2015
DOI: 10.1039/c5cc00307e
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High efficiency pure blue thermally activated delayed fluorescence molecules having 10H-phenoxaborin and acridan units

Abstract: Highly efficient blue thermally activated delayed fluorescence molecules having 10H-phenoxaborin and acridan units were reported. Pure blue emission peaking at around 450 nm with a high external electroluminescence quantum efficiency of around 20% was demonstrated.

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Cited by 298 publications
(231 citation statements)
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“…Interestingly, triarylboron derivatives have often been opposed to donors, such as 9,10-dihydroacridine, triphenylamine of the popular carbazole group [91][92][93]. Some of them even show CIE coordinates of (0.15, 0.09) and (0.15, 0.08) for the PL of emitters in toluene but none of them gave OLEDs with colour coordinates satisfying or being close to the NTSC blue standard of CIE coordinates (0.14, 0.08) [94]. Recently, Hatakeyama et al reported a new strategy to design effective deep blue triarylboron based emitters [95].…”
Section: Triarylborane Emittersmentioning
confidence: 99%
“…Interestingly, triarylboron derivatives have often been opposed to donors, such as 9,10-dihydroacridine, triphenylamine of the popular carbazole group [91][92][93]. Some of them even show CIE coordinates of (0.15, 0.09) and (0.15, 0.08) for the PL of emitters in toluene but none of them gave OLEDs with colour coordinates satisfying or being close to the NTSC blue standard of CIE coordinates (0.14, 0.08) [94]. Recently, Hatakeyama et al reported a new strategy to design effective deep blue triarylboron based emitters [95].…”
Section: Triarylborane Emittersmentioning
confidence: 99%
“…17,22 Such subvertical D-A structure can suppress the conjugation between D and A segments, and strictly isolate the HOMO and LUMO orbitals on D and A segments, respectively. [17][18][19][20]22 Till now, nearly all of the reported TADF emitters are based on such design strategy, and successfully exhibit high efficiencies in the devices. However, without the restriction from the conjugation between D and A segments, the structural relaxations of TADF emitters become evident, resulting in increased Stokes shift and broadened emission spectra.…”
Section: Introductionmentioning
confidence: 99%
“…32 Thus, it is impossible to realize high efficiencies in OLED displays with current TADF emitters. 17,[29][30][31][32] Most recently, Hatakeyama and his co-workers successfully utilized the multiple resonance effect to construct TADF emitters with extremely narrow FWHM. 32 However, this strategy is strictly confined to specific molecular structure and inapplicable for current D-A structure TADF emitters; and the OLEDs based on their new TADF emitters suffer serious efficiency roll-off and extremely low maximum luminance of about 200 cd m -2 .…”
Section: Introductionmentioning
confidence: 99%
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“…[19][20][21][22][23] However, these OLEDs can only utilize singlet excitons for electroluminescence (EL) and the resulting internal EL quantum efficiency (η int ) is limited to 25% because of the inherent spin-statistical limitation of electrical excitation, which generates radiative singlet excitons and non-radiative triplet excitons in a 1:3 ratio. 24 Recent research efforts in our group 25 and others [26][27][28][29][30] have focused on exploring AIE-active materials that simultaneously exhibit thermally activated delayed florescence [31][32][33][34][35][36][37][38][39] to harvest triplet excitons for EL via efficient reverse intersystem crossing. To expand the library of such unique fluorophores that display aggregation-induced delayed fluorescence (AIDF), we report on two yellow AIDF materials, PTZ-XT and PTZ-BP ( Figure 1) that consist of an electron-donating phenothiazine unit coupled with an electron-accepting xanthone or benzophenone unit.…”
Section: Introductionmentioning
confidence: 99%