dc.description.abstract |
Amorphous silicon thin films based solar cells have a low efficiency comparing to
the conventional poly-crystalline silicon wafer based solar cells. To overcome the
efficiency limitation, the attempt to crystallize the amorphous silicon thin layers
deposited by Plasma enhanced chemical vapor deposition (PECVD) on glass is
investigated. the crystallization process is based on zone-melting technology and
called liquid phase crystallization (LPC). Raman spectroscopy is used to analyze
the properties of the silicon thin layers that is deposited by PECVD process and
crystallized by LPC process; for better understanding of these processes. The
present thesis provides the possibility of engaging Raman spectroscopy as a characterization
method with MATLAB software as the analysis tool to investigate the
properties of thin silicon precursor layers for liquid phase crystallized solar cells.
The exported data after analysis has been plotted into two different categories;
depth profiling as well as two-dimensional mapping. The first category includes
three samples deposited on glass by plasma enhanced chemical vapour deposition
with different deposition parameters (e.g.: silane concentration, rf power, and
pressure) to investigate the influence of these parameters on having amorphous or
micro-crystalline structure, as well as hydrogen content and micro-structure parameters.
The first sample has a µc-Si structure with crystallinity changing with
depth. The other two samples have a-Si structures. All samples have nearly a
constant hydrogen content and micro-structure parameters with depth. Then, the
amorphous samples have been annealed to investigate the influence of annealing
on the structural order and hydrogen diffusion. The first one is thermally unstable,
only 0.50 µm remains on glass after annealing. While the other is stable
and the whole thickness remains unchanged during annealing. All hydrogen has
been diffused in both samples. Raman spectroscopy is a useful technique to create
data that can be plotted as depth profiles for the crystallinity, structural order,
hydrogen content, and micro-structure parameters for PECVD deposited precursors;
hence gives a better understanding of the changes in these properties with
depth. PECVD parameters of the last sample (SiH4 flow rate of 6 sccm, H2 flow
rate of 12 sccm, pressure of 1 mbar, rf power of 25W, and heater temperature of
450 oC) have been taken as the standard, since they deposit an a-Si structure, that
is thermally stable after annealing among all samples. The second section includes
one sample, which has been deposited by electron beam deposition, cut into five
small samples, and then crystallized by liquid phase crystallization with different
crystallization parameters (e.g.: laser scan speed and power) to investigate the
influence of these parameters on stress inside the crystallized precursors. Three
2D maps have been taken in grain boundaries, where c-Si peak is shifting to lower
wavenumbers; hence a tensile stress behavior along grain boundaries is mapped.
Two 2D maps have been taken in the middle of a crack, where the stress behavior
is varied between a tensile stress on one side of the crack and a compressive
stress on the other side. The last 2D maps have been taken at a crack tip, where
the crack starts at the surface but does not continue with depth. higher tensile
stress has been mapped from the glass side, which does not reach its threshold
value to form the crack yet. Raman spectroscopy is a helpful tool in investigate
the stress resulted in LPC-Si precursors for better understanding of LPC process.
LPC parameters of the first sample (red laser beam of 808 nm wavelength, substrate
temperature of 510 oC, laser speed of 1 mm/s, and power of 45W) have been
taken as the standard, since they produce a non-cracked precursor with minimum
number of grain boundaries among all samples. |
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