Modern Observational/Instrumentation Techniques Astronomy 500

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Presentation transcript:

Modern Observational/Instrumentation Techniques Astronomy 500 Andy Sheinis, Sterling 5520,2-0492 sheinis@astro.wisc.edu MW 2:30, 6515 Sterling Office Hours: Tu 11-12

Ch1 of Birney, Gonzalez and Oesper has coordinate stuff

Preliminary Processing Image display Bias subtraction Flat fielding Photometric Calibration Sky subtraction Wavelength calibration Spectro-photometric calibration

Preliminary Processing There are two types of instrumental signature to remove: Additive: Bias Level Bias Structure Dark Counts Multiplicative: Q.E. variations on all scales Constant # of counts added independent of the brightness of the source(s). Constant fractional effect

Astronomy Packages IRAF (http://iraf.noao.edu) IDL (astronomy users library: http://idlastro.gsfc.nasa.gov/homepage.html) XVISTA (http://astro.nmsu.edu/holtz/xvista) FIGARO MIDAS AIPS Add-on packages: DAOPHOT

Astronomy Packages Issues: availability, cost, philosophy, data handling (disk vs. memory), speed, ease of use (e.g., keywords vs. parm files), language and access to existing code, ability to add new code, scripts/ procedures (internal control language).

Image Display DS9 or SAO image with IRAF ATV with IDL Issues: Dynamic Range (8-bit) Sampling (spatial and depth) Scaling (depth) Color map

Image file formats FITS (Flexible Image Transport System) Header (80 byte ASCII records) Data (16-but Int, 32 bit int or 32 bit FP) Details of the data are conmtained in the header keywords, I.e. Simple Bitpix Naxis Ad infinitum

Image file formats IRAF uses internally defined data format (BAD!) Used for all (disk based) calculations Proprietary and subject to change! As an option, they now offer FITS format calculations. (I highly recommend this!) Not the default, need to add something to your login.cl file

Preliminary Processing Bias subtraction Model bias level Subtract (may be different for different readout amplifiers) Definitely different for mosaiced images

Bias Correction Bias level and any y (along columns) gradient is taken out via overscan subtraction. Bias structure is taken out by subtracting a zero-level frame. In IRAF ccdproc takes care of both.

Overscan After reading out the CCD `real’ pixels, you can continue to read out virtual pixels and record the bias level and read noise of the amplifiers. These virtual pixels are called the overscan region Active area of CCD Row or line # Column # overscan region

Two amplifier overscan

Overscan subtraction First you need to identify the relevant columns. In IRAF use the format: [x1,x2:y1,y2] Sky level Overscan#1 Oscan#2 In IRAF, plots like this are made using implot

Preliminary Processing Flat fielding 2 kinds high order, pixel-to-pixel variations Low order, sky illumination, vignetting, scattered light Model the flat field based on dome flats, sky flats, twilight flats Divide by normalized flat field

Flat Fielding There are pixel-to-pixel QE variations and lower spatial frequency QE variations in all electronic detectors. The goal of flat-fielding is to multiply every pixel by the correct normalizing factor to eliminate these QE differences. Ideally, illuminate the detector with a source that is as flat on the sky as the background and collect at least a million e- per pixel. Then could flat-field to =0.1%.

Flat Fielding If you could illuminate the CCD uniformly, then normalize the mean to 1, this image could be divided into every frame. For direct imaging, usually use a combination of: Dome Flats Twilight Flats Dark Sky Flats

Dome Flats Put some quartz (hot, continuum source) lamps on the telescope and illuminate a white screen or spot on the dome. These often don’t work very well for two reasons: The lamps are always too cool (red) The dome is not even close to infinity and usually illuminates the primary differently than the sky But, you can collect a lot of photons during the day

Twilight Flats These often work pretty well The Sun is pretty hot, the scattering surface illuminates the telescope just like the dark night sky Doesn’t use dark time

Dark-sky Flats These tend to work very well. They match the sky perfectly They sometimes require useful dark time They sometimes contain fringes

Stars and Galaxies For twilight and dark sky flats you have a problem in that they contain stars and galaxies. The usual trick is to move the telescope between exposures and then do a non-registered stack of the frames in each filter. Median or better yet minmax rejection (for example, in the frame combining can effectively eliminate all the stars and galaxies in the combined flat.

Minmax rejection Pixel value: 1000 200 180 180 Average with minmax rejection, reject 2 highest value averaging lowest two will give the sky value. NOTE! Must normalize frames to common mean or mode before combining! Sometimes it is necessary to pre-clean the frames before combining.

Combining Frames In IRAF, imcombine is the task to combine frames. combine=average reject=minmax scale=mode nlow=0 nhigh=2

Combining Frames In IDL, just do arithmetic on the images Image C=Image A+Image B Can use canned routines such as: “medarr,bigarray,outarray”

Flat fielding tricks Combine domes (high counts, bad illumination) with dark sky flats (low counts, excellent illumination). Spatially smooth (or fit low-order surface to) both combined dome and combined dark sky. > sDome, sDark Remove dome low-spatial-frequency pattern: Dome/sDome sDark is the sky flat with the low-f pattern already removed. Best of both worlds is (Dome/sDome) x sDark

I-band PFCam flat fields Dust on filter Note differences with color. This means that objects with different spectra will be flat-fielded slightly incorrectly. V-band Rings due to non uniform thinning U-band Two amplifer readout

Flat-field tests Take cuts through your flat-fielded frames and make sure the sky is flat (check corners). IRAF implot, IDL (ATV (r and c) implot) In blank areas, make sure the pixel-to-pixel variations are consistent with shot noise from the sky level. IRAF imexam and the `m’ key, IDL (ATV, imexam, photometry)

Preliminary Processing Photometric Calibration Measure R* for real, using a known standard through the exact same setup and conditions Find a nearby standard May want to observe before and after

Preliminary Processing Wavelength calibration (for spectroscopy Measure arcd lamps, and/or night sky lines Fit lines to a model Check and modify

Preliminary Processing Spectro-photometric calibration (spectroscopy) Measure R* for a photometric standard under the same conditions Get photon caount at every wavelength bin