When organic light emitting diodes (OLEDs) appeared commercially aming to replace conventional display devices in early 2000s, it was not easy to guess OLEDs would become a dominant lighting source in display and lighting products industry. With abili...
When organic light emitting diodes (OLEDs) appeared commercially aming to replace conventional display devices in early 2000s, it was not easy to guess OLEDs would become a dominant lighting source in display and lighting products industry. With ability of displaying colors in higher quality and wider viewing angle than those of liquid crystal display (LCD), and its adaptability to other technology from being able to be flexible and transparent, now OLEDs have become the ultimate display means. However, there are unsolved issues that need to draw our attention.
Competition rose between phosphorescent and fluorescent OLEDs especialy to take better position for the commercial blue OLED. Blue phosphorescent OLEDs exhibit highly efficient blue light, however the stability issue still need to be cleared and further, phosphorescent OLEDs are considered to be toxic for containing heavy metal complex. Therefore, blue fluorescent OLEDs are being used commercially in spite of their low EL efficiency from limitation of exciton production portion of singlet to ~25%.
Theoretically, if singlet-triplet splitting () is small enough, then reverse intersystem crossing (RISC) can take place harvesting additional triplets in fluorescent OLEDs. In order to have small, it is necessary to have spatial separation of the highly occupied molecular orbital (HOMO) and the lowest occupied molecular orbital (LUMO). Recently, by taking advantage of small, efficient intra- and intermolecular charge transfer (CT) materials have been reported, which are referred to thermally activated delayed fluorescence (TADF) material and excited charge transfer complex (exciplex) system, respectively. Especially, OLEDs adopting exciplex system exhibit high EL efficiency from efficient energy transfer (ET) of host to dopant material and charge balance in emission layer (EML).
Further investigating into the method to boost EL efficiency in fluorescent OLEDs, there are sensitizing and heavy atom effect (HAE). Implementing phosphorescent or TADF material in EML working as assisted dopants in organized structure of cascading enegy levels of singlet and triplet among the constituents, improved EL efficiencies in fluorescent OLEDs were reported. Also, in CT type host material, HAE can be induced to improve EL efficiency of fluorescent OLED by enhancing mixing of singlet and triplet state taking advantage of both the sensitizing and HAE.
In this dissertation, the work is focused on the investigation of full potential of fluorescent OLEDs, especially blue fluorescent OLEDs, attempting to answer the series of questions: 1) Is it possible to turn all the triplets into light in fluorescent OLED? 2) Can there be efficient host system for blue fluorescent OLED? 3) Is it possible to achieve high EL efficiency and color purity in a same blue fluorescent OLED, simultaneously? 4) Is it possible to achieve high EL efficiency in conventional blue fluorescent OLEDs?
Starting from the first question of the possibility of achieving high EL efficiency in fluorescent OLED equivalent to that of phosphorescent OLED. In Chapter 2, 100% internal quantum efficiency (IQE) is achieved in a green fluorescent OLED exhibiting 30% external quantum efficiency (EQE) comparable to that of phosphorescent OLED. The OLED comprises an exciplex-forming cohost system doped with a fluorescent dye that has a strong delayed fluorescence as a result of reverse intersystem crossing (RISC); the exciplex-forming cohosts contributed efficient ET and charge balance in the system. Large distribution of exciton in exciplex cohost lowered exciton density in EML resulting in the smallest efficiency roll-off among the other reported OLEDs using the same fluorescent emitter. The orientation of the transition dipole moment of the fluorescent dye is shown to have an influence on the EQE of the device.
Motivated by the result of the highly efficient green fluorescent OLED using exciplex cohost system in Chapter 2, the efficient mixed cohost system for blue fluorescent OLED was investigated in Chapter 3. Selecting host material for blue emitter is particulary difficult for the requirement of high triplet energy, therefore the majority of reported efficient blue fluorescent OLEDs have been dependent on the same single host material of high triplet energy, which arouse the second question for efficient host system for blue fluorescent OLEDs. The efficient mixed cohost suggested in this work boosted electorluminescence (EL) efficiency of the blue fluorescent OLED by fully utilizing the ability of blue TADF emitter. The EQE was increased from previously reported ~13% to 21.8% from perfect charge balance through bipolar character of the mixed cohost. The achieved EQE was the highest among the blue fluorescent OLEDs of the same emitting material in the single host. The achieved EQE was one of the highest EQEs in blue fluorescent OLEDs and identical to the theoretically achievable maximum EL efficiency using the emitter under consideration of none electrical loss.
Through the works in chapter 2 and 3, the fluorescent OLED was proven to be able to achieve the equivalent EL efficiency to that of phosphorescent OLED achieving 100% IQE, and highly efficient blue fluorescent OLED based on the mixed cohost was reported, therefore the motivation of further investigating into the potential of blue fluorescent OLEDs has risen. Despite of numerous reports on efficient blue fluorescent OLEDs, not many have achieved color purity and high EL efficiency at the same time. In Chapter 4, the mixed cohost was further utilized to realize deep blue emission and high EL efficiency at the same time using blue TADF emitter based on azasiline unit. For electroluminescence with delayed fluorescence, the azasiline unit has been introduced for the first time as a donor in a TADF material. The TADF material of 5-(4-(4,6-diphenyl-1,3,5-triazin-2-yl)phenyl)-10,10-diphenyl-5,10-dihydrodibenzo[b,e][1,4]azasiline (DTPDDA) shows strong intramolecular CT character with large spatial separation with the acceptor of triazine leading to narrow splitting of singlet and triplet excited states for the efficient RISC. A blue OLED based on DTPDDA not only displayed deep blue emission in the Commission Internationale de L’Eclairage (CIE) coordinates of (0.149, 0.197) but also exhibited EQE of 22.3% which is the highest value ever reported for a blue fluorescent OLED. Theoretical prediction based on transient photoluminescence (PL) and optical simulation result agrees well with the achieved EQE indicating the successful conversion of triplet excitons to singlet in the blue fluorescent OLED by using DTPDDA.
In Chapter 5, further utilizing azasiline unit for blue TADF emitter, donor-connector-acceptor (D-C-A) and donor-acceptor-donor (D-A-D) type blue TADF emitters were implemented into the mixed cohost in order to investigate the full potential of blue fluorescent OLEDs based on azasilin unit. Utilizing the azasiline unit, 5-(4’-(4,6-diphenyl-1,3,5-triazin-2-yl)-[1,1’-biphenyl]-4-yl)-10,10- diphenyl-5,10-dihydrodibenzo[b,e][1,4]azasiline (DTPPDDA), the TADF blue emitter of D-C-A type resulted in deep blue emission with CIE coordinate of (0.151, 0.087), close to the blue standard of the National Television System Committee (NTSC) of (0.140, 0.080) with 4.7% EQE. In D–A–D type materials of bis(4-(10,10-diphenyldibenzo[b,e]-[1,4]azasilin-5(10H)-yl)phenyl)methanone (BDAPM) and 5,5’-(sulfonylbis(4,1-phenylene))bis(10,10-diphenyl-5,10-dihydro dibenzo[b,e][1,4]azasiline) (SPDDA), carbonyl and sulfone units were used as the acceptors where the azasiline moeity was used as the donor unit, respectively. The sulfonyl unit contributed to a large twist of the molecular structure while the carbonyl unit led to a small twist of the molecular structure. As a result, the blue fluorescent OLEDs containing BDAPM and SPDDA demonstrated 11.4% and 2.3% EQEs with CIE y-values of 0.310 and 0.107, respectively.
However, emitting from TADF material often shows broad EL spectrum due to strong CT state of the material, and the stability of the TADF based OLEDs still need to be improved. As an alternative, conventional fluorophore can be used as an emitter, where assisted dopants either phosphorescent or TADF material is strategically implemented to enhance spin mixing of singlet and triplet excited states. Recently, the high EL efficiencies were reported from blue fluorescent OLEDs based on conventional blue fluorescent dye, taking advantage of TADF material as a sensitizer. With smallof TADF material, RISC can occur effectively harvesting additional triplet excitons. Also, adopting heavy metal compound of platinum or iridium enhances spin mixing of singlet and triplet from HAE, consequently EL efficiency of OLED can be improved. Even more, increased spin reversal of triplet to singlet was observed by taking advantage of CT state of host on the induction of HAE from iridium complex, eventually enhancing the singlet to triplet ratio (ηs/T). In Chapter 6, almost all the triplets were harvested in the conventional blue fluorescence OLED by promoting both sensitizing and HAE through co-doping TADF material and phosphorescent material into EML. Comparison of the theoretical and experimental data indicates that ηs/T was increased from 0.23 to 0.94 with increased EQE from 5.6% to 12.3% in blue fluorescent OLED when the both TADF material and phosphorescent material were doped together as assisted dopants, indicating the nearly all the triplets harvested in the conventional blue fluorescent OLED.