Films minces à base de Si nanostructuré pour des cellules ...
Films minces à base de Si nanostructuré pour des cellules ...
Films minces à base de Si nanostructuré pour des cellules ...
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Introduction<br />
State of the art<br />
tel-00916300, version 1 - 10 Dec 2013<br />
In the quest for new renewable sources of energy, the focus of research today is on<br />
cost-eective photovoltaic technologies with higher levels of eciency. The second<br />
generation thin lm solar cells were promising compared to the rst generation<br />
of bulk solar cells in reducing the manufacturing costs. But, the eciencies are<br />
lower since the thin lms in general cannot absorb eciently the solar spectrum<br />
without light trapping mechanisms. The combination of the third generation solar<br />
cell concepts and the second generation thin lm materials has been i<strong>de</strong>ntied as<br />
a solution to economically meet the global energy needs. The major targets of the<br />
third generation photovoltaics (PV) are:<br />
ˆ to reduce the cost from 1$/watt of second generation PV to 0.50-0.20 $/watt<br />
by increasing the eciency and lowering the material need.<br />
ˆ to overcome the power loss mechanisms in single bandgap solar cells using<br />
approaches that eectively absorb photons below and above the bandgap of<br />
the solar cell material.<br />
Tan<strong>de</strong>m cell is one of the third generation concepts that enables to absorb a wi<strong>de</strong><br />
range of solar spectrum by stacking individual cells with dierent bandgaps. The<br />
wi<strong>de</strong> availability of the non-toxic <strong>Si</strong>, and its compatibility with the already existing<br />
technologies make All-<strong>Si</strong> tan<strong>de</strong>m cell an attractive approach. <strong>Si</strong>licon, being an<br />
indirect semiconductor is not an i<strong>de</strong>al material in reducing the cost of solar cells<br />
because it requires about 125 micron thickness to absorb 90% of solar radiation,<br />
while in a direct bandgap material such as GaAs about 1 micron is sucient. The<br />
discovery of quantum connement eect in <strong>Si</strong> nanostructures resolves this problem<br />
arising from conventional c-<strong>Si</strong> solar cells, and therefore can be eciently incorporated<br />
in a tan<strong>de</strong>m cell. The bandgap engineering is achieved by stacking quantum wells<br />
(QW) or quantum dots (QD) of <strong>Si</strong> with dielectric barriers which are also <strong>base</strong>d on<br />
<strong>Si</strong>-compounds such as <strong>Si</strong>O 2 , <strong>Si</strong> 3 N 4 or <strong>Si</strong>C. With increasing QD <strong>de</strong>nsity, the eective<br />
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