• types of organic materials
• growth of organic materials
• organic light emitting devices
• OLED-based displays
Lecture 7
6.976 Flat Panel Display Devices
Emissive Displays –
Organic Electroluminescence
Flexible OLED
Organic Materials
Alq 3
PPV
MOLECULAR MATERIALS
POLYMERS
Attractive due to:
Attractive due to:
• Integrability with inorganic semiconductors •
• Low cost • (fabric dyes, biologically derived materials)
• Large area bulk processing possible •
• Tailor molecules for specific •
electronic or optical properties
• Unusual properties not easily attainable • with conventional materials
But problems exist:
But problems exist:
• Stability •
• Patterning •
• Thickness control of polymers •
• Low carrier mobility •
n
Scientific Interest in Organic Materials
• 1828 - Wöhler first synthesized urea
without the assistance of a living organism
• 1950’s - steady work on crystalline organics starts
• 1970’s - organic photoconductors (xerography)
• 1980’s - organic non-linear optical materials
• 1987 - Kodak group published the first
efficient organic light emitting device (OLED)
• Since then, the field has dramatically expanded both commercially and scientifically
(OLEDs, transistors, solar cells, lasers, modulators, ... )
to date, about two million organic compounds have been made to date, about two million organic compounds have been made
- this constitutes nearly 90% of all known materials -
- this constitutes nearly 90% of all known materials -
VACUUM CHAMBER TURBO
PUMP COLD TRAP
ROUGHING PUMP
substrate holder thickness
monitor shutter
GND
substrate
POWER SUPPLIES
source boats
Device Preparation and Growth
• Glass substrates precoated with ITO - 94% transparent
- 15 Ω/square
• Precleaning Tergitol, TCE
Acetone, 2-Propanol
• Growth
- 5 x 10
-7Torr - Room T
- 20 to 2000 Å
layer thickness
OMBD II OMBD I Sputtering
Analysis Chamber
Load Lock
Materials Growth Laboratory
III-V MBE
Load Lock Transfer
Chamber Metal
e-Beam
Base Pressure 10
-9~ 10
-11torr
Princeton
Princeton University University
Integrated Materials Growth System
Evaporative Deposition
• molecular organics
(amorphous and crystalline)
• metals
Sputtering
• ITO
• ceramics
Wet N2 Glove Box
Load Lock
with Sample Storage Ante Chamber
and Oven
Laminar Flow Hood
Dry N2 Glove Box Shadow Mask Storage
Probe Station with Cryostat
AFM STM
Physical & Vapor Phase Dep.
• molecular organics
• nano-dots **
• solvated polymers **
• colloids **
• Spin-on
• Langmuir-Blodgett
• Inkjet Printing
• Dye Diffusion
• Silkscreen
Other Growth Methods
glass substrate ITO
doped polymer film highly doped polymer film
glass substrate
}
}
DIFFUSION SOURCE
SHADOW MASK
DEVICE
Development of Organic LEDs
• Conventional, Transparent, Inverted, Metal-Free, Flexible, Stacked
~ OLED, TOLED, OILED, MF-TOLED, FOLED, SOLED ~
• Displays
Personal Organizer, Personal Organizer,
Notebook Notebook
Rugged, high resolution, full-color, video-rate
displays
Multi-Function Multi-Function
Video Watch Video Watch
Rugged, high resolution, full-color, video-rate displays enable a multitude
of applications
Automotive Automotive
Dashboard displays, external indicator lights,
and road signs
Active Wallpaper Active Wallpaper
Large area displays
Active Clothing Active Clothing
Light, rugged, low voltage,
flexible displays
Why do OLEDs Glow ?
+
electrons and holes form excitons excitons (bound e - -h + pairs)
some excitons radiate some excitons radiate
HOMO LUMO
rec ombination regi on
ETL HTL
E
_
V +
-
Glass ITO Alq
3TPD Mg:Ag
Ag
400 500 600 700 800 Alq
3PL
OLED EL
Wavelength [nm]
Alq 3
Al N
O 3
TPD
N N
~1000 Å
~500 Å
~500 Å
Electroluminescence
Single Layer Device
Heterostructure Device
ITO Al
2.1 eV 2.4 eV CN-PPV
PPV
h νννν
ITO Ca
h νννν
PPV
EXCITON RECOMBINATION
CARRIER TRANSPORT CARRIER
INJECTION
Exciton Recombination Zone
C. Adachi, et al.
1 10 10
-1110
-1010
-910
-810
-710
-610
-510
-410
-3T=141K T=180K T=240K T=295K
Cu rren t [ A ]
Voltage [V]
4 6 8
5 10 15
Tt = 1780 K
m
1/T [10-3/K]
HOMO LUMO
trap level
molecule distorts
E
Trap Limited Conduction in Organic Materials
charge trapping can dominate conduction
free molecule
molecule distorts
Þ Þ
Þ Þ ∆∆∆∆ E _
_
_
∆∆∆∆ E
N t =3.1x10 18 cm -3 ,
µµµµ n N LUMO =4.8x10 14 /cm-V-s J ∝ N LUMO µµµµ n N t m d -2m-1 V m+1
m = T t /T
Shen, Burrows, Bulovic, McCarty, Thompson, Forrest,
Jpn. J. Appl. Phys. 35, L401 (1996). ´
Progress in LED Efficiency
after Sheats et al., Science 273, 884 (1996).
M ol ec ul ar S ol id s
OLEDs
PLEDs
WE DEMONSTRATED
WE DEMONSTRATED OLEDs OLEDs THAT ARE : THAT ARE :
• Bright - 100,000 cd/m2 (30,000 ft-L)
• Efficient - >30 lm/W
• Scalable Emissive Area - from a few µµµµ m to a few cm in size
• Colors - fluorescent R,G,B and phosphorescent R,G
• Low Voltage - 3 to 10 V
• Low Cost Materials
• Low Cost Substrates
• Wide Viewing Angle - >160 deg
• Reliability - 1,000,000 hrs (phosphorescent R half-life)
Why Make Organic LEDs
Alq 3 devices driven at 20 mA/cm 2 Initial luminance for Alq 3 is 510 cd/m 2
for QA doped Alq 3 devices is 1600 cd/m 2
and for MQA doped Alq 3 devices is 1400 cd/m 2 (C.W. Tang)
QA/Alq
MQA/Alq
Alq
Hours of operation Rela tive l u mina nce [L /L
0]
1.0
0.9
0.8
0.7
0.6
0.5 1 5 10 50 100 1000 10000
OLED Stability
Electroluminescence in Doped Organic Films
2.
Excitons transfer to luminescent dye
1.
Excitons formed from combination
of electrons and holes
6.0 eV a-NPD
2.6 eV
5.7eV
Alq
32.7 eV electrons
exciton
trap states
low work function cathode
transparent anode holes
host molecules (charge transport
material)
dopant molecule
(luminescent dye)
400 500 600 700 800 0.0
0.2 0.4 0.6 0.8 1.0
Nor m alized EL I n tensit y
Wavelength [nm]
Alq
3PtOEP:Alq
3DCM2:Alq
3N Pt N N N Al N
O 3
O NC CN N
αααα -NPD
N N
Effect of Dopants on the OLED EL Spectrum
Solid State Solvation Effect
Bulovic ´et al., Chem. Phys. Lett. 287, 455 (1998); 308, 317 (1999).
Alq Alq
33DCM2 in Alq DCM2 in Alq
33low DCM2
low DCM2 high DCM2 high DCM2
500 600 700 800
0.0 0.2 0.4 0.6 0.8
1.0 10%
5%
2%
1%
EL Intens ity [a.u. ]
Wavelength [nm]
Alq
3DCM2 in Alq
3EL Spectrum Tuning EL Spectrum Tuning
Temporal Response Temporal Response
0.25 ns 0.50 ns
0.75 ns
1.00 ns 1.50 ns 2.00 ns
5.00 ns
4 8 12 16
0
600 650 700 750
35 nm 35 nm wavelength shift
10% DCM2 in Alq
310% DCM2
in Alq
3In te n s it y [a .u .]
host
dopant (chromophore)
with DIPOLE MOMENT µµµµ
Influence of µ 0 and µ 1
on Chromatic Shift Direction
solvent solute (chromophore)
WITH DIPOLE MOMENT µµµµ
µ 0 < µ 1 µ 0 < µ 1
SOLVENT POLARITY
S 0 S 1
ground state excited
state
µ 0 > µ 1 µ 0 > µ 1
SOLVENT POLARITY
S 0 S 1
∆∆∆∆ E
Solid State Solvation Effect (SSSE)
E loc R
dipolar host with moment µ
polar lumophore
áááá µµµµ ññññ > > > > 0 áááá µµµµ ññññ → → → → 0
as R → large
“self polarization”
for strongly dipolar lumophores
500 600 700 800 900 0.0
0.2 0.4 0.6 0.8 1.0
1%
2%
5%
10%
20%
In te n s it y [a .u .] 50%
Wavelength [nm]
0.0 0.2 0.4 0.6 0.8 1.0
Intensit y [a. u .] 1%
2%
5%
10%
20% 100%
DCM2 in Alq Alq 3 3
DCM2 in Zrq Zrq 4 4
polar host µµµµ ~ 5.5 D
non-polar host
Thin Film Photoluminescence
400 500 600 700 120 Å BCP
80 Å BCP 40 Å BCP 0.0
0.2 0.4 0.6 0.8 1.0
Wavelength [nm]
400 500 600 700
In ten s ity [a .u.]
0.6%
1.5%
3%
6%
0.0 0.2 0.4 0.6 0.8 1.0
In ten s ity [a .u.]
changing DCM2 in α -NPD
concentration
(with 40A BCP)
changing BCP layer
thickness
(with 0.6% DCM2)
TPD
Ag Mg:Ag
ITO glass Alq 3
BCP
NPD:DCM2
Tuning
Emission of
White OLEDs
• symmetry conserved fast process ~10 -9 s
• triplet to ground state transition is not permitted
slow process ~ 1s
Fluorescence
E
ground state (singlet) singlet excited state
triplet excited state
S 1 T 1
S 0
FLUORESCENCE FLUORESCENCE
singlet exciton singlet exciton
E
Phosphorescence
PHOSPHORESCENCE PHOSPHORESCENCE
triplet exciton triplet exciton
S 1 T 1
S 0
0 1 2 3 4 5 6 7 8 9 10 0.1
1 10 100 1,000 10,000 100,000
Lumina n ce [cd/m
2]
Voltage [V]
0 5 10 15 20 25 30
P o w e r E ffi c ie n c y [l m/ W]
10,000 cd/m
2Phosphorescent OLED Performance
N N
CBP
Ir
3 N
Ir(ppy) 3 6% Ir(ppy) 3 in CBP OLED:
at 100 cd/m 2 : 4.5 V, 19 lm/W at 10,000 cd/m 2 : 7.2 V, 8 lm/W
100 cd/m
2Simulated Power Consumption
(5 inch/320x240 pixels monochrome display) 33% pixels “on”
UDC, Inc.
0 100 200 300 400 500 600 700 800
Po wer [mW ]
0 50 100 150 200
Brightness [nits]
PM - Fl uo re sc en t
PM - P hos pho res cen t
AM - Phosp horescent
AM - Flu ores ecen t
A ML CD
Monochrome Passive-Matrix Polymer-LED Display
Cambridge Display Technologies, Ltd.
Full-Color OLED Display
Kodak - Sanyo
Transparent Substrate:
Glass, Plastic, Metal
Low Cost Potential
ITO Anode Multi-Color Icons
Organic LED Transparent Cathode
• Lower cost materials than LCDs
• Fewer process steps than LCDs
• Less capital cost than LCDs
15” XGA Cost Comparison
0 50 100 150 200 250 300 350 400
AMLCD LTPS/OLED
US$
Other Labor
Module Material Cell Material Array Material
Equipment Depreciation Building Depreciation
Source: DisplaySearch
AT SAME YIELDS
TECHNOLGY/
FEATURES
AMLCD PMLCD LED PDP FED OLED
Brightness Good Good Very
Good Good Good Very
Good
Resolution High High Low Medium High High
Voltage Low Low High High High Low
Viewing Angle Medium Poor Excellent Excellent Excellent Excellent Contrast Ratio Good Fair Good Poor-
Good
Good Excellent Response Time Good Poor Fast Very Fast Very Fast Very Fast Power Efficiency Good Good Fair-
Good Medium Very
Good Very
Good Temp Range Poor Poor Very
Good
Very Good
Very Good
Very Good
Form Factor Thin Thin Wide Wide Thin Very Thin
Conformable
Weight Light Light Above
Avg.
Heavy Light Light
Screen Size Small-
Large Small to
Medium Small to
Large Large Medium Small to Large Primary
Applications Laptops,
Desktop Small
Display Signs,
Indicators Large
Screen Multiple Multiple New/Existing
Cost Average Low High High Average Below
Average
Technology Landscape
Transparent OLEDs
Parthasarathy et al., Appl. Phys. Lett. 72, 2138 (1998).
-
V
+
EL Light
500 Å
500 Å ITO ETL HTL ITO Glass
EL Light
50-100 Å
50-100 Å Mg-Ag
Bulovic et al., Nature 380, 29 (1996). ´
> 70% transparent
Alphanumeric TOLED Display Alphanumeric TOLED Display
TOLEDs MF-TOLEDs
TOLED Applications
UDC, Inc.
E1 E2 E4 E3 E5
Glass substrate
Red
E1 E2 E3
E4 E5
R-G-B light
Stacked Organic LEDs (SOLEDs)
head-up, high resolution, true-color, high-contrast, brightly-emissive, flexible displays
Shen et al., Science 276, 2009 (1997).
Gu et al., J. Appl. Phys. (1999).
0.0 0.2 0.4 0.6 0.8
0.0 0.2 0.4 0.6 0.8
y
x
YELLOW YELLOW
BLUE BLUE
RED RED ORANGE ORANGE GREEN
GREEN
WHITE WHITE
PURPLE PURPLE
PINK PINK
450 400 480 490
500 520
550 560 540
580 600
650 700 530
Microcavity Effects Microcavity Effects
Bulovic et al.,
Phys. Rev. B 58, 3730 (1998).
´
Glass
ITO
Mg:Ag Electrode ααα
α - NPD
RADIATION RADIATION
Modes Modes
WAVEGUIDE WAVEGUIDE
Modes Modes
Surface Surface Plasmons Plasmons Metal
Metal Losses Losses
emissionEDGE SURFACE
emission
Alq3
Θ
k- EL Region -
MATERIAL THICKNESS [Å] n
Mg:Ag 1000 ----
Ag 1000 ----
αααα -NPD 540 1.78
ITO 490 2.02
3% DCM2 in Alq
3330 1.72
Alq
3170 1.72
Alq’
2OPh 390 1.66
αααα -NPD 250 1.77
CuPc 80 1.5+0.8i
Alq
350 1.72
Mg:Ag 80 ----
Alq
3540 1.72
αααα -NPD 445 1.77
ITO 1600 1.8
Glass ~1 mm 1.45
V 4
V 1 V 2 V 3
MI CR O C A V IT Y 1 MI CR O C A V IT Y 2 RE D OLED BLUE OLED GREEN OLED
Example of a Stacked OLED Structure
Up to 3 times the resolution of conventional displays
Advantages of Stacked OLEDs
True-Color Pixels
AMLCD
OLED backlight
TOLED stack
}
G R B
~ 1mm
for full-color displays for full-color displays the backlight can consist of a the backlight can consist of a stack
stack of R,G, and B TOLED backlights of R,G, and B TOLED backlights
Organic LED Backlight Integrated with an AMLCD
TOLED Stack
R - on G - off B - off
Principle of OLED Backlight Operation
R G B sub-cycles
one display write cycle
ON OFF ON
OFF ON
OFF
R sub-cycle
time
ON OFF