Title: CCDs Charge Coupled Devices
1CCDs(Charge Coupled Devices)
- An Imaging Technology in Visible Light
- Marino Maiorino - Dec. 1st 2006
- 1500 Downstairs Meeting Room
2Summary
- Introduction
- The Birth of New Technologies
- CCD Features
- Technological Limitations
- Basic Data Manipulation
- IFAE and CCDs
- Improper Applications
- Alternative Technologies
- Latest Developments
3Introduction
- On Visible and Optical Wavelengths
- Image Recording Techniques
- Transition between film and Solid-State detectors
- Digital revolution
- Astronomical Imaging With Film
- Telescopes do NOT magnify they get more light!
Massimo Capaccioli
4On Visible and Optical Wavelengths(Introduction)
- Visible (380 750 nm)
- What is visible to the human eye
- Optical (300 1000 nm)
- Includes some UV and IR
- Range of wavelengths where optics laws apply
5Naked Eye Observation(Image Recording Techniques)
- 6 Mcones
- 200 Mrods
- Logarithmic sensor
- Daylight (Photopic) vision
- Nighttime (Scotopic) vision
6Naked Eye Observations(Image Recording
Techniques)
7Film(Image Recording Techniques)
- Allows
- Objective Measurements
- Light Integration
- Features
- Higher Quantum Eff.
- Broader Spectral Allowance
8Film(Image Recording Techniques)
- Reciprocity failure
- Exp. ? Aperture ShutterTime FilmSpeed
- The law of reciprocity golden rule of
photography. Defines the relationship between
shutter time, aperture, and film speed with
respect to an exposure - Changes to any of the latter three elements are
done in stops. A stop is equal to a factor of 2
9Film(Image Recording Techniques)
- Unsharp Masking
- A form of photographic alchemy
- Subtract a blurred image to the original
- Enhance the local contrast
10Solid-State Detectors(Image Recording Techniques)
- An incoming photon kicks an electron in the
conduction band - The read-out system gives you a digital signal,
which can be numerically processed!
11Astronomical Imaging with Film(Introduction)
- Special film or photographic plates
- A method to combat reciprocity failure is
gas-hypering the film is soaked in a mixture of
hydrogen and nitrogen gas at elevated
temperatures for prolonged periods before
exposure - Very long exposure times (hours)
- Filtered Imaging
- Chemical Development
12The Birth of New Technologies
- CCD (Charge-Coupled Devices)
- CMOS (Complementary Metal Oxide Semiconductors)
- Comparing Technologies
- Companies Rule
13CCD (Charge-Coupled Devices) (The Birth of New
Technologies)
- Willard Boyle and George Smith, 1969, Bell Labs
- Working on the bubble memories
- Silicon is sensitive to light
- If exposed to light, one can grab images
14CCD (Charge-Coupled Devices) (The Birth of New
Technologies)
- Bucket Brigade
- Integration
- Charge Shift and Read-out
15CMOS(The Birth of New Technologies)
- Every pixel has its own charge-to-voltage
converter - Sensor often also includes
- Amplifiers
- Noise-correction circuitry
- Digitization circuitry
- The chip outputs digital bits
- Increased design complexity
- Reduced area for light capture
- As each pixel does its own conversion, uniformity
is lower - The chip can be built to require less off-chip
circuitry for basic operation (camera on a chip)
16Film vs. CCD(Comparing Technologies)
CCD
Film
- no loss of sensitivity to light during exposure
- reciprocity failure beyond a few second exposure
- no minimal light intensity needed to detect a
target
- minimal light intensity required to detect a
target at all
- low quantum efficiency (max. 4 at optimal
wavelengths)
- high efficiency of light detection (up to 90,
though device- and wavelength-dependent)
- signal is proportional to light intensity
- response to light is non-linear
- large dynamic range (typically 16-bit)
- small dynamic range (6-bit)
- picture elements (pixels) are regularly spaced
- picture elements (grain) are randomly distributed
- ready for digital processing
- needs to be processed in a chemical darkroom
17Film vs. CCD(Comparing Technologies)
18Film vs. CCD(Comparing Technologies)
19CCD vs. CMOS(Comparing Technologies)
20Companies Rule(The Birth of New Technologies)
- Commercial Requirements (fast read-out time, high
noise) -
- (HAD) ?
- (CMOS)
- (Super CCD)
21Trichromy(Companies Rule)
- Color Filter Array (CFA), by Dr. Bryce Bayer,
Kodak, 1970 - Where not available, color values are interpolated
22Device Shape(Companies Rule)
- Ideal shapes
- Square (easy to manufacture)
- Hexagonal (use most of focal plane area)
- Circular (use all of the focal plane area)
- Typical Width to Height factor is 43 (TV, PC
monitors, etc.)
23(Companies Rule)
- Color Filter Array (CFA), 1970
- Transparent Gate Technology, 1998 (aka Blue Plus)
to improve device sensitivity - They even sell you evaluation boards, or you can
build them on your own! http//www.kodak.com/ezpre
s/business/ccd/global/plugins/acrobat/en/eval/Koda
kAreaArrayCCDTimingGenerator.pdf
24(Companies Rule)
- HAD (Hole Accumulated Diode)
- Technique to reduce electronic noise by reducing
the dark current. - The holes created by heat or imperfections in the
creation of the imaging chip are accumulated in a
separate semiconductor layer that acts as a diode
and prevents them from returning or creating
noise. - Microlenses layers
25-(Companies Rule)
- Three CCDs Trichromy
- Philips trichroic beam-splitter
26(Companies Rule)
- Introducing CMOS devices with a 32 factor
(compatible with old fashioned film) - EOS 1Ds Mark II, 16.7 Mpxl sports a 3624mm sensor
27Fujifilm - SuperCCD(Companies Rule)
28CCD Features
29Charge Transfer Efficiency(CCD Features)
- Kodak KAF-1001 features a 10241024 image matrix
- CTE gt 0.99997 at 40 C
- If xs, ys is the horizontal/vertical position of
a pixel in the CCD matrix, charge being read by
the read-out amplifier is - Qreadout QpixelCTE(xs ys)
- The farthest pixel from the amplifier loses 6 of
its charge - If CTE 0.999 ? loss 87!!!
30Sensitivity Improvements(CCD Features)
- Front-Illuminated CCDs
- Back Illuminated (Back-Thinned) Higher QE,
Wider illuminated area, Semi-transparent to NIR - Deep Depletion (deeper photoactive region)
- Electron Multiplying CCDs A gain amplifier is
put before the output amplifier (avalanche diode)
31Technological Limitations
- Noise Sources
- CCD output stage kT/C-noise
- Semiconductor Noise Shot, Flicker, White Noise
- Resistor / Thermal Noise
- ADC Quantization Noise
- Line Frequency, 50/60 Hz
- Blooming
- Effective Energy Resolution
- Spectral Insensitivity
- Time insensitivity
32Noise Sources(Technological Limitations)
- Blind Frame around the central sensor
- Cool the sensor (-40 C)
- Take a dark frame image and subtract it from real
images
-
33Blooming(Technological Limitations)
- The charge generated into a pixel spills over
to the neighbouring ones. - At readout time, this charge can be found in the
pixels along one column/raw - Can be cured by introducing an anti-blooming
drain gate
34Effective Energy Resolution(Technological
Limitations)
- The energy needed to kick an electron in the
conduction band, in Si, is at least 1.12eV (1100
nm, far IR) - This is very good for far UV, X-rays and ?-rays
(from 100 eV and beyond), but useless in visible
(300 nm 4.1eV) - Read-out noise ( 10 e-) limits any serious
discussion about the topic in visible light
35Spectral Insensitivity(Technological
Limitations)
- A time-integrated image contains electrons
generated by photons of different energies - How to discriminate among them?
36Time Insensitivity(Technological Limitations)
- Dark subjects require long exposure times
- Time-integrated images contain electrons
generated by photons arrived at different times - Gamma ray bursts and other phenomena may require
much higher time resolution
37Basic Data Manipulation
- Dark Frame Acquisition
- Flat Field Acquisition
- Image Acquisition
- Noise Subtraction
- Gain Adjustment
38Basic Data Manipulation
- For multi-band images, repeat the processing for
any monochrome image, then stack them
39IFAE and CCDs
- DES (Dark Energy Survey)
- 500 Megapixel camera, DAQ system fast enough to
take images in 17 seconds - Galaxy Cluster counting - 20,000 clusters to z1
with M gt 2x1014 M? - Weak lensing - 300 million galaxies with shape
measurements over 5000 sq deg. - Spatial clustering of galaxies - 300 million
galaxies to z 1 and beyond - Standard Candles - 2000 SN Ia, z 0.30.8
- Multi-bandpass wide area survey, designed to
produce photometric redshifts from 0.2 lt z lt 1.3
40g, r, i, z Photometry(IFAE and CCDs)
- Gunn griz System was originally defined in terms
of photoelectric detectors (Thuan Gunn 1976
Wade et al. 1979), but is now used primarily with
CCDs - It is defined by a few dozen standard stars
- The star BD17deg4708, an F6 subdwarf with
B-V0.43, is defined to have colors equal to zero
41DES CCDs(IFAE and CCDs)
- 40962048 pixel
- Square pixels, 15µm size
- Resolution 0.27/pixel
- Back-thinned
- CTE lt 0.99999 (Lose at most 6)
- Noise lt 5 e-
42DES CCDs(IFAE and CCDs)
43Improper Applications
- X-ray Imagers (Astrophysics, Medicine)
- Cover the sensor with some fluorescent material
- High energy photons get absorbed and re-emit at
lower energy - Single-photon counting (far UV, X- and ?rays)
- Make sure that the number of photons per unit
time is AT MOST 1 per pixel - Take one image per unit time
- The charge measured per pixel is directly
proportional to the incoming photon energy
44Latest Developments
- Multi-Layer Sensors
- Originally, an April fish about CANON, in 2000
- It was actually under development at FOVEON and
released in 2002 - CMOS technology
- Principle silicon absorbs different wavelengths
at different depths - 100 of light, captured
- No colour interpolation needed
- Sigma, Polaroid and Hanvision products feature
this technology
45Alternative Technologies
- Scientists want a device with
- Reasonable noise (i.e. ? Poisson limit)
- Reasonable sensitivity (i.e ? 100)
- Reasonable space resolution (i.e. ?
diffraction limited) - Reasonable spectral resolution (i.e. ? ?E/E lt
0.1) - Reasonable time resolution (i.e. ? 0 ps)
46Bibliography Web References
- http//aberrator.astronomy.net/moon/index.html
- http//ncmi.bcm.tmc.edu/ncmi/events/workshops/work
shops_53/proceeding/2005July26_DetectingElectronsL
ecture.ppt - http//home.earthlink.net/kitathome/LunarLight/mo
onlight_gallery/technique/reciprocity.htm - http//www.lumigen.com/documents/CL_measure.shtml
- http//www.olympusfluoview.com/theory/detectorsint
ro.html - http//angryastronomer.blogspot.com/2006/06/astron
omical-data-2b-light-detection.html - http//www.fvastro.org/presentations/ImagingFilm/I
maging20with20Film.pdf - http//micro.magnet.fsu.edu/primer/digitalimaging/
concepts/concepts.html - http//www.astrosurf.com/jwisn/deepsky.htm
- http//en.wikipedia.org/wiki/Science_of_photograph
y
47Bibliography Web References
- http//www.avaloninst.com/content/raman_informatio
n/glossary.htm - http//fy.chalmers.se/astro/master/vl/lp1/photfilt
ers.pdf - http//www.cs.wisc.edu/graphics/Courses/559-s2002/
lectures/cs559-2.ppt - http//www.kodak.com/US/en/dpq/site/SENSORS/name/I
SSHome - http//www.canon.com/technology/canon_tech/explana
tion/cmos.html - http//www.fujifilm.com/about/technology/super_ccd
/ - http//www.fujifilm.com/news/n030122.html
- http//www.telescope-service.com/atik/start/atikst
art.html - http//soho.estec.esa.nl
- http//starizona.com/acb/ccd/advtheorycolor.aspx
- http//www.astrosurf.com/re/index.html
48Bibliography Web References
- http//www.foveon.com/article.php?a67
- https//www.darkenergysurvey.org/
- http//www.astro.utoronto.ca/patton/astro/mags.ht
ml - http//ulisse.pd.astro.it/Astro/ADPS/Systems/index
.html - Ron Wodaski, The New CCD Astronomy