ASTRA Spectrophotometer: Reduction and Flux Calibrations Barry Smalley Astrophysics Group Keele University Staffordshire United Kingdom [email protected] http://www.astro.keele.ac.uk/~bs/ Saul Adelman (The Citadel), Austin Gulliver (Brandon University), Barry Smalley (Keele University), John Pazder (Dominion Astrophysical Observatory), The Future of Photometric, Spectrophotometric Frank Younger (Aurora Astronomical Services), and Polarimetric Standardization, Louis Boyd & Don Epand (Fairborn Observatory) B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Belgium 8-11 May 2006 Blankenberge, BelgiumBlankenberge, 8-11 May 2006 1 Outline ● ● From 2-d CCD images to flux-calibrated spectra. – Spectral Extraction – Atmospheric Extinction Determination – Flux Calibration ASTRA will produce a vast quantity of high quality data – procedures automated as far as possible – sentinels to watch for unusual events B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 2 2-d Images ● ● Two orders on CCD image Optimal reductions using CCDSPEC developed by Austin Gulliver & Graham Hill B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 3 Spectral Extraction ● ● Standard procedures common to normal spectra – Correction for CCD properties: dead rows, hot pixels. – Addition of many Bias and Flat Field frames – Order tracing and PSF fitting using optimal extraction – Scattered light removal – Removal of cosmic rays Issues to investigate – Characterize fringing in red – Shutter timing corrections – Flexure of spectrograph B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 4 Issues for Spectrophotometry ● Spectrophotometry is precise relative photometry at many wavelengths. – Extraction must use same relative amount of flux from all spectra ● ● ● ● extraction of identical fraction of spectral enclosed energy Spectral width depends on seeing and trailing Important to preserve the observed count level and not bin onto a linear wavelength scale. Output instrumental wavelengths and counts/s per wavelength bin. B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 5 Simulated Extracted Spectra B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 6 Earth's Atmosphere ● Rayleigh Scattering ARAY ∝−4 ● Aerosol Scattering AAERO ∝− is variable0.5~1.5 ● Molecular Absorption – Ozone bands ● – ● Huggins & Chappuis Water and Oxygen (Telluric) lines Night Sky Emission lines B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 7 Atmospheric Extinction B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 8 Extinction Law ● Extinction given by Bouguer's Law: m=m 0k X where m=observed stellar magnitude m 0=stellar magnitude above Earth Atmosphere k =extinction coefficient X =airmass ● Extinction coefficient is sum of the various individual contributions – B. Smalley Rayleigh, Aerosol, Ozone, Oxygen, Water The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 9 Airmass ● Airmass determined using simple formula of Young & Irvine (1967) X z =sec z [ 1−0.0012sec 2 z−1 ] ● ● good to better than 1% up to X ≈ 4 Airmass can change significantly during a long exposure – can use effective airmass (Stetson 1989) 1 X eff = [ X START 4 X MIDDLE X END ] 6 B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 10 Seeing ● In slitless spectroscopy resolution depends on seeing: 2 2 ∝ seeing inst ● seeing is variable: – temporal t – airmass ~X 0.6 – wavelength ~−0.2 ● B. Smalley fixed but resolution different to instrumental The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 11 Spectral Resolution Issues ● Important where spectrum is varying most rapidly – e.g. Balmer lines λ 4867 4894 4940 ● B. Smalley k(fit) 0.157 0.178 0.174 k(true) 0.184 0.180 0.176 Important on nights of poor seeing The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 12 Scintillation ● Normal minimum exposure time to 10 seconds to minimize scintillation noise. – Dravins et al. (1998) formula: =0.09 D−2/3 X 1.75 exp – For ASTRA 10-second exposure gives ● ● B. Smalley h 2T −1/ 2 H σ = 0.001 mag. at zenith σ = 0.007 mag. for X = 3. The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 13 Extinction Determination ● Extinction determination without the use of assumed stellar true fluxes – extinction stars are tested to be constant ● – Initially will perform single night reductions ● ● ● variability << 0.01 mag. Assess reliability. investigate multi-night reductions. The brightest stars will be observed through neutral density filter – B. Smalley determine and monitor throughput The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 14 Extinction variability ● Initially assume perfect night – time-independent multi-star Bouguer Law fitting (Sterken & Manfroid 1992) – assessment of residuals ● looking for correlations with time and/or airmass – ● ● χ² and R-statistics (Baptista & Steiner 1993) If variable, use kλ(t) as polynomial, adding terms and use F-test for significance of improvement. Can also split night into smaller blocks – B. Smalley avoid parts of night with poor conditions The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 15 Visual Plotting: Good Night O2 B. Smalley H2O The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 16 Visual Plotting: Variability O3 H2O O2 H2O H2O B. Smalley Grey Cloud Grey Cloud O3 The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 17 Visual Plotting: Poor Seeing Hγ Hβ B. Smalley Hα The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 18 Fitting Telluric Regions ● ● Non-linear extinction violates Bouguer's Law – several methods have been used in the literature – we will use synthetic telluric spectra – least squares fitting to obtain oxygen and water columns and their variability Beware of stellar lines (dis)appearing in and out of telluric lines due to radial velocity variations – Earth's orbital velocity (30 km/s): 0.5Å shift at 5000Å – will assess the level of this uncertainty using model spectra. B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 19 Telluric Spectra ● ● ● Generate synthetic water and oxygen absorption spectra – HITRAN modelling (Rothman L.S. et al. 2005) – simplified 6-layer model of Earth's atmosphere (Nicholls 1988) Calculate with varying water and oxygen columns. Tabulate at high resolution (0.5Å steps) for rapid interpolation. B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 20 Flux Calibration ● Flux calibration against Vega standard – requires neutral density filter ● throughput measured and periodically checked ● Ensure Flux consistency within Standards ● Quality Control – stellar (micro) variability. – long term variability of extinction stars to ensure that there are constant. – instrumental/telescope throughput variations. B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 21 Flux Calibration (cont) ● Re-calibration of whole data set as necessary. ● Ensure spectral resolution effects are allowed for – ● For standards use only the best observations at the highest resolution. Non-standards will be co-added if non-varying – variable stars will not be co-added ● B. Smalley except if variation insignificant between observations. The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 22 Final Stellar Fluxes ● ● Reduction procedures will store intermediate results – extracted spectra as counts – instrumental counts/second above Earth's Atmosphere – nightly extinction models – individual flux calibrated spectra Results as FITS files including headers and processing history – B. Smalley wavelength,bin size,instrumental counts/second,flux relative to Vega,absolute fluxes (photons/s/nm),internal errors,external errors, quality flags The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 23 Summary ● Stellar flux measurements with internal (star-tostar) precision better than 1%. – down to around 10th mag. ● – ● Faint spectrophotometric standards. full error propagation to include both internal and external errors. Absolute flux scale uncertainties will dominate. – revision of absolute fluxes required. http://www.citadel.edu/physics/astra/ B. Smalley The Future of Photometric, Spectrophotometric and Polarimetric Standardization, Blankenberge, Belgium 8-11 May 2006 24
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