Title: CCD-1
1Basic Principles of CCD Imaging in Astronomy
Based on Slides by Simon Tulloch available
from http//www.ing.iac.es/smt/CCD_Primer/CCD_Pri
mer.htm
2What is a CCD?
- CCD Charge-Coupled Device
- Invented in 1970s, originally for
- Memory Devices
- Arithmetic Processing of Data
- When Made of Silicon (Si), has same
Light-Sensitive Properties as Light Meters - Use them to Measure Light
- Applied to Imaging as Sensor
3CCDs in Astronomy
- Revolutionized Astronomical Imaging
- More Sensitive than Photographic Emulsions
- Factor of 100? ? Measure Light only 0.01 as
Bright - Improved Light-Gathering Power of Telescopes by
nearly 100? - Amateur w/ 15-cm (6") Telescope CCD can get
similar performance as 1960s Professional with
1-m (40") Telescope Photography - Now Considered to be Standard Sensor in
Astronomical Imaging - Special Arrangements with Observatory Now
Necessary to use Photographic Plates or Film
4What is a CCD?
- Made from Crystalline Material
- Typically Silicon (Si)
- CCD Converts Light to Electronic Charge
- Spatial Pattern of Light Produces a Spatial
Pattern of Charge Image - Digitized
- Analog Measurements (Voltages) Converted to
Integer Values at Discrete Locations - Stored as Computer File
5Si Crystal Structure
- Regular Pattern of Si atoms
- Fixed Separations Between Atoms
- Atomic Structure Pattern Perturbs Electron
Orbitals - Changes Layout of Available Electron States from
Model of Bohr Atom
http//www.webelements.com/webelements/elements/te
xt/Si/xtal.html
6Electron States in Si Crystal
- Available States in Crystal Arranged in Discrete
Bands of Energies - Lower Band ? Valence Band
- More electrons
- Upper Band ? Conduction Band
- Fewer electrons
- No States Exist in Gap Between Bands
Conduction Band of Electron States
Increasing energy
Gap 1.12 electron-volts (eV)
Gap
Valence Band of Electron States
7Comparison of State Structure in Crystal with
Bohr Model
Conduction Band
Orbitals
Valence Band
Gap
States Blur Together To Form Bands
Discrete Transition
Single Atom in Crystal
Isolated Atom (as in Gas)
8Action of Light on Electron States
- Incoming Photon w/ Energy ? 1.12 eV Excites
Electrons From Valence Band to Conduction
Band - Electron in Conduction Band Moves in the Crystal
Lattice - Excited Electron e- leaves Hole (Lack of
Electron h) in Valence Band - Hole Carrier of Positive Charge
9Action of Charge Carriers
- Carriers are Free to Move in the Band
- Electron e- in Conduction Band
- Hole h in Valence Band
- Charge Carriers may be Counted
- Measurement of Number of Absorbed Photons
10Maximum ? to Jump Si Band Gap
- 1 eV 1.602 ? 10-12 erg 1.602 ? 10-12 Joule
- ? To Energize Electron in Si Lattice Requires
- ? lt 1.1 ?m
11Energy and Wavelength
- Incident Wavelength ? gt 1.1 ?m ? Photon CANNOT be
Absorbed! - Insufficient Energy to Kick Electron to
Conduction Band - ? Silicon is Transparent to long ?
- ? CCDs constructed from Silicon are Not Sensitive
to Long Wavelengths
12After Electron is Excited into Conduction Band.
- Electron and Hole Usually Recombine Quickly
- Charge Carriers are Lost
- Apply External Electric Field to Separate
Electrons from Holes - Sweeps Electrons Away from Holes
- Maintains Population of Free Electrons
- Allows Electrons to be Counted
13Generation of CCD Carriers
photon
photon
Conduction Band
Valence Band
14Spontaneous Recombination
photon
photon
Conduction Band
Valence Band
15Prevent Spontaneous Recombination by Applying
Voltage to Sweep Electrons
??
Ammeter
16Prevent Spontaneous Recombination by Applying
Voltage to Sweep Electrons
?
?
?
?
??
Ammeter
17Thermal Noise
- Big BUT Other Kinds of Energy Have Identical
Effect - Thermally Generated Electrons are
Indistinguishable from Photon-Generated Electrons
- Heat Energy can Kick e- into Conduction Band
- Thermal Electrons appear as Noise in Images
- Dark Current
- Keep CCDs COLD to Reduce Number of Thermally
Generated Carriers (Dark Current)
18How Do We Count Charge Carriers
(Photoelectrons)?
- Must Move Charges to an Amplifier
- Astronomical CCDs Amplifier Located at Edge of
Light-Sensitive Region of CCD - Charge Transfer is Slow
- Most of CCD Area Sensitive to Light
- Video and Amateur Camera CCDs Must Transfer
Charge QUICKLY - Less Area Available to Collect Light
19Bucket Brigade CCD Analogy
- Electron Charge Generated by Photons is
Transferred from Pixel to Edge of Array - Transferred Charges are Counted to Measure
Number of Photons
20Rain of Photons
VERTICAL COLUMNS of PIXELS
BUCKETS (PIXELS)
MEASURING CYLINDER (OUTPUT AMPLIFIER)
CONVEYOR BELT (SERIAL REGISTER)
21Rain of Photons
Shutter
22Empty First Buckets in Column Into Buckets in
Conveyor Belt
MEASURING CYLINDER (OUTPUT AMPLIFIER)
CONVEYOR BELT (SERIAL REGISTER)
23MEASURING CYLINDER (OUTPUT AMPLIFIER)
CONVEYOR BELT (SERIAL REGISTER)
24Empty Second Buckets in Column Into First Buckets
25(No Transcript)
26Empty Third Buckets in Column Into Second Buckets
27Start Conveyor Belt
28(No Transcript)
29After each bucket has been measured, the
measuring cylinder is emptied, ready for the
next bucket load.
Measure Drain
30(No Transcript)
31Measure Drain
32(No Transcript)
33(No Transcript)
34Empty First Buckets in Column Into Buckets in
Conveyor Belt
Now Empty
35(No Transcript)
36Empty Second Buckets in Column Into First Buckets
37(No Transcript)
38Start Conveyor Belt
39(No Transcript)
40Measure Drain
41(No Transcript)
42(No Transcript)
43Measure Drain
44(No Transcript)
45(No Transcript)
46Measure Drain
47Empty First Buckets in Column Into Buckets in
Conveyor Belt
48(No Transcript)
49Start Conveyor Belt
50(No Transcript)
51Measure Drain
52(No Transcript)
53Measure Drain
54(No Transcript)
55Measure Drain
56Ready for New Exposure
57Features of CCD Readout
- Pixels are Counted in Sequence
- Number of Electrons in One Pixel Measured at One
Time - Takes a While to Read Entire Array
- Condition of an Individual Pixel Affects
Measurements of ALL Following Pixels - A Leaky Bucket Affects Other Measurements in
Same Column
58Leaky Bucket Loses Water (Charge)
for this Pixel
AND following Pixel
? Less Charge Measured for This Column
59Structure of Astronomical CCDs
Image Area
Package
- Image Area of CCD Located at Focal Plane of
Telescope - Image Builds Up During Exposure
- Image Transferred, pixel-by-pixel to Output
Amplifier
Connection pins Gold bond wires
Bond pads Silicon chip
Output amplifier
Serial register (Conveyor Belt)
60CCD Manufacture
Don Groom LBNL
61Fabricated CCD
Kodak KAF1401
1317 ? 1035 pixels (1,363,095 pixels)
62Charges (Buckets are Moved by Changing Voltage
Pattern
Apply Voltages Here
63Charge Transfer
64Charge Transfer - 1
5V 0V -5V
5V 0V -5V
5V 0V -5V
Time-slice shown in diagram
65Charge Transfer - 2
5V 0V -5V
5V 0V -5V
5V 0V -5V
66Charge Transfer - 3
5V 0V -5V
5V 0V -5V
5V 0V -5V
67Charge Transfer - 4
5V 0V -5V
5V 0V -5V
5V 0V -5V
68Charge Transfer - 5
5V 0V -5V
5V 0V -5V
5V 0V -5V
69Charge Transfer - 6
5V 0V -5V
5V 0V -5V
5V 0V -5V
70Charge Transfer - 7
5V 0V -5V
5V 0V -5V
5V 0V -5V
71CCD Blooming - 1
Charge Capacity of CCD pixel is Finite (Up to
300,000 Electrons) After Pixel Fills, Charge
Leaks into adjacent pixels.
Spillage
Spillage
pixel boundary
pixel boundary
Overflowing charge packet
Photons
Photons
72CCD Blooming - 2
- Channel Stops (Charge Barrier)
- Charge Spreads in Column
- Up AND Down
Charge Transfer Direction
Flow of bloomed charge
73CCD Blooming - 3
M42
- Long Exposure for
- Faint Nebulosity
- ? Star Images are
- Overexposed
Bloomed Star Images with Streaks
74CCD Image Defects
- Dark Columns
- Charge Traps Block Charge Transfer
- Charge Bucket with a VERY LARGE Leak
- Not Much of a Problem in Astronomy
- 7 Bad Columns out of 2048
- ? Little Loss of Data
75CCD Image Defects
- Bright Columns
- Electron Traps
- Hot Spots
- Pixels with Larger Dark Current
- Caused by Fabrication Problems
- Cosmic Rays (?)
- Unavoidable
- Ionization of e- in Si
- Can Damage CCD if High Energy (HST)
Bright Column
Cluster of Hot Spots
Cosmic rays
76CCD Image Defects
M51
Negative Image
Dark Column
Hot Spots, Bright Columns
- Bright First Row
- incorrect operation of
- signal processing electronics
77CCD Image Processing
- Raw CCD Image Must Be Processed to Correct for
Image Errors - CCD Image is Combination of 4 Images
- Raw Image of Scene
- Bias Image
- Dark Field Image with Shutter Closed
- Flat Field Image of Uniformly Lit Scene
78Bias Frame
- Exposure of Zero Duration with Shutter Closed
- Zero Point or Baseline Signal from CCD
- Resulting Structure in Image from Image Defects
and/or Electronic Noise - Record ? 5 Bias Frames Before Observing
- Calculate Average to Reduce Camera Readout Noise
by 1/?5 ? 45
79Dark Field Image
- Dark Current Minimized by Cooling
- Effect of Dark Current is Compensated Using
Exposures of Same Duration Taken with Shutter
Closed. - Dark Frames are Subtracted from Raw Frames
Dark Frame
80Flat Field Image
- Sensitivity to Light Varies from Pixel to Pixel
- Fabrication Problems
- Dust Spots
- Lens Vignetting
-
- Image of Uniform (Flat) Field
- Twilight Sky at High Magnification
- Inside of Closed Dome
81Correction of Raw Imagewith Bias, Dark, Flat
Images
Raw File
Dark Frame
Raw ? Dark
Flat Field Image
Output Image
Bias Image
Flat ? Bias
82Correction of Raw Imagew/ Flat Image, w/o Dark
Image
Assumes Small Dark Current (Cooled Camera)
Raw File
Raw ? Bias
Bias Image
Output Image
Flat Field Image
Flat ? Bias