Charge balance in OLEDs: Optimization of hole injection layer using novel p‐dopants

Charge balance is one of the most important factors for realizing high performance organic light emitting devices (OLEDs). In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer (HIL) as well as the electron transporting layer (ETL) an...

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Veröffentlicht in:Journal of the Society for Information Display 2024-02, Vol.32 (2), p.71-81
Hauptverfasser: Xie, Menglan, Pang, Huiqing, Wang, Jing, Cui, Zhihao, Ding, Hualong, Zheng, Renjie, Kwong, Ray, Xia, Sean
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container_title Journal of the Society for Information Display
container_volume 32
creator Xie, Menglan
Pang, Huiqing
Wang, Jing
Cui, Zhihao
Ding, Hualong
Zheng, Renjie
Kwong, Ray
Xia, Sean
description Charge balance is one of the most important factors for realizing high performance organic light emitting devices (OLEDs). In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer (HIL) as well as the electron transporting layer (ETL) and thereby controlling the charge carrier supplies in the device. First, we develop a p‐dopant material (PD02), with a lowest unoccupied molecular orbit (LUMO) of −4.63 eV, much shallower than that of the commercial material (PD01) of which the LUMO is −5.04 eV. Nevertheless, this enables us to modulate the supply of holes to the emissive layer through tuning doping concentration. We demonstrate that device performances are significantly improved by employing such a scheme. With a 23% molar doping of PD02, a bottom emission red OLED achieves an external quantum efficiency (EQE) of over 30%, an operating voltage of 3.4 V and a LT95 ~15,000 h at 10 mA/cm2, with a Digital Cinema Initiative P3 (DCI‐P3) chromaticity of CIE (X, Y) = (0.68, 0.32). Moreover, the efficiency roll‐off is suppressed up till ~3500 cd/m2, a desirable feature in display applications. The lateral conductivity of by using such HIL is also found to be much lower than that of PD01, resulting in reduced crosstalk among RGB pixels. Next, a new electron transporting material (ETM‐02) with a deep LUMO of −2.86 eV is also introduced to further optimize the charge balance. Although devices with ETM‐02 shows lower voltage and higher EQE, lifetime is compromised. In order to improve lifetime, additional fine tuning of the charge balance is essential. Finally, a second p‐dopant PD03 with a LUMO of −4.91 eV is added to the HIL to further extend the modulation flexibility in the hole injection. A double‐layer HIL consisting of 8 nm of HTM:16% PD02 and 2 nm of HTM:3% PD03, where the former is in contact with anode, is adopted in the device structure. The bottom emission deep red device achieve EQE over 30%, an operating voltage of 3.2 V and an improved LT95 ~13,000 h at 10 mA/cm2 with a BT.2020 range chromaticity of CIE (X, Y) = (0.701, 0.299). In the double HIL configuration, the introduction of PD03 provides one more parameter for tuning and therefore improves the overall device performances. Charge balance is one of the most important factors for realizing high performance OLEDs. In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer and the e
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In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer (HIL) as well as the electron transporting layer (ETL) and thereby controlling the charge carrier supplies in the device. First, we develop a p‐dopant material (PD02), with a lowest unoccupied molecular orbit (LUMO) of −4.63 eV, much shallower than that of the commercial material (PD01) of which the LUMO is −5.04 eV. Nevertheless, this enables us to modulate the supply of holes to the emissive layer through tuning doping concentration. We demonstrate that device performances are significantly improved by employing such a scheme. With a 23% molar doping of PD02, a bottom emission red OLED achieves an external quantum efficiency (EQE) of over 30%, an operating voltage of 3.4 V and a LT95 ~15,000 h at 10 mA/cm2, with a Digital Cinema Initiative P3 (DCI‐P3) chromaticity of CIE (X, Y) = (0.68, 0.32). Moreover, the efficiency roll‐off is suppressed up till ~3500 cd/m2, a desirable feature in display applications. The lateral conductivity of by using such HIL is also found to be much lower than that of PD01, resulting in reduced crosstalk among RGB pixels. Next, a new electron transporting material (ETM‐02) with a deep LUMO of −2.86 eV is also introduced to further optimize the charge balance. Although devices with ETM‐02 shows lower voltage and higher EQE, lifetime is compromised. In order to improve lifetime, additional fine tuning of the charge balance is essential. Finally, a second p‐dopant PD03 with a LUMO of −4.91 eV is added to the HIL to further extend the modulation flexibility in the hole injection. A double‐layer HIL consisting of 8 nm of HTM:16% PD02 and 2 nm of HTM:3% PD03, where the former is in contact with anode, is adopted in the device structure. The bottom emission deep red device achieve EQE over 30%, an operating voltage of 3.2 V and an improved LT95 ~13,000 h at 10 mA/cm2 with a BT.2020 range chromaticity of CIE (X, Y) = (0.701, 0.299). In the double HIL configuration, the introduction of PD03 provides one more parameter for tuning and therefore improves the overall device performances. Charge balance is one of the most important factors for realizing high performance OLEDs. In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer and the electron transporting layer and thereby controlling the charge carrier supplies in the device. 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In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer (HIL) as well as the electron transporting layer (ETL) and thereby controlling the charge carrier supplies in the device. First, we develop a p‐dopant material (PD02), with a lowest unoccupied molecular orbit (LUMO) of −4.63 eV, much shallower than that of the commercial material (PD01) of which the LUMO is −5.04 eV. Nevertheless, this enables us to modulate the supply of holes to the emissive layer through tuning doping concentration. We demonstrate that device performances are significantly improved by employing such a scheme. With a 23% molar doping of PD02, a bottom emission red OLED achieves an external quantum efficiency (EQE) of over 30%, an operating voltage of 3.4 V and a LT95 ~15,000 h at 10 mA/cm2, with a Digital Cinema Initiative P3 (DCI‐P3) chromaticity of CIE (X, Y) = (0.68, 0.32). Moreover, the efficiency roll‐off is suppressed up till ~3500 cd/m2, a desirable feature in display applications. The lateral conductivity of by using such HIL is also found to be much lower than that of PD01, resulting in reduced crosstalk among RGB pixels. Next, a new electron transporting material (ETM‐02) with a deep LUMO of −2.86 eV is also introduced to further optimize the charge balance. Although devices with ETM‐02 shows lower voltage and higher EQE, lifetime is compromised. In order to improve lifetime, additional fine tuning of the charge balance is essential. Finally, a second p‐dopant PD03 with a LUMO of −4.91 eV is added to the HIL to further extend the modulation flexibility in the hole injection. A double‐layer HIL consisting of 8 nm of HTM:16% PD02 and 2 nm of HTM:3% PD03, where the former is in contact with anode, is adopted in the device structure. The bottom emission deep red device achieve EQE over 30%, an operating voltage of 3.2 V and an improved LT95 ~13,000 h at 10 mA/cm2 with a BT.2020 range chromaticity of CIE (X, Y) = (0.701, 0.299). In the double HIL configuration, the introduction of PD03 provides one more parameter for tuning and therefore improves the overall device performances. Charge balance is one of the most important factors for realizing high performance OLEDs. In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer and the electron transporting layer and thereby controlling the charge carrier supplies in the device. Red OLEDs with improved performance were achieved.</description><subject>charge balance</subject><subject>Chromaticity</subject><subject>cross talk</subject><subject>Crosstalk</subject><subject>Current carriers</subject><subject>deep red</subject><subject>device optimization</subject><subject>Dopants</subject><subject>Doping</subject><subject>doping concentration</subject><subject>double HIL</subject><subject>efficiency roll‐off</subject><subject>Electric potential</subject><subject>Electron transport</subject><subject>electron transport material</subject><subject>Electrons</subject><subject>Emission</subject><subject>EQE</subject><subject>ETL</subject><subject>hole injection, p‐dopant</subject><subject>hole transport material</subject><subject>HOMO</subject><subject>LUMO</subject><subject>OLED</subject><subject>operating voltage</subject><subject>Optimization</subject><subject>Organic light emitting diodes</subject><subject>phosphorescent emitter</subject><subject>Quantum efficiency</subject><subject>recombination zone</subject><subject>Voltage</subject><issn>1071-0922</issn><issn>1938-3657</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp1kL1OwzAQgC0EEqUw8AaWmBjS-i9OwobaAkWVOkBny7Gd1lEaBzsFlYlH4Bl5EpKWlelOd9_96APgGqMRRoiMy2D1CJMEn4ABzmgaUR4np12OEhyhjJBzcBFC2aE8ZnwAVpON9GsDc1nJWhloa7hczKbhDi6b1m7tp2ytq6Er4MZVfbs06lCp5N54uAu2XsPavZsKNj9f39o1sm7DJTgrZBXM1V8cgtXD7HXyFC2Wj_PJ_SJSJO7-IcwUhdFJTvNMJQQbw4hhXKcZSzRNdZxiwqTUChW54oQmmEquM8aYVjHROR2Cm-Pexru3nQmtKN3O191JQTKKU84R4x11e6SUdyF4U4jG2630e4GR6K2J3prorXXs-Mh-2Mrs_wfF88t8epj4BaXEb70</recordid><startdate>202402</startdate><enddate>202402</enddate><creator>Xie, Menglan</creator><creator>Pang, Huiqing</creator><creator>Wang, Jing</creator><creator>Cui, Zhihao</creator><creator>Ding, Hualong</creator><creator>Zheng, Renjie</creator><creator>Kwong, Ray</creator><creator>Xia, Sean</creator><general>Wiley Subscription Services, Inc</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SC</scope><scope>8FD</scope><scope>JQ2</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope><orcidid>https://orcid.org/0000-0002-0174-1463</orcidid><orcidid>https://orcid.org/0009-0006-7634-985X</orcidid><orcidid>https://orcid.org/0000-0001-7215-3899</orcidid></search><sort><creationdate>202402</creationdate><title>Charge balance in OLEDs: Optimization of hole injection layer using novel p‐dopants</title><author>Xie, Menglan ; 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In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer (HIL) as well as the electron transporting layer (ETL) and thereby controlling the charge carrier supplies in the device. First, we develop a p‐dopant material (PD02), with a lowest unoccupied molecular orbit (LUMO) of −4.63 eV, much shallower than that of the commercial material (PD01) of which the LUMO is −5.04 eV. Nevertheless, this enables us to modulate the supply of holes to the emissive layer through tuning doping concentration. We demonstrate that device performances are significantly improved by employing such a scheme. With a 23% molar doping of PD02, a bottom emission red OLED achieves an external quantum efficiency (EQE) of over 30%, an operating voltage of 3.4 V and a LT95 ~15,000 h at 10 mA/cm2, with a Digital Cinema Initiative P3 (DCI‐P3) chromaticity of CIE (X, Y) = (0.68, 0.32). Moreover, the efficiency roll‐off is suppressed up till ~3500 cd/m2, a desirable feature in display applications. The lateral conductivity of by using such HIL is also found to be much lower than that of PD01, resulting in reduced crosstalk among RGB pixels. Next, a new electron transporting material (ETM‐02) with a deep LUMO of −2.86 eV is also introduced to further optimize the charge balance. Although devices with ETM‐02 shows lower voltage and higher EQE, lifetime is compromised. In order to improve lifetime, additional fine tuning of the charge balance is essential. Finally, a second p‐dopant PD03 with a LUMO of −4.91 eV is added to the HIL to further extend the modulation flexibility in the hole injection. A double‐layer HIL consisting of 8 nm of HTM:16% PD02 and 2 nm of HTM:3% PD03, where the former is in contact with anode, is adopted in the device structure. The bottom emission deep red device achieve EQE over 30%, an operating voltage of 3.2 V and an improved LT95 ~13,000 h at 10 mA/cm2 with a BT.2020 range chromaticity of CIE (X, Y) = (0.701, 0.299). In the double HIL configuration, the introduction of PD03 provides one more parameter for tuning and therefore improves the overall device performances. Charge balance is one of the most important factors for realizing high performance OLEDs. In this work, we provide a novel strategy to improve the charge balance in OLEDs by optimizing the hole injection layer and the electron transporting layer and thereby controlling the charge carrier supplies in the device. Red OLEDs with improved performance were achieved.</abstract><cop>Campbell</cop><pub>Wiley Subscription Services, Inc</pub><doi>10.1002/jsid.1271</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-0174-1463</orcidid><orcidid>https://orcid.org/0009-0006-7634-985X</orcidid><orcidid>https://orcid.org/0000-0001-7215-3899</orcidid></addata></record>
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subjects charge balance
Chromaticity
cross talk
Crosstalk
Current carriers
deep red
device optimization
Dopants
Doping
doping concentration
double HIL
efficiency roll‐off
Electric potential
Electron transport
electron transport material
Electrons
Emission
EQE
ETL
hole injection, p‐dopant
hole transport material
HOMO
LUMO
OLED
operating voltage
Optimization
Organic light emitting diodes
phosphorescent emitter
Quantum efficiency
recombination zone
Voltage
title Charge balance in OLEDs: Optimization of hole injection layer using novel p‐dopants
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