GROWTH OF CNT/A-SI IN PECVD REACTORS FOR SOLAR CELL APPLICATIONS
Technological advances and ever-increasing population growth have resulted in a large demand for energy globally, thereby accelerating threats to human survival. In this era where the increasing need for clean energy is the main focus, solar photovoltaic (PV) or solar cell technology has emerged...
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Format: | Dissertations |
Language: | Indonesia |
Online Access: | https://digilib.itb.ac.id/gdl/view/83418 |
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Institution: | Institut Teknologi Bandung |
Language: | Indonesia |
Summary: | Technological advances and ever-increasing population growth have resulted in a
large demand for energy globally, thereby accelerating threats to human survival.
In this era where the increasing need for clean energy is the main focus, solar
photovoltaic (PV) or solar cell technology has emerged as a promising candidate
to meet these demands and become an alternative environmentally friendly energy
source that is expected to be able to replace conventional petroleum-based energy
sources. and coal. Solar cells mark an important point in the evolution of renewable
energy technology. With the continued development of research and innovation, the
hope of having a cleaner, more efficient and affordable energy source is getting
closer. Along with this, strong support is needed from various parties, including
industry, government and research institutions, to accelerate the adoption and
development of this technology.
Currently, the application of Carbon Nanotubes (CNT) in solar cells is of interest
to photovoltaic researchers, because of its unique characteristics, namely wide
optical absorption, durability, low resistance and high charge carrier mobility.
Apart from that, CNTs have very large electrical conductivity so they are easier to
conduct electric current, therefore they have the potential to increase the efficiency
of thin film solar cells. Quality improvement is also carried out through
development and optimization in experiments.
One of the developments in CNT growth that has been carried out is the growth of
metal catalysts, because they play an important role in the process of forming CNT
tubes. Nickel (Ni) material is used as a metal catalyst which is grown on SiO4 and
Corning glass substrates using the vacuum thermal evaporation method.
Meanwhile, the hot wire cell in plasma-very high frequency-plasma enhanced
chemical vapor deposition (HWC in plasma-VHF-PECVD) technique, which is a
new modification of the development of the PECVD technique, is used to grow CNT
layers and fabricate amorphous silicon (a-Si) based solar cell devices with
optimization. i-layer thickness. The resulting CNT layer was obtained through
optimization of several parameters, then applied in a solar cell device based on pi-n type amorphous silicon, with a Corning glass/TCO/Ni/CNT/a-Si (p-i-n) layer
structure.
Optimization in the growth of the Ni metal catalyst was obtained at a deposition
time parameter of 50 s, with an annealing suhue of 500 ?C for 4.5 hours which
produced a metal catalyst measuring 26.18 nm, with a standard deviation and
polydispersity of 6.005 nm and 22.94 % respectively. Furthermore, the resulting Ni
metal catalyst becomes a medium for the deposition of CNTs grown on a Corning
glass+TCO substrate using the HWC in plasma-VHF-PECVD technique with
optimization of deposition parameters including of CH4 precursor gas flow rate,
deposition time, substrate suhue, and chamber pressure. From this optimization,
CNT obtained with optimum results at a CH4 gas precursor flow rate of 80 sccm
that deposited for 1 hour with a substrate suhue of 250 ?C and chamber pressure
of 500 mTorr. Through this optimization, semiconducting CNTs were obtained with
a diameter and length of ~29 nm and a length of ~2206 nm respectively, an ID/IG
ratio of 0.87 with an energy band gap of 2.31 eV. The overall results obtained show
that the energy band gap of the CNTs produced in this research includes a "wide
band gap" so that CNTs can be well applied as a front layer in a-Si based p-i-n
solar cell devices.
The resulting CNT layer is then applied in amorphous silicon-based solar cells,
which is one of the development options in this research by looking at the effect of
the CNT layer on a-Si based p-i-n solar cell devices on optimizing the i-layer
thickness. From the results of this application, the largest efficiency value of
0,061% was obtained at a i-layer thickness of 1.8 ?m.
This research is the first research carried out at the PECVD KK FTMM ITB
Laboratory, namely by applying a CNT layer to an a-Si based p-i-n solar cell device
using the HWC in plasma-VHF-PECVD method. The process of deposition of the
CNT layer on the a-Si solar cell device is carried out in-situ so that this research is
more practical and economical. The results of this research can be an initial study
in efforts that expected to provide new contributions in the development of solar
cells, especially the application of CNT thin layers on a-Si solar cell devices.
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