Published: October 17, 2011 r2011 American Chemical Society 8470 dx.doi.org/10.1021/ma201911a | Macromolecules 2011, 44, 84708478 ARTICLE pubs.acs.org/Macromolecules Thermal Stability of Poly[2-methoxy-5-(2 0 -phenylethoxy)-1,4- phenylenevinylene] (MPE-PPV):Fullerene Bulk Heterojunction Solar Cells J. Vandenbergh, B. Conings, S. Bertho, J. Kesters, D. Spoltore, S. Esiner, J. Zhao, § G. Van Assche, § M. M. Wienk, W. Maes, ,|| L. Lutsen, ^ B. Van Mele, § R. A. J. Janssen, J. Manca, ,^ and D. J. M. Vanderzande* ,,^ Institute for Materials Research (IMO), Hasselt University, Universitaire Campus, Building D, B-3590 Diepenbeek, Belgium Molecular Materials and Nanosystems, Eindhoven University of Technology, P.O. Box 513, 5600MB Eindhoven, The Netherlands § Physical Chemistry and Polymer Science, Department of Materials and Chemistry, Vrije Universiteit Brussel, Pleinlaan 2, B-1050 Brussels, Belgium ) Molecular Design and Synthesis, Katholieke Universiteit Leuven, Celestijnenlaan 200F, B-3001 Heverlee, Belgium ^ Division IMOMEC, IMEC, Universitaire Campus, Wetenschapspark 1, B-3590 Diepenbeek, Belgium b S Supporting Information INTRODUCTION In polymer:fullerene bulk heterojunction solar cells, the nanoscale morphology of the active layer inuences the electronic properties of the devices to a great extent. 14 Via proper sample preparation, such as annealing conditions and the choice of proces- sing solvents, the (nano)morphology of the donoracceptor blend can be optimized, leading to improved exciton dissociation and charge transport. 36 It was already demonstrated, however, that this initial optimized morphology deteriorates rather fast (during storage at elevated temperatures). 717 Long-term annealing treatments induce severe phase separation between the donor polymer and the fullerene acceptor material, leading to a decreased interfacial area and less ecient exciton dissociation. 1820 To stabilize the initial (nano)morphology of a bulk heterojunction layer, several pathways can be followed. A rst approach is to use donoracceptor diblock copolymers to covalently xate the morphology via the scale of the block lengths. 13,14 A second way to obtain a stable network is to build in a certain amount of functional groups in the donor polymer which can cross-link and freeze in the ultimate morphology after a thermal or UV light treatment. 21 In this paper, a third approach is further investigated, which is based on the use of a donor polymer with a high glass transition temperature (T g ). 2226 In this context the question arises how to adjust the chemical structure of the polymer to induce a higher T g , without jeopardizing the opto- electronic characteristics of the polymer. Here we demonstrate that by changing the side-chain substituents of the polymer, the T g can be deliberately increased. Poly[(2-methoxy-5-(3 0 ,7 0 -dimethyl- octyloxy))-1,4-phenylenevinylene] (MDMO-PPV) has a quite low T g of around 45 °C due to the long exible alkoxy side chains, which cause a plasticizing eect on the PPV backbone. 22 To reduce the side-chain exibility, a novel poly(p-phenylenevinylene) derivative, poly[2-methoxy-5-(2 0 -phenylethoxy)-1,4-phenylenevinylene] Received: August 22, 2011 Revised: October 2, 2011 ABSTRACT: To improve the thermal stability of polymer:fullerene bulk hetero- junction solar cells, a new polymer, poly[2-methoxy-5-(2 0 -phenylethoxy)-1,4- phenylenevinylene] (MPE-PPV), has been designed and synthesized, which showed an increased glass transition temperature (T g ) of 111 °C. The thermal character- istics and phase behavior of MPE-PPV:[6,6]-phenyl C 61 -butyric acid methyl ester ([60]PCBM) blends were investigated by means of modulated temperature dier- ential scanning calorimetry and rapid heatingcooling calorimetry. The thermal stability of MPE-PPV:[60]PCBM solar cells was compared with devices based on the reference MDMO-PPV material with a T g of 45 °C. Monitoring of the photo- currentvoltage characteristics at elevated temperatures revealed that the use of high- T g MPE-PPV resulted in a substantial improvement of the thermal stability of the solar cells. Furthermore, a systematic transmission electron microscope study of the active polymer:fullerene layer at elevated temperatures likewise demonstrated a more stable morphology for the MPE-PPV:[60]PCBM blend. Both observations indicate that the use of high-T g MPE-PPV as donor material leads to a reduced free movement of the fullerene molecules within the active layer of the photovoltaic device. Finally, optimization of the PPV:fullerene solar cells revealed that for both types of devices the use of [6,6]-phenyl C 71 -butyric acid methyl ester ([70]PCBM) resulted in a substantial increase of current density and power conversion eciency, up to 3.0% for MDMO-PPV:[70]PCBM and 2.3% for MPE- PPV:[70]PCBM.