Abstract

Recent pronounced global warming has attracted keen interest in solar cells due to their renewable feature exploiting tremendous solar energy (89 PW) during sun’s lifetime of ~5 billion years. Of the solar cells invented so far, inorganic solar cells are now in market but they have a demerit such as high fabrication cost and hard characteristics of inorganic materials which restrict the spreading of solar cells. In this regard organic solar cells have been studied as a contingency because of their potential for cheaper manufacturing cost and variety of applications owing to flexible and semitransparent features. To date, the most widely used polymer as a light-absorbing material is regioregular poly(3-hexylthiophene) (P3HT) which does also act as an electron-donating (i.e., holeaccepting) component in a bulk heterojunction layer inside corresponding solar cell geometry. Here we note that the bulk heterojunction film is, broadly speaking, a mixture of electron-donating and electron-accepting materials, whilst in more specific terms it has integrated and randomly distributed p-n junctions in the bulk polymeric film. As an electron-accepting material, soluble fullerenes such as 1-(3-methoxycarbonyl)-propyl-1-phenyl-(6,6)C61 (PCBM) are widely used. Considering the principle of electron flows in the bulk heterojunction polymer solar cells, it is not necessary to insert a low work function metal in between the bulk heterojunction layer and the electron-collecting electrode, which has been proven in our previous report. However, the direct hole collection from the bulk heterojunction layer to transparent conducting oxide, mostly indium tin-oxide (ITO), was not efficient owing to the insufficient interfacial contact between the bulk heterojunction layer and the ITO surface. Hence most of efficient organic solar cells employ a buffer layer, in most cases poly(3,4-ethylenedioxythiophene): poly (styrenesulfonate) (PEDOT:PSS), between the bulk heterojunction layer and the ITO layer. However, the influence of thickness and thermal annealing conditions of PEDOT:PSS layer was not much studied. In this work, we have briefly investigated the effect of thermal annealing temperature on the performance of polymer solar cells with the PEDOT:PSS nanolayer of which thickness is 20 nm. The result showed that about 40% power conversion efficiency was improved by thermal annealing of the PEDOT:PSS layer at 120 C.

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