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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 />

1

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