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Extremely High-Efficiency Multi-Photon Emission Blue Phosphorescent
OLEDs with External Quantum Efficiency Exceeding 40%
Hisahiro Sasabe*a,b
, Kazuhiro Minamoto b
, Yong-Jin Pua,b
, Masakatsu Hirasawaa,b
, Junji Kido*a,b
aDepartment of Organic Device Engineering, Yamagata University, Yonezawa, Yamagata, 992-8510
Japan; bResearch Center for Organic Electronics (ROEL), Yamagata University, Yonezawa,Yamagata, 992-8510 Japan
ABSTRACT
We developed high-efficiency multi-photon emission (MPE) blue phosphorescent OLEDs with external quantum
efficiency exceeding 40% at 100 cd m –2
. In these MPE devices, we used a blue phosphorescent emitter, FIrpic and
pyridine-containing electron-transporters, 3,5,3’’,5’’-tetra-3-pyridyl-[1,1’;3’,1’]terphenyl (B3PyPB) and bis-4,6-(3,5-dipyridylphenyl)-2-methylpyrimidine derivatives (B3PyMPM, B4PyMPM). We also used a well-known electron-
transporter, 2,9-dimethyl-4,7-diphenylphenanthroline (BCP) for comparison. We used a combination of
TAPC/MoO3/Al/Liq layers as the charge-generation layer unit. An optimized MPE device showed an extremely high
current efficiency of over 90 cd A –1 and a high power efficiency of over 40 lm W –1 at 100 cd m –2 without any
outcoupling enhancement.
Keywords: phosphorescent OLED, electron-transport material, tandem device, charge-generation layer
1. INTRODUCTION
A tandem OLED, so-called multiphoton emission (MPE) OLED is recognized as a key technology for use in general
lighting, because we can obtain high-brightness at low current density leading to an OLED with high efficiency and long
life.[1,2] MPE device consists of multiple emissive units connected with charge generation layer (CGL). In this device,
each CGL generates electrons and holes upon voltage application. Injected holes and electrons recombine in each
emissive layers (EML). Therefore, extremely high external quantum efficiency (η ext) can be obtained. In this study, we
developed high-efficiency MPE blue phosphorescent OLEDs with EQE exceeding 40% at 100 cd m –2
.
2.
RESULTS AND DISCUSSIONPrior to the fabrication of MPE device, we evaluated FIrpic-based conventional OLEDs using a pyridine-containing
electron-transporting layer (ETL), such as 3,5,3’’,5’’-tetra-3-pyridyl-[1,1’;3’,1’]terphenyl (B3PyPB), bis-4,6-(3,5-
dipyridylphenyl)-2-methylpyrimidine derivatives (B3PyMPM, B4PyMPM)[3,4] and a well-known electron-transporter,
2,9-dimethyl-4,7-diphenylphenanthroline (BCP) for comparison (Figure 1).
N N
H3C CH3
BCP
N
N N
N
N N
N
N N
N
N NN
N N
N
CH3 CH3
B3PyPB B3PyMPM B4PyMPM
Figure 1. Chemical structures of materials
We fabricated a blue phosphorescent OLED with a structure of [ITO (130 nm) / TAPC (60 nm) / TCTA: 7wt% FIrpic
(5 nm) / TCTA: FIrpic 20wt% (5 nm) / ETL (20 nm) / ETL: 25 wt% Liq (35 nm) / Liq (1 nm) / Al (100 nm)].
* [email protected]; phone +81 238 26-3924; fax +81 238 26-3412; yamagata-univ.
Invited Paper
Organic Light Emitting Materials and Devices XVI, edited by Franky So, Chihaya Adachi,Proc. of SPIE Vol. 8476, 847604 · © 2012 SPIE · CCC code: 0277-786X/12/$18 · doi: 10.1117/12.927997
Proc. of SPIE Vol. 8476 847604-1
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EL spectra showed an emission only from FIrpic with no emission from neighboring materials (inset in Figure 2(b)).
The current density–voltage – luminance ( J–V–L) and the power efficiency–luminance ( PE–L) characteristics are shown
in Figure 2(a) and Figure 2(b), respectively. A reference OLED using BCP gave a very poor η ext of ~5.6% and an η p of
~10 lm W –1 probably because of two factors: (a) much lower E T (2.63 eV) than that of FIrpic (2.77 eV) and (b) lower
carrier balance. Among pyridine-containing ETLs, B3PyPB showed superior performances in FIrpic-based OLED
despite the high-lying E a of 2.62 eV. B3PyPB-based OLED showed much reduced driving voltage of 2.87 V at 100 cd
m
–2
, and gave an η p,100 of 56.5 lm W
–1
(51.6 cd A
–1
, η ext,100 21.8%) at 100 cd m
–2
and 43.2 lm W
–1
(46.3 cd A
–1
, η ext,100 19.6%) at 1000 cd m
–2, respectively. These are among the best performances in FIrpic-based OLEDs. Whereas
B3PyMPM- and B4PyMPM-based OLEDs showed lower η ext of ~15% and η p,100 of ~30 lm W –1
indicating carrier
imbalance in EML.
Figure 2. (a) J–V–L characteristics and (b) PE–L characteristics of blue OLEDs using B3PyPB (circle), B3PyMPM
(square) and B4PyMPM (triangle), respectively. Inset: EL spectra of the devices.
B3PyPB (20 nm)
TAPC (60 nm)
ITO
TCTA: 7 FIrpic (5 nm)
TCTA: 20 FIrpic (5 nm)
B3PyPB: 25 wt% Liq (35 nm)
Liq (1 nm)
Al
1 unit device
B3PyPB (55 nm)
TAPC (60 nm)
ITO
TCTA: 7 FIrpic (5 nm)
TCTA: 20 FIrpic (5 nm)
Liq (1 nm)
Al (1 nm)
B3PyPB (55 nm)
TAPC (60 nm)
MoO3 (5 nm)
TCTA: 7 FIrpic (5 nm)
TCTA: 20 FIrpic (5 nm)
Liq (1 nm)
Al
MPE I
TAPC (60 nm)
ITO
TCTA: 7 FIrpic (5 nm)
TCTA: 20 FIrpic (5 nm)
Liq (1 nm)
Al (1 nm)
B3PyPB (20 nm)
TAPC (60 nm)
MoO3 (5 nm)
TCTA: 7 FIrpic (5 nm)
TCTA: 20 FIrpic (5 nm)
Liq (1 nm)
Al
B3PyPB: 25wt% Liq (35 nm)
B3PyPB (20 nm)
B3PyPB: 25wt% Liq (35 nm)
MPE II
Figure 3. Device structure of 1 unit device, MPE I and MPE II.
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0 1 2 3 4 5 6 7
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d e n s i t y ( m A c m
2 )
L umi n an c e ( c d m
2 )
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(a)
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Next, we fabricated two types of MPE devices using Liq. Device structures are shown in Figure 3. MPE I is using Liq,
and MPE II is using Liq-doped B3PyPB layer. As a reference, we also showed 1 unit device. J–V and QE–L
characteristics are shown in Figure 4(a) and Figure 4(b), respectively. By using Liq as an EIL, performances in MPE
device were clearly improved. Especially, MPE II using Liq-doped B3PyPB gave superior performances.[5] MPE II
showed much reduced driving voltage of 6.93 V at 100 cd m –2, which is 2.4 times higher than that in 1 unit device. An
η p,100 of 40.8 lm W –1 (90.0 cd A –1, η ext,100 41.1%) at 100 cd m –2 and 28.4 lm W –1 (77.6 cd A –1, η ext,100 35.4%) at 1000 cd
m
–2
were also obtained. These are highest performances in a blue phosphorescent OLEDs so far.
Figure 4. (a) J–V characteristics and (b) QE–L characteristics of blue OLED using conventional structure (circle), Liq
(triangle) and Liq-doped B3PyPB (square) respectively.
3. CONCLUSION
By using FIrpic and pyridine-containing electron-transporter B3PyPB, we successfully developed extremely high-
efficiency MPE blue phosphorescent OLEDs with an η ext,100 exceeding 40%. To maximize a FIrpic-based OLED
performance, we pointed out the importance of high-lying E a level as well as high E T for an ETL due to the deep I p of
FIrpic. These findings will provide a guideline to design a next-generation ETL for a high-performance blue phosphorescent OLED. In these MPE OLEDs, we introduced a combination of TAPC/MoO3/Al/Liq layers as a CGL
unit. For CGL unit, Liq plays a critical role to reduce a driving voltage of a MPE device. An optimized MPE OLED
showed an extremely high η c,100 of over 90 cd A –1
and a high η p,100 of over 40 lm W –1
without any outcoupling
enhancement. These performances are the highest in a blue phosphorescent OLED so far. We believe that this MPE
concept will provide a key solution for a high-performance white OLED for general lighting.
REFERENCES
[1]
Kido, J., Matsumoto, T., Nakada, T., Endo, J., Mori, K., Kawamura, N. and Yokoi, A., "High Efficiency Organic
EL Devices having Charge Generation Layers," SID 03 Digest 964-995 (2003).
[2]
Matsumoto, T., Nakada, T., Endo, J., Mori, K., Kawamura, N., Yokoi A. and Kido, J., "Multiphoton Organic EL
Device having Charge Generation Layers," SID 03 Digest 979-981 (2003).[3]
Sasabe, H., Gonmori, E., Chiba, T., Li, Y-J., Tanaka, D., Su, S-J., Takeda, T., Pu, Y-J., Nakayama, K. and Kido, J.,
"Wide-Energy-Gap Electron-Transport Materials Containing 3,5-Dipyridylphenyl Moieties for an Ultra High
Efficiency Blue Organic Light-Emitting Device," Chem. Mater. 20, 5951-5953 (2008).
[4]
Sasabe, H. and Kido, J., "Multifunctional Materials in High-Performance OLEDs: Challenges for Solid-State
Lighting," Chem. Mater. 23, 621-630 (2011).
[5]
Endo, J., Matsumoto, T. and Kido, J., "Organic Electroluminescent Devices Having Metal Complexes as Cathode
Interface Layer," Jpn. J. Appl. Phys. 41, L800-L803 (2002).
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