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8. Introduction to Displays and Imaging Systems
39

8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Dec 22, 2015

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Page 1: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

8. Introduction to Displays and Imaging Systems

Page 2: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Radiation Sources

Bohr’s atomic model:

• Nucleus (protons+neutrons), surrounding orbits (electrons)

• Electrons absorb energy to reach higher orbits

• High Low energy level + Radiation

The origins of radiation:

Page 3: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Classification of Radiation Source (1)

1. Classification by Flux Output -- Point source Eg. LED, small filament clear bulb -- Area source Eg. Frosted light bulb -- Collimated source Eg. Search light -- Coherent source Eg. Laser

Page 4: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Classification of Radiation Source (2)

2. Classification by Wavelength and Color (in visible region)

-- Hue (色相 ) Eg. blue , red , green (color)

-- Saturation (飽和度或彩度 ) Eg. pink—red with less saturation (purity)

-- Intensity (強度 ) Eg. flux density of a radiating source

Note : Primary colors : Red (700nm) , Green (546nm) , Blue (440nm)

Note : Chroma (彩色度 ) : combination of hue and saturation

C=R+G+B , where G , R , B are primary flux component

Page 5: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Classification of Radiation Source (3)

3. Classification by radiation spectrum

-- Continuous spectrum Eg. thermally excited source incandescent bulb)

-- Line spectrum Eg. gas discharge and phosphorescent source (螢光 )

-- Single wavelength Eg. source radiated only in a narrow band of wavelength (LED)

-- Mono chromatic source Eg. lasers

Page 6: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Classification of Radiation Source (4)

4. Classification by source excitation

-- Thermal excitation Eg. heating (incandescent bulb)

-- Electroluminescence (EL , 場致發光 ) Eg. LED

--Vacuum fluorescence Eg. CRT , TV tube , X-ray machine

-- Chato-luminescence (閃光發光 ) Eg. Low pressure gas-filled tube , plasma ,

gas discharge devices

-- Lasing Eg. Electroluminascedce and chemical exciting method

Page 7: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Classification of Radiation Source (4’)

Page 8: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Liquid Crystals

Three types of liquid crystals: Cholesteric, Nematic, and Smectic

Page 9: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Liquid Crystal Display (LCD) LCD includes light source, liquid crystal, polarizer, color filter (CF), thin film tansistor (TFT), and so on.

TFT controls orientation of liquid crystal, and Black Matrix fills in the gap between color filters.

Page 10: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Output Light Intensity Depending on the Orientation of Liquid Crystal

Page 11: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Colorful PixelThe pixels are addressed in rows and columns, reducing the connection complexity. The column and row wires attach to transistor switches, one for each pixel.

Controlling color filter to adjust the transmissions of three primary colors, one can obtain various colors.

Page 12: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Colorful Pixel (Cont’)

Page 13: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Overall Descriptions of TFT- LCD

Page 14: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

TFT-LCD Component

Page 15: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Array/Cell Structure & Equivalent Circuit

Page 16: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Function of TFT Devices

• In the TFT-LCD, TFT device acts as a switch to conduct electric current charging the LC capacitor and storage capacitor.

• When the TFT device is turned on, the signal is written (recorded) into the LC capacitor. With TFT turned-off, the signal will be locked on the LC capacitor and prevent it from being leaky.

Page 17: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Passive Matrix Liquid Crystal Display (PMLCD) and Active Matrix Liquid Crystal Display (AMLCD)

Page 18: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Transmission/voltage Characteristics

Page 19: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Directional Characteristics

Page 20: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Response Time

Page 21: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Contrast

Note : To design a display with maximum contrast or contrast ratio

)(cd/m luminance sourceor object :

)(cd/m luminance backgroung:

10 ,

2

2

o

B

o

BO

L

L

CL

LLC

For passive display (eg: LCD)

)(cd/m luminance sourceor object :

)(cd/m luminance backgroung:

1 ,

2

2

o

B

B

o

L

L

CL

LC

For active display (eg: LED)

Page 22: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Brightness : Perception of Luminance

Page 23: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Plasma Display

Plasma display panel

Page 24: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Electroluminescent Source

Electroluminescence Excitation of electron by electric field

+ Dielectric with embedded phosphor

Page 25: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Electroluminescent Source (cont’)Source luminance is a function of (1) voltage (2) frequency (3) temperature

Page 26: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Eletroluminescent Display

Display cell (pixel) ~ -

(resolution : 3 lines/mm)

Number of pixel ~ 65,000 – 250,000 pixels

25.05.0 mm 225.025.0 mm

Electroluminescent dot matrix display Electroluminescent display panel

Page 27: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Vacuum Fluorescent SourceVacuum fluorescent

high-speed electron + phosphor

Vacuum fluorescent display

Page 28: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Cathode Ray Tube (CRT)

Page 29: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Cathode Ray Tube (cont’)

Page 30: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Spatial Light Modulators (SLMs)

Two major classes of SLM:— electrically addressed SLM— optically addresses SLM

Spatial light modulator — SLM can modulate certain properties of wavefronte.g., amplitude, intensity, phase, or polarization.

SLM information-bearing element

Major applications of SLM:— electro-optic system— optical signal processing— optical interconnection— optical computing

Page 31: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Magneto-optic Modulators

Faraday effect: rotation of polarization by magnetic field = VBd V: Verdet constant

B: magnetic fieldd: travel distance in the medium

Operations of M-O Modulator:— magneto-optic effect — electrically addressed SLM— binary amplitude/phase modulation — switching speed: ~ 10 ns— frame rate: 100-300 Hz (256256 pixels)— spatial resolution: center-to-center distance between pixels 70 m— contract ratio: 300:1@633nm— transmittance: 5%

Page 32: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Pockel’s Readout Optical Modulators (PROMs)

Operations of PROMs:— Pockel,s effect (linear electro-optic effect) e.g., e-o crystal: BSO— Optically addressed SLM (inconherent to conherent conversion/wavelength conversion)— amplitude and phase modulation, and optical logic operation— writing energy: 5~600 J/cm2

— spatial resolution: 100 lines/mm— contract ratio: 10,000:1— write-read-erase cycle: 30 frames/s (at video rate; write and erase times < 1ms)

Pockel’s effect: n E n: induced birefringence

E: applied electric field

Page 33: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Liquid Crystal Light Valves (LCLVs)

Operations of LCLV:— twisted nematic liquid crystal— optically addressed SLM— inconherent-to-conherent converter/ wavelength converter— amplitude and phase modulation— writing energy: 10 J/cm2

— spatial resolution: 60 lines/mm— contract ratio: 100:1— readout time: 10 ms

Page 34: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Liquid Crystal Television (LCTV)

Operations of LCTV:— twisted nematic liquid crystal (90o)— electronically addressed SLM— amplitude and phase modulation— low cost and programmability— writing energy: 10 J/cm2

— spatial resolution: (1) 640480 pixels (2) center-to-center distance between pixels 50 m— contract ratio: 100:1— frame rate: 60 Hz

Page 35: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Microchannel Plate Spatial Light Modulators (MSLMs)

Operations of LCTV:

— linear electro-optic effect (LiNbO3)

— optically addressed SLM

— inconherent-to-conherent converter/

wavelength converter

— very high sensitivity~30nJ/cm2

— spatial resolution: 20~50 lines/mm

— contract ratio: 1000:1

— writing time: 10 ms

Page 36: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Photoplastic Devices

Operations of photoplastic device:

— Charge Exposure Recharge Develop Erase

— phase modulation/phase grating

— light sensitivity~ J/cm2

— spatial resolution: ~2000 lines/mm

— diffraction efficiency: ~ 10% @60 J/cm2

— lifetime: 300-2000 cycles

Page 37: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Deformable Mirror Array Devices (DMDs)

Operations of DMD:

— micro-mirror deformation

— electrically addressed 2-D phase modulator

— spatial resolution: (1) 128128 ~ 10001000 pixels

(2) 10 lines/mm

— frame rate: ~150 frames/s

— contrast ratio: ~100:1

Page 38: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Optical Disks

Operations of ODs:

— optical discs

— binary phase modulating SLM

— spatial resolution:

track separation: 1.6 m

width of a pit: 0.5~0.7 m

(typically, /NA1.55)

Page 39: 8. Introduction to Displays and Imaging Systems. Radiation Sources Bohr’s atomic model: Nucleus (protons+neutrons), surrounding orbits (electrons) Electrons.

Photorefractive Crystals

Operations of Photorefractive Crystals:

— Photorefractive effect

— E-O crystals e.g., LiNbO3, BaTiO3, SBN

— light induced phase modulation

— refractive index grating:

n n0(1-e-t/)

: photorefractive response time

n0: maximum refractive index change

t: exposure time