Presentation is loading. Please wait.

Presentation is loading. Please wait.

CCDs. CCDs—the good (+)  Linear response  photometry is “simple” +High efficiency, compared to other detectors +Sensitive to many wavelengths +2-D arrays.

Similar presentations


Presentation on theme: "CCDs. CCDs—the good (+)  Linear response  photometry is “simple” +High efficiency, compared to other detectors +Sensitive to many wavelengths +2-D arrays."— Presentation transcript:

1 CCDs

2 CCDs—the good (+)  Linear response  photometry is “simple” +High efficiency, compared to other detectors +Sensitive to many wavelengths +2-D arrays possible in large formats +Can be shuttered, or “frame transfer” +High dynamic range (i.e., contrast)

3 CCDs—the bad (-) -Read noise: electrons not transferred perfectly (but pretty good) -Dark current –Temperature sensitive –Coolant/cooler? –Accumulates condensates (i.e., gook)

4 CCDs—the ugly Electron wells are finite and imperfect Leakage Saturation blooms Cosmic rays Pixel-to-pixel variation Age-dependent

5 Linearity (good) Expose to more light, get more electrons—linearly increasing Photometry made easier because signal can be expressed as (data numbers per second), unambiguously Makes comparison of different images easier

6 Linearity—one more thing Allows straightforward normalization and addition of images

7 Quantum efficiency Generally, higher than most other detection schemes—that’s good (especially photographic film) Wavelength dependent

8 Exposure metering Can be shuttered, or Can be “frame transfer”

9 Dark current Thermal motions of electrons produces a spurious signal that is not due to incident light Temperature-dependent, so most cameras are cooled The level of spurious signal is still linear w.r.t. temperature and exposure duration, so can be subtracted from the “real” images Examples…

10 Temperature dependence of dark current Q: Why’d we do this? A: The camera is cold, so any residue floating around in the telescope will condense on the CCD. Yuck! Therefore, periodic “bakeouts” to remove gook from the CCD.

11 Pixel-to-pixel variation Differences in charge transfer efficiency Differences in well depth (less important) Shorted pixels continuously leaking charge Age-dependent (see example) Compensate via flat fielding and subtraction of dark frames

12 CCD aging

13 Pixel saturation Potential wells have a finite depth, can hold only a finite number of electrons 100,000 to 200,000 electrons is typical limit When the well is full, where do those electrons go? They spill over into neighboring pixels Example…

14 Composite Example 1. Raw data

15 Composite Example 2. Subtract dark frame 3. Correct for stray light (no true flat fields for X-rays) 4. Co-register the cleaned images, normalize for exposure time 5. Replace saturated parts of “long” exposure with pixels from “short” exposure, to yield the final product…

16 Why composite? Trivial answer: It looks nice. Less trivial answer: Enhanced dynamic range. You get to see the faint parts and the brighter parts, with quantitative accuracy.

17 Troublesome Aesthetically unpleasant Confuse morphology of imaged object How to remove? One more thing: cosmic rays


Download ppt "CCDs. CCDs—the good (+)  Linear response  photometry is “simple” +High efficiency, compared to other detectors +Sensitive to many wavelengths +2-D arrays."

Similar presentations


Ads by Google