Photoelectron Spectroscopic Study of C12A7:e-and Alq3Interface:  The Formation of a Low Electron-Injection Barrier

2007 ◽  
Vol 111 (24) ◽  
pp. 8403-8406 ◽  
Author(s):  
Ki-Beom Kim ◽  
Maiko Kikuchi ◽  
Masashi Miyakawa ◽  
Hiroshi Yanagi ◽  
Toshio Kamiya ◽  
...  
2010 ◽  
Vol 114 (28) ◽  
pp. 12258-12264 ◽  
Author(s):  
Pierluigi Gargiani ◽  
Antonio Calabrese ◽  
Carlo Mariani ◽  
Maria Grazia Betti

2011 ◽  
Vol 15 (09n10) ◽  
pp. 964-972
Author(s):  
Ronghua Guo ◽  
Lijuan Zhang ◽  
Yuexing Zhang ◽  
Yongzhong Bian ◽  
Jianzhuang Jiang

Density functional theory (DFT) calculations were carried out to investigate the semiconductor performance of a series of phthalocyaninato zinc complexes, namely Zn[Pc(β-OCH3)8] (1), ZnPc (2), and Zn[Pc(β-COOCH3)8] (3) {[ Pc(β-OCH3)8]2- = dianion of 2,3,9,10,16,17,23,24-octamethoxyphthalocyanine; Pc2- = dianion of phthalocyanine; [ Pc(β-COOCH3)8]2- = dianion of 2,3,9,10,16,17,23,24-octamethoxycarbonylphthalocyanine} for organic field effect transistor (OFET). The effect of peripheral substituents on tuning the nature of phthalocyaninato zinc semiconductor has been clearly revealed. Introduction of eight weak electron-donating methoxy groups onto the peripheral positions of ZnPc (2) leads to a decrease in the hole injection barrier relative to Au electrode and an increase in the electron injection barrier, making compound 1 a better p-type semiconductor material in comparison with 2. In contrast, peripheral methoxycarbonyl substitution depresses the energy level of LUMO and thus induces an increase for the electron affinity (EA) value of ZnPc (2), resulting in the change of semiconductor nature from p-type for ZnPc (2) to n-type for Zn[Pc(β-COOCH3)8] (3) due to the improved electron injection ability. The calculated charge transfer mobility for hole is 1.05 cm2.V-1.s-1 for 1 and 5.33 cm2.V-1.s-1 for 2, while that for electron is 0.16 cm2.V-1.s-1 for 3. The present work should be helpful for designing and preparing novel phthalocyanine semiconductors in particular with good n-type OFET performance.


ACS Omega ◽  
2018 ◽  
Vol 3 (8) ◽  
pp. 10008-10018 ◽  
Author(s):  
Apostolis Verykios ◽  
Michael Papadakis ◽  
Anastasia Soultati ◽  
Maria-Christina Skoulikidou ◽  
George Papaioannou ◽  
...  

2016 ◽  
Vol 18 (48) ◽  
pp. 33077-33084 ◽  
Author(s):  
Dipjyoti Das ◽  
Peddaboodi Gopikrishna ◽  
Rahul Narasimhan ◽  
Ashish Singh ◽  
Anamika Dey ◽  
...  

The influence of the electron injection barrier on charge transport, brightness and EL properties of WPLEDs with PVK as an emissive layer has been reported.


2010 ◽  
Vol 46 (43) ◽  
pp. 8210 ◽  
Author(s):  
Toan V. Pho ◽  
Peter Zalar ◽  
Andres Garcia ◽  
Thuc-Quyen Nguyen ◽  
Fred Wudl

2020 ◽  
Vol 20 (7) ◽  
pp. 4364-4367 ◽  
Author(s):  
Da-Young Park ◽  
Jae-Hoon Lim ◽  
Bum-Joo Lee ◽  
Dae-Gyu Moon

Zinc oxide (ZnO) nanoparticles layers are used as a substitute for organic electron transport layer due to high electron mobility, higher thermal stability and less sensitivity to the oxygen/moisture. In this study, we investigated the electron injection properties of ZnO nanoparticles in QLED compared with TPBi commonly used as injection layer in OLEDs. The expected electron injection barrier from energy diagram is similar in both devices, but the current density of the ZnO injection layer was slightly high compared with the TPBi injection layer. The current efficiency of ZnO and TPBi devices were 5.21 cd/A and 2.24 cd/A, respectively. The current efficiency of TPBi device is below half of ZnO device. We found that the electron–hole recombination occurs not only in the QD but also in the poly-TPD for TPBi device.


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