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 ...
Figure 1.1: World energy consumption-2007 Statistics [Internet 03]. tel-00916300, version 1 - 10 Dec 2013 ductors to convert light into electric energy. Solar PV can be eectively used to power isolated homes in remote places. The sustainability and availability of the solar energy serves as a motivation to achieve cost-eective PV devices with high eciency, by developing novel materials. 1.2 Solar Photovoltaics 1.2.1 A brief history of PV cells The solar photovoltaic approach generates power using solar panels, which are made up of a large number of solar cells. It works on the principle discovered by Edmond Becquerel in 1839 known as the photovoltaic eect, which is the production of current in a material on illumination. A century later, Russel Ohl discovered the presence of a p-n junction in Silicon, by observing that one area of the material offered more resistance to current ow than the other, when heated or illuminated. He reasoned this junction formation to be a contribution from segregation of impurity in recrystallized silicon (Si) melts during the growth of monocrystalline Si rods. This discovery of p-n junction resulted in the rst PV devices in 1941 [Ohl 41a, Ohl 41b]. In 1952, conversion eciency of about 1% was achieved by controlling the location of junction formation, which was a major problem in the earlier devices [Kingsbury 52]. In 1954, the rst modern solar cell developed at the Bell laboratories using the silicon p-n junction, increased the eciency to 6% which is the rst milestone in the PV research industry [Chapin 54]. The wide usage of PV cells for space applications resulted in modications of the device structures by placing contact grids on the top surface and this resulted in a further increase of eciency to 14% [Mandelkorn 62]. Eversince, a lot of materials have been investigated for PV applications and presently 6
mono-, poly- and amorphous silicon, cadmium telluride, and copper indium gallium selenide/sulde (CIGS) have become the most used materials. 1.2.2 Three Generations of PV cells The major challenges faced by the PV industry are the high costs of production for a relatively low eciency 1 . To overcome this challenge, PV cells are categorized into three generations on their genealogical basis, and all three are being currently investigated towards protable development. Figure 1.2 shows a consolidated representation of the conversion eciencies and cost of the three generations of PV cells. tel-00916300, version 1 - 10 Dec 2013 Figure 1.2: Consolidated representation of conversion eciencies and cost of the three generations of PV cells [Conibeer 07]. The rst generation PV cells are largely based on mono- or polycrystalline Si and has the major share of over 85% commercial production. Laboratory eciencies of 23-24.7% [Green 93, Green 01a] and commercial module eciencies lying between 14-19% [Parida 11] have been reported from these cells. The main drawback of rst generation cells arises from the indirect bandgap nature of Si which necessitates a thick active layer which is at least 50 µm thick for ecient absorption [Chopra 04]. In general, about 300-500 µm thick layer is used for a solar cell, which accounts to about 28% of the module cost. The sophisticated procedures for high temperature processing to obtain highly puried electronic grade silicon for a device, combined with the need for large material area has made these solar cells expensive with about US$ 3.50/W. The second generation PV cells aim at reducing the production costs by 1 Eciency = Maximum electrical power/ Incident optical power 7
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mono-, poly- and amorphous silicon, cadmium telluri<strong>de</strong>, and copper indium gallium<br />
seleni<strong>de</strong>/sul<strong>de</strong> (CIGS) have become the most used materials.<br />
1.2.2 Three Generations of PV cells<br />
The major challenges faced by the PV industry are the high costs of production<br />
for a relatively low eciency 1 . To overcome this challenge, PV cells are categorized<br />
into three generations on their genealogical basis, and all three are being currently<br />
investigated towards protable <strong>de</strong>velopment. Figure 1.2 shows a consolidated representation<br />
of the conversion eciencies and cost of the three generations of PV<br />
cells.<br />
tel-00916300, version 1 - 10 Dec 2013<br />
Figure 1.2: Consolidated representation of conversion eciencies and cost of the three<br />
generations of PV cells [Conibeer 07].<br />
The rst generation PV cells are largely <strong>base</strong>d on mono- or polycrystalline <strong>Si</strong><br />
and has the major share of over 85% commercial production. Laboratory eciencies<br />
of 23-24.7% [Green 93, Green 01a] and commercial module eciencies lying between<br />
14-19% [Parida 11] have been reported from these cells. The main drawback of rst<br />
generation cells arises from the indirect bandgap nature of <strong>Si</strong> which necessitates a<br />
thick active layer which is at least 50 µm thick for ecient absorption [Chopra 04].<br />
In general, about 300-500 µm thick layer is used for a solar cell, which accounts to<br />
about 28% of the module cost. The sophisticated procedures for high temperature<br />
processing to obtain highly puried electronic gra<strong>de</strong> silicon for a <strong>de</strong>vice, combined<br />
with the need for large material area has ma<strong>de</strong> these solar cells expensive with about<br />
US$ 3.50/W.<br />
The second generation PV cells aim at reducing the production costs by<br />
1 Eciency = Maximum electrical power/ Inci<strong>de</strong>nt optical power<br />
7