Balancing charge-transporting characteristics in bipolar host materials
Introduction
The use of white organic light emitting diodes (WOLEDs) as a lighting source has received growing attention as the next-generation lighting [1], [2], [3], [4], [5], [6], [7]. The production cost of WOLEDs should be reduced to improve the price competitiveness against a conventional lighting device. OLED devices prepared via a conventional vacuum process show improved efficiency; however, the equipment for this vacuum process is very expensive. One of the most probable methods to reduce the production cost is utilization of a solution process. The process of forming a single organic active layer by mixing electrons and hole transporting materials combined with active materials is used in the soluble OLED process worldwide. The lifetime and efficiency of the OLED device with a single active layer are drastically reduced if the organic active layer containing various materials is phase separated by deterioration, resulting from its continuous usage [8,9], or if inhomogeneities occur due to the relative miscibility difference [10,11]. Thus, utilization of a bipolar host material both reduces the numbers of mixed material and helps maintain the device stability [8]. A bipolar host containing both hole- and electron-transporting moieties facilitates the charge balance in the emitting layer, resulting in broad charge recombination zones [12], which reduces the triplet-triplet annihilation and leads to high efficiency and decreased efficiency roll-off [13,14].
Recently, OLEDs using phosphorescence have been employed worldwide as a lighting application because of their excellent efficiency. Bipolar hosts for solution-processable phosphorescence OLEDs require large energy gaps, high charge carrier mobility for both electrons and holes, high thermal stability and high solubility. The hosts with carbazole moieties have been extensively used in phosphorescence OLEDs because of their good hole mobility and high intrinsic triplet energy (~ 3.02 eV) [15]. OLED lighting usually employs white light, which is obtained by mixing blue and yellow emitters [16] or mixing blue, green and red emitters [17]. Thus, the bipolar host material must exhibit good transport properties for various band gaps [18], [19], [20].
In this study, solution-processable bipolar host materials were synthesized, and the charge-transporting properties for the hole and electron were controlled by attaching different sizes of alkyl groups, thus changing the molecular spatial geometries. WOLEDs were fabricated through a solution process. The device characteristics demonstrated that the host materials with balanced charge-transporting properties exhibits enhanced electroluminescence properties.
Section snippets
Synthesis of 9H-thioxanthene-9-one-S,S-dioxide (1)
Hydrogen peroxide (35% aqueous solution, 8 g, 235 mmol) was added to a solution of thioxanethene-9-one (25 g, 118 mmol) in acetic acid (400 mL) at room temperature. The resulting mixture was placed under reflux for 2 h and then cooled to room temperature to yield a precipitate, which was filtered and washed with n-hexane (400 mL) to produce yellow crystal. (Yield: 93%) 1H NMR (300 MHz, CDCl3, δ): 8.35(dd, J= = 7.5 Hz. J= = 1.5 Hz, 2H), 8.19 (dd, J= = 7.5 Hz. J= = 1.5 Hz, 2H), 7.88 (td, J
Results and discussion
The bipolar hosts composed of 9,9-Bis(9-alkylcarbazole)thioxanthene-S,S-dioxide were synthesized by a solvent-less green reaction method [21]. Here, the alkyls were ethylhexyl (BH1), octyl (BH2), dodecyl (BH3), and heptadecane (BH4) and were synthesized by multi-step reactions, as shown in Fig. 1. The thioxanthene-S,S-dioxide moiety possessed good electron-transporting ability, whereas the bis-alkylcarbazole moiety has good hole-transporting ability. The thermal properties of each compound were
Conclusions
The bipolar host materials demonstrated excellent thermal stability based on the TGA and DSC measurements. All four host materials showed quite similar thermal characteristics. The HOMO level of the host materials was obtained from the oxidation potential measured using CVs, whereas the LUMO level was calculated from the band gap estimated from the band edge of the absorption spectrum. The optimized molecular geometries and spatial distributions were obtained using the Gaussian 03 program. The
Declaration of Competing Interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgments
This work was supported by the Industrial Technology Innovation Program (Grant no. 10063277, Development of pattern deposition system based on roll to roll processing under low temperature and atmospheric pressure condition for smart thin film device fabrication) funded by Ministry of Trade, Industry & Energy.
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