) Aper Radius [pix]
Calibrated photometry Methods Calibrate the apparatus (but atmosphere) Local standard stars Global standard stars E.g., CalibMag = InstMag + ZP + … aAM + b color + c AM color + … time…, CCD position, atmo cond,…
Calibrated photometry Photometry calibration good to 2-3% CCD 4 Ofek et al. 2012a,b
Calibrated photometry Ofek et al. 2011 submitted Photometry calibration good to 2-3% Using SDSS stars as standard stars to calibrate fields outside SDSS footprint (photometric nights) CCD 4
Relative photometry Find the ZP per image to add to magnitudes such that the scatter in the Light curves is minimized
Relative photometry The ensemble method Everett & Howell (2001) Solving per field i-star (1..p), j-image (1..q) fij – instrumental flux sij – instrumental flux err Normalize by the ensamble: Caveats: requires stars that appears in all images + multiple iterations
Relative photometry & LSQ Linear least squares – a reminder see a nice review in Gould (2003; arXiv/0310577)
Relative photometry Solution using linear least squares Linear least squares – a reminder However, sometime inversion is hard… For large sets of equations use conjugate gradient
Relative photometry Solution using linear least squares Honeycutt (1992); Padmanabhan et al. (2007); Ofek et al. (2011) Solving per field (overlap between fields not guaranteed) i-star (1..p), j-image (1..q) mij – instrumental mag sij – instrumental mag err
Relative photometry Using linear least squares z <m> Free parameters H (“design matrix”) Observations
Relative photometry Simultaneous absolute calibration H is (pq)x(p+q) matrix However, rank is p+q-1 Adding calibration block
Relative photometry Additional de-trending We can add more columns to H and P. For example: Airmass x color term Positional terms Multiple CCDs (i.e, overlap) – ubercal (SDSS; PS1; LSST)
Relative photometry Method presented in: Ofek et al. 2011 ApJ 740, 65 Relative photometry ~3-5mmag
Relative photometry Limiting factors Poisson statistics Flat fielding Charge diffusion variations Atmospheric intensity scintilations
Relative photometry Limiting factors Flat Credit: Malagon (BNL)
Astrometry Motivation Relating objects… Is a transient associated with gal. nuc.? Searching for SN progenitors Proper motions Parallaxes Binarity
Motivation Example Astrometric amplitude of 10kK WD-WD binary at 14-18 mag range
State of the art Best proper motions available: Hipparcos: ~0.25 (1σ) mas/yr (V<9) PS-1/MDS ~10mas/yr (1σ) Tonry+2012 USNO-B vs. SDSS (+): ~6 mas/yr (1σ) GAIA…
Large field of view What effects astrometry?
Relative astrometry Limitations However…
Large field of view Field distortion Precession/Nutation Atmospheric refraction Color dependent refraction Abberation of light Light deflection Scintillations Centeroiding
Large field of view Atmospheric refraction
Large field of view Light Deflection Light Deflection
Large field of view Light Deflection Differential Light difl.
Large field of view Distortions ~1”/deg Precession >3”/yr Refraction ~1-2”/deg Color Ref. ~80mas/500Å Abberation ~0.5”/deg Deflection ~0.1mas/deg Scintillations 2”/√(60 x 100)~25mas Centeroiding ? <20 mas
Stratergies for PTF PTF deep coadd vs. SDSS good for faint stars ~10 mas/yr Use PTF multiple epochs beat scintillation noise using √N Periodicity in the residuals… Binaries
Search for proper motion stars Comparing PTF deep coadd with SDSS
Search for proper motion stars Comparing PTF deep coadd with SDSS
Search for proper motion stars Comparing PTF deep coadd with SDSS
Search for proper motion stars Comparing PTF deep coadd with SDSS
Stratergies for PTF PTF deep coadd vs. SDSS good for faint stars ~10 mas/yr Use PTF multiple epochs beat scintillation noise using √N Periodicity in the residuals… Binaries
Metodology i – image, j - star Xij – (abb…) = DXi + <X>j + Xij cos(Θi) – Yij sin(Θi) + … ai Xij2 + bi Yij2 + … (distortions per image) c Xj2 + d Yj2 + … (distortion per set of images) ei AMij sin(Qij) + fi AMij Colorj sin(Qij) + … g (Xij – floor(Xij)) + … (sys. Center. Errors) (proper motion) + (parallax) + … Yij – (abb…) = … Produce: ~107 equations with ~30,000 unknowns (single field/ccd)
Relative astrometry Ofek & Gorbikov
Relative astrometry Ofek & Gorbikov
Summary Relative photometry 0.5-1 mmag precision is possible using ground based observation Relative astrometry Sub-mas precision is possible using (non-AO) ground based observations. Both – requires excellent understanding of systematic effects. Tips: explore the residuals Relative astrometry: PTF can deliver sub-mas precision relative astrometric measurements
End Thank you!