Electronic Band Structure ofGaNxPyAs1−x−yHighly Mismatched Alloys: Suitability for Intermediate-Band Solar Cells

2014 ◽  
Vol 1 (3) ◽  
Author(s):  
R. Kudrawiec ◽  
A. V. Luce ◽  
M. Gladysiewicz ◽  
M. Ting ◽  
Y. J. Kuang ◽  
...  
2016 ◽  
Vol 108 (11) ◽  
pp. 112103 ◽  
Author(s):  
Keith T. Butler ◽  
Scott McKechnie ◽  
Pooya Azarhoosh ◽  
Mark van Schilfgaarde ◽  
David O. Scanlon ◽  
...  

Nanoscale ◽  
2021 ◽  
Vol 13 (1) ◽  
pp. 175-184
Author(s):  
Liudmila L. Larina ◽  
Oleksii Omelianovych ◽  
Van-Duong Dao ◽  
Kyunglim Pyo ◽  
Dongil Lee ◽  
...  

XPS study of the electronic structure of the Au22(SG)18 clusters and their interface with TiO2 reveals that tailoring of the electronic band structure at the interface can be exploited to increase the efficiency of metal-cluster-sensitized solar cells.


Optik ◽  
2021 ◽  
Vol 228 ◽  
pp. 165921
Author(s):  
Hyeongsu Choi ◽  
Namgue Lee ◽  
Hyunwoo Park ◽  
Yeonsik Choi ◽  
Hyunwoo Yuk ◽  
...  

2011 ◽  
Vol 106 (2) ◽  
Author(s):  
N. López ◽  
L. A. Reichertz ◽  
K. M. Yu ◽  
K. Campman ◽  
W. Walukiewicz

2010 ◽  
Vol 74 ◽  
pp. 143-150 ◽  
Author(s):  
Antonio Martí ◽  
Antonio Luque

Intermediate band (IB) solar cells aim to exploit in solar cells the energy of below bandgap energy photons. They are based in a material that, in addition to the conventional conduction and valence bands, has an electronic band (named intermediate band) located inside the bandgap and separated from the conduction and valence band by a null density of states. The theoretical limiting efficiency of these cells (63.2 % at maximum concentration) is equivalent to a triple junction solar cell but requiring a single material instead. Several approaches are being followed worldwide to take to practice this concept that can be divided into two categories: quantum dots and bulk materials. This paper reviews the main experimental results obtained under both approaches.


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