scholarly journals Simulation of Nonpolar p-GaN/i-N/n-GaN Solar Cells

2012 ◽  
Vol 2012 ◽  
pp. 1-8 ◽  
Author(s):  
Ming-Jer Jeng

It is well known that nitride-based devices suffer the polarization effects. A promising way to overcome the polarization effects is growth in a direction perpendicular to thec-axis (nonpolar direction). Nonpolar devices do not suffer polarization charge, and then they have a chance to achieve the high solar efficiency. The understanding of the solar performance of non-polar InGaN-based solar cells will be interesting. For a pin non-polar solar cell with GaN p- and n-cladding layers, the conduction band offset (or barrier height, ) between an intrinsic layer and n-GaN layer is an important issue correlating to the efficiency and fill factor. The efficiency and fill factor will be seriously degraded due to sufficiently high barrier height. To reduce a high barrier height, some graded layers with an energy bandgap between the energy bandgap of n-GaN and InxGa1−xN intrinsic layer can be inserted to the interface of n-GaN and InxGa1-xN layers. From simulation, it indicates that the insertion of graded layer is an effective method to lower energy barrier when there exists a high energy band offset in non-polar nitride devices.

2017 ◽  
Vol 47 (2) ◽  
pp. 1201-1207 ◽  
Author(s):  
Yunfei Chen ◽  
Xuehai Tan ◽  
Shou Peng ◽  
Cao Xin ◽  
Alan E. Delahoy ◽  
...  

2001 ◽  
Vol 89 (12) ◽  
pp. 8327-8330 ◽  
Author(s):  
Takashi Minemoto ◽  
Yasuhiro Hashimoto ◽  
Takuya Satoh ◽  
Takayuki Negami ◽  
Hideyuki Takakura ◽  
...  

CrystEngComm ◽  
2020 ◽  
Vol 22 (26) ◽  
pp. 4416-4426
Author(s):  
Qian Du ◽  
Boyan Li ◽  
Sihan Shi ◽  
Kaizhi Zhang ◽  
Yunxiang Zhang ◽  
...  

Intermediate phases are formed in Zn(O,S) thin films with different oxygen fluxes, affecting the device performance.


2001 ◽  
Vol 67 (1-4) ◽  
pp. 83-88 ◽  
Author(s):  
Takashi Minemoto ◽  
Takuya Matsui ◽  
Hideyuki Takakura ◽  
Yoshihiro Hamakawa ◽  
Takayuki Negami ◽  
...  

2007 ◽  
Vol 1012 ◽  
Author(s):  
Takashi Minemoto ◽  
Yasuhiro Hashimoto ◽  
Takuya Satoh ◽  
Takayuki Negami ◽  
Hideyuki Takakura

AbstractThe impact of the conduction band offset (CBO) between window/Cu(In,Ga)Se2 (CIGS) layers on the light soaking (LS) effect in CIGS solar cells has been studied with continuous CBO control using a (Zn,Mg)O (ZMO) window layer. Two types of CIGS solar cells with different window/buffer/absorber layers configurations were fabricated, i.e., ZMO/CIGS (without buffer layer) and ZMO/CdS/CIGS structures. The CBO values between ZMO and CIGS layers were controlled to -0.15~0.25 eV. Plus and minus signs of CBO indicate the conduction band minimums of ZMO above and below that of CIGS, respectively. Current-voltage (J-V) characteristics of the solar cells with different LS durations revealed that a positive CBO value higher than 0.16 eV induces J-V curve distortion, i.e., LS effect, and all the J-V characteristics stabilized in 30 min. The degrees of the LS effect were dominated by the CBO value between ZMO and CIGS layers in the both structure regardless of the existence of CdS buffer layers. These results indicate that the LS effect is dominated by the highest barrier for photo-generated electrons in the conduction band diagram, i.e., the CBO between ZMO and CIGS layers, and quantitatively the LS effect emerges the CBO value higher than 0.16 eV.


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