efficiency engineering of blue, green and yellow oleds · ref: h. heil et al, sid 2014, 35.1. 14...
TRANSCRIPT
𝜂𝑒𝑥𝑡 = 𝛾 ∗ 𝜒 ∗ 𝜙 ∗ 𝜂𝑜𝑢𝑡
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Introduction
External Quantum Efficiency in OLEDs
charge
balance
radiative
exciton ratio
PL quantum
yield
light
outcoupling
external
quantum efficiencyHow to influence
by materials?
Transport materials
(e/h)
Emissivematerials
(host/dopant)
Charge balanceand confinement
Indirectly by e.g. stimulating TTA/
avoiding quenching
RefractiveIndex/
scattering
Emissivemechanism
DopantPLQY
Emissive dipoleorientation
(Mixed) host type&ratio
Exciplexforming host
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Agenda
New Fluorescent Blue Dopant Development
Highly Oriented Phosphorescent Emissive Systems
Tuning Efficiency by Transport Layers
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Blue OLED performance is strongly influenced by a phenomenological charge balance law, which typically leads to a trade-off between LT and efficiency.
Observation
Efficiency and lifetime as function of charge balance
To tune OLED performance, it is key to understand the charge balance regime a given device is operating in
Ref: E. Böhm et al, IDW’09, OLED1-2
Statistics with various ETL configuartions: Reducing e-transport by diluting ETL:
ETM diluter [%]
Blue OLED performance is strongly influenced by a phenomenological charge balance law, which typically leads to a trade-off between LT and efficiency.
De-tunedregime
De-tunedregim
e
Efficiency optimizedregime
Balancedregime
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Charge balance – Influence of transport layers
The key to tune and understand HTM/ETM performance in blue
e-rich/h-poor
Eff
icie
ncy
Only changingcharge balance
Efficiency / LT plots help to understand and categorize charge-balance induced performance changes
e-poor/h-rich
LT
Eff
icie
ncy
LT
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Example
Merck’s Electron Transport Material portfolio (selection)
ETM portfolio covering a wide range of charge balance for tuning between LT and eff.
more e-transporting
less e-transporting
ETL
Blue EML
EBL
HTL
p-doped HTL
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Example
Merck’s Electron Blocking Material portfolio for s-blue (selection)
• HTM portfolio for tuning between LT and efficiency by choice of EBL• Interaction with choice of ETL has to be considered
h-poor
h-rich
Same order of materials but different curvature
ETL
Blue EML
EBL
HTL
p-doped HTL
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Example
Interaction between HTL and EBL
• Strong interaction with HTL• Most efficient EBL in one device can be least efficient in another!
Eff
icie
ncy
LT
Reminder
HOMO
HTL EBL HTL EBL HTL EBL ETL
Blue EML
EBL
HTL
p-doped HTL
h-poor h-rich
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Is it only charge balance?
Influence of triplet-triplet annihilation (TTA)
• TTA plays a role in efficiency increase of e-rich OLED “charge balance induced TTA”
• However, other mechanisms must be involved
Measurement method: Results:
0.00
0.10
0.20
0.30
0.40
0.50
-10 0 10 20
EL [a
.u.]
t [µs]
DEL (delayed EL)
Steady-state EL
DEL/Steady-state EL
applied on
e-diluter EQE @10mA/cm²
DEL ratio@10mA/cm²
EQE withoutDEL
50% 7.3% 31% 5.6%
70% 5.6% 23% 4.6%
75% 4.6% 11% 4.1%
e-p
oor
ETL:diluter
Blue EML
EBL
HTL
p-doped HTL
ETM diluter [%]
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How about green OLED?
Merck’s Electron Blocking Material portfolio for green (selection)
• Efficiency / LT trade-off is typically also present in phosphorescent green OLEDs• Wide EBL portfolio range available for green OLED
Established generation
New generation
ETL
Green EML
EBL
HTL
p-doped HTL
„Charge Balance“ is often
dominating the LT/efficiencyperformance
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Key Messages
Tuning efficiency by transport layers
Portfolio approach is key for offeringTransport Layers.
Interplay between HTL/EBL/HBL/ETL determines overall performance.
Extensive combination screening isnecessary to optimize OLED stack.
• Actively developing materials for various OLED layers to understand full stack• Significant investments in physics / application lab resources
Merck‘sapproach
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Agenda
Tuning Efficiency by Transport Layers
Highly Oriented Phosphorescent Emissive Systems
New Fluorescent Blue Dopant Development
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In 2014, Merck introduced a novel ultra-deep blue dopant (peak <450nm)
Review
Introduction of ultra-deep blue dopant
• Ultra-deep blue dopant with excellent color and lifetime properties• However, EQE limited due to dopant PLQY of 0.8
Ref: H. Heil et al, SID 2014, 35.1
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New development
Ultra-deep blue dopant with improved efficiency
• Successor dopant with similar characteristics but 10% higher PLQY• Ideally suited for ultra-deep blue bottom emission application
95
96
97
98
99
100
101
0 50 100
rel. lu
m. [%
] @
60
mA
/cm
²
time [h]
0
2
4
6
8
10
12
0 2000 4000 6000
EQ
E [%
]
luminance [cd/m²]
0
0,2
0,4
0,6
0,8
1
1,2
400 500 600
EL n
orm
. [a
rb. u
nits]
wavelength [nm]
Al
1 nm LiQ
30 nm ETL:LiQ
20 nm Blue EML
10 nm EBL
160 HTL
20 nm HTL:p-doped
ITO
Dopant PLQY EL peak FWHM CIE x/y Voltage@10mA/cm²
Lum. Eff. @10mA/cm²
EQE@10mA/cm²
LT95 @60mA/cm²
LT95 @1000cd/m²
Old 0.80 447 nm 30 nm 0.148 / 0.080 4.0 V 6.0 cd/A 8.0 % 78 h ~400 h
New 0.88 449 nm 26 nm 0.146 / 0.078 4.0 V 6.5 cd/A 8.9 % 76 h ~450 h
Old
New
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Agenda
Tuning Efficiency by Transport Layers
New Fluorescent Blue Dopant Development
Highly Oriented Phosphorescent Emissive Systems
Measurement method: Simulation: Results:
Molecular dynamics sim.
Optical excitation of film by polarized laser of evaporation process
Measurement of PL spectra (angularly res.)
Fit optical model to obtain dopant orientation
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Dopant orientation
Preferred dipole orientation parallel to substrate
New ph.-yellow dopants with significant suppression of perpendicular orientation
Dopant Orientation simulated(p|| : p┴)
Orientation measured(p|| : p┴)
Isotropic 2:1
Perfectorientation
2:0
New Yellow 1 2:0.68 2:0.58
New Yellow 2 2:0.43 2:0.44
Ref: Appl. Phys. Lett. 96, 073302 (2010) Similar method to:
Nature Comm. 8, 791 (2017)
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Dopant orientation
Phosphorescent yellow dopants with improved efficiency
Dopant Orientation measured
EQE @ 2000 cd/m²
Ir(bzq)3 2:1(assumed)
19.6%
New Yellow 1 2:0.58 25.4%
New Yellow 2 2:0.44 29.8%
Up to x1.5
EQE
increase!
• Close to 30% EQE from a conventional bottom emission OLED!• Concept will be transferred to green dopants
Al
ETL:Liq (x%)
Yellow EML
EBL
HTL
p-doped HTL
ITO
- Ir(bzq)3
- New Yellow 1
- New Yellow 2
New ultra-deep blue dopant with increasedefficiency
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Summary
Merck offers a rich material portfolio addressing efficiency topics
Typically dominating efficiency tuning bytransport layers
New highly efficient phosphorescent yellowdopants
Charge Balance
PLQY
Emitter Orientation
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