ELECTRONIC STRUCTURE, TRANSPORT, AND OPTICAL PROPERTIES OF CSPBX3 (X = CL, BR, I) COMPOUNDS
Global warming causes more and more parties to realize the need to reduce the energy dependence on the fossil-based resources. Solar cell is one of the electrical energy producing devices with a lot of advantages such as envirommentally friendly and unlimited resources. Solar cells have signif...
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Format: | Final Project |
Language: | Indonesia |
Subjects: | |
Online Access: | https://digilib.itb.ac.id/gdl/view/64819 |
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Institution: | Institut Teknologi Bandung |
Language: | Indonesia |
Summary: | Global warming causes more and more parties to realize the need to reduce the energy
dependence on the fossil-based resources. Solar cell is one of the electrical energy producing
devices with a lot of advantages such as envirommentally friendly and unlimited resources.
Solar cells have significantly developed, with Dye-Sensitized Solar Cell (DSSC) is the latest
generation of solar cell. DSSC can use CH3NH3PbI3 as materials to absorb lights (dyes) with
high energy conversion. However, this material has many disadvantages, one of them is that
this material is unstable at high temperature and under UV lights. Therefore, it is necessary
to develop alternative materials that have the same advantages as CH3NH3PbI3, namely
CsPbX3 (X = Cl, Br, I). Computational studies have been carried out on CsPbX3 (X = Cl, Br,
I), but no one has reported the relativistic effect as spin-orbit coupling in computational
calculations. On the other side, to study complex materials, it needs a faster and accurate
calculations. One of the methods to speed up the calculations is by using Graphical
Processing Unit (GPU). In this research, computational calculations have been carried out to
determine physical properties of CsPbX3 (X = Cl, Br, I) such as band structures, transport
properties, and optical properties. Band gap width (Eg) for CsPbX3 (X = Cl, Br, I) decrease
as spin-orbit coupling present, with Eg CsPbCl3 non-SOC = 1.8114 eV; Eg CsPbCl3 SOC =
0.6827 eV; Eg CsPbBr3 non-SOC = 2.0934 eV; Eg CsPbBr3 SOC = 0.9807 eV; Eg CsPbI3
non-SOC = 2.4741 eV; and Eg CsPbI3 SOC = 1.9211 eV. For transport properties, at 600 K
and ? = 0.5 eV, electrical conductivity of CsPbCl3, CsPbBr3, and CsPbI3 are 1.25×1018
(?.m.s)-1, 1.25×1012 (?.m.s)-1, and 1.51×1017 (?.m.s)-1, respectively. Optical properties
shows that all the first absorption peak of CsPbCl3 and CsPbBr3 are close to the band gap
energy values for each material. Calculation using CPU and GPU shows that there is no
difference in calculations in terms of accuracy and calculation with GPU is 2 times faster
than using CPU only. |
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