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Relative measurements with Synoptic surveys I.Photometry & Astrometry Eran Ofek Weizmann Institute
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Talk Layout Motivation and science case Relative photometry Limiting factors Methods Linear regression Relative astrometry Effects and limiting factors Methods and results
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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
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Light curves Some eclipsing M-dwarfs in PTF
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Asteroids rotation Poolishok et al. 2012
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Asteroids rotation Poolishok et al. 2012
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Photometry How? Aperture photometry e.g., phot, SExtrator PSF photometry e.g., daophot, dophot Galaxy fitting e.g., GalFit Absolute (Calibrated) Relative
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Photometry Aperture photometry Summing the intensity within an aperture Complications: Subtracting the background Interpolating Optimal aperture Centering
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Aperture photometry Interpolating Solution: Bickerton & Lupton 2013 Fraction of light
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Aperture photometry Optimal aperture Aper Radius [pix] S/N
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Aperture photometry Biases Aper Radius [pix] S/N Biases may influence photometry, mainly At the faint end (e.g., due to uncertainty in position) Fraction of light S/N
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Calibrated photometry Methods Calibrate the apparatus (but atmosphere) Local standard stars Global standard stars E.g., CalibMag = InstMag + ZP + … AM + color + AM color + … time…, CCD position, atmo cond,…
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Calibrated photometry Photometry calibration good to 2-3% CCD 4 Ofek et al. 2012a,b
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Calibrated photometry Photometry calibration good to 2-3% Using SDSS stars as standard stars to calibrate fields outside SDSS footprint (photometric nights) CCD 4 Ofek et al. 2011 submitted
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Relative photometry Find the ZP per image to add to magnitudes such that the scatter in the Light curves is minimized
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Relative photometry The ensemble method Everett & Howell (2001) f ij – instrumental flux i-star (1..p), j-image (1..q) Solving per field ij – instrumental flux err Normalize by the ensamble: Caveats: requires stars that appears in all images + multiple iterations
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Relative photometry & LSQ Linear least squares – a reminder see a nice review in Gould (2003; arXiv/0310577)
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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
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Relative photometry Solution using linear least squares Honeycutt (1992); Padmanabhan et al. (2007); Ofek et al. (2011) m ij – instrumental mag i-star (1..p), j-image (1..q) Solving per field (overlap between fields not guaranteed) ij – instrumental mag err
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Relative photometry Using linear least squares H (“design matrix”) Observations Free parameters z
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Relative photometry Simultaneous absolute calibration H is (pq)x(p+q) matrix However, rank is p+q-1 Adding calibration block
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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)
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Relative photometry Relative photometry ~3-5mmag Method presented in: Ofek et al. 2011 ApJ 740, 65
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Relative photometry Limiting factors Poisson statistics Flat fielding Charge diffusion variations Atmospheric intensity scintilations
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Relative photometry Limiting factors Credit: Malagon (BNL) Flat
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Astrometry Motivation Relating objects… Is a transient associated with gal. nuc.? Searching for SN progenitors Proper motions Parallaxes Binarity
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Motivation Example Astrometric amplitude of 10kK WD-WD binary at 14-18 mag range
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State of the art Best proper motions available: Hipparcos: ~0.25 (1 σ ) mas/yr (V<9) PS-1/MDS ~10mas/yr (1 σ ) Tonry+2012 USNO-B vs. SDSS (+): ~6 mas/yr (1 σ ) GAIA…
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Large field of view What effects astrometry?
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Relative astrometry Limitations However…
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Large field of view Field distortion Precession/Nutation Atmospheric refraction Color dependent refraction Abberation of light Light deflection Scintillations Centeroiding
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Large field of view Atmospheric refraction
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Large field of view Light Deflection
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Large field of view Light Deflection Differential Light difl.
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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
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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
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Search for proper motion stars Comparing PTF deep coadd with SDSS
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Search for proper motion stars Comparing PTF deep coadd with SDSS
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Search for proper motion stars Comparing PTF deep coadd with SDSS
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Search for proper motion stars Comparing PTF deep coadd with SDSS
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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
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Metodology i – image, j - star X ij – (abb…) = DX i + j + X ij cos(Θ i ) – Y ij sin(Θ i ) + … a i X ij 2 + b i Y ij 2 + … (distortions per image) c X j 2 + d Y j 2 + … (distortion per set of images) e i AM ij sin(Q ij ) + f i AM ij Color j sin(Q ij ) + … g (X ij – floor(X ij )) + … (sys. Center. Errors) (proper motion) + (parallax) + … Yij – (abb…) = … Produce: ~10 7 equations with ~30,000 unknowns (single field/ccd)
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Relative astrometry Ofek & Gorbikov
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Preliminary results
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Relative astrometry Ofek & Gorbikov
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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
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End Thank you!
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Preliminary results
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Absolute astrometry Limitations
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Abs. astrometry Reference catalogs: SDSS or UCAC-3 or USNO-B1 (in SCAMP) or USNO-B1 (in Astrometry.NET) In PTF IPAC pipeline images
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Abs. astrometry In PTF IPAC pipeline images
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Abs. astrometry In PTF IPAC pipeline images
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Search for proper motion stars Comparing PTF deep coadd with SDSS Advantage: deeper than previous surveys
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Search for proper motion stars PM [“/yr] = V [km/s] / (4.74 d [pc] ) H=M+5 log 10 (V)–3.379 = m–5 log 10 (PM) Reduced Proper motion
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