We will treat this seconds the multi-junction solar cells that combine several materials deposited in thin films by PCV. Here we present a theoretical curve on the left that gives a conversion efficiency when combining two materials with different band gaps. If the wide band gap material is amorphous silicon 1.8 eV, the so-called material with narrower band gap will extend the congestion is inside them. The optimum, therefore, correspond to a gap of 1.2 eV associated with hydrogenated amorphous silicon. This correspond to silicon germanium alloys or nano-crystalline silicon. We then obtain a tandem cell which is displayed here. The tandem cells may have several electrical terminals, because one can introduce an intermediate transparent electrode layer between the two cells. This is not possible for crystalline cells because of the requirements of epitaxy. The thin film's multi-junction display more flexibility. We can make cells with three or four terminals and make the two cells independent in the later case, and avoid the current conservation issues. I present in this animation the principles of preparation of a thin film cells. Firstly, amorphous silicon. So we see the various layers which are deposited on the glass substrate, and below, the example of cells which are made in the laboratory. In the case of a tandem structure, it's first deposited the wider band gap materials, the amorphous silicon and glass, which will be exposed to the photon flux, and then, a secure layer of nano or micro crystalline silicon. Such micro morph cell is thus obtained which combines the optical properties of the two materials. Amorphous silicon absorbs visible photons, [inaudible] ,and the micro-crystalline silicon extend the absorption in the near infrared. Here, we schematically show, in this animation, the light trapping in such cells. Texturing of the cell induces light-scattering, thereby, increasing its optical lengths. In the case of the tandem cell, reflections at the interfaces allow further increases in the optical path. To optimize the cell optically, a tissue layer, intermediate refractive index is deposited on the metal electrode, and that reflection layer with a refractive index lower than your glass, less than 1.5, can be added onto glass substrate to reduce reflection of the glass which is of the order of five percent. At the level of performance of the multi-junction cells, it is here that one can reach the order of 12 percent in conversion efficiency on large area, 30 by 30 centimeter square. With a doubling of the short-circuit current with respect to amorphous silicon. Furthermore, we find that these cells are less sensitive to instability phenomena, top figure. This is due to a thick layer of partially crystalline silicon in the cell. Another way to prepare multi-junction cells is to use silicon germanium alloys. We will present here an example of a triple-junction cell with two silicon germanium compositions. This gives a stable efficiency of around 13 percent on small area. However, unlike partially crystallized silicon, germanium silicon is sensitive to instability phenomenon. It is possible to exceed 13 percent with thin film multi-junction as can be seen on this simulation published in 2014. By combining four materials based on silicon and germanium, amorphous or nano-crystalline, one can obtain a theoretical efficiency of close to 20 percent not stabilized. Experimentally, one can get more than 16 percent in the laboratory conditions. The complexity of preparing such structures in continuous on flexible substrate, the so-called wall to wall, can be great because it needs at least a plasma reactor by layer. It's therefore necessary to increase the number of plasma reactor, thus increasing the cost. We presented the different types of solar thin-film cells, mono or multi-junction. We will focus now on photovoltaic modules made from these cells. Thank you.