The relative permittivity of the materials constituting heterojunction solar cells is usually not considered as a design parameter when searching for novel combinations of heterojunction materials. In this work, we investigate whether such an approach is valid. Specifically, we show the effect of the materials permittivity on the physics and performance of the solar cell by means of numerical simulation supported by analytical relations. We demonstrate that, depending on the specific solar cell configuration and materials properties, there are scenarios where the relative permittivity has a major influence on the achievable conversion efficiency, and scenarios where its influence can be safely ignored. In particular, we argue that high-permittivity materials should always be the preferred choice as heterojunction partners of the absorber layer when prototyping new materials combinations. When the heterojunction partner has a high permittivity, solar cells are consistently more robust against several non-idealities that are especially likely to occur in early-stage development, when the device is not yet optimized.
We report on the microstructure, morphology, and growth of 5,5´-bis(naphth-2yl)-2,2´-bithiophene (NaT2) thin films deposited on graphene, characterized by grazingincidence X-ray diffraction (GIXRD) and complemented by atomic force microscopy (AFM) measurements. NaT2 is deposited on two types of graphene surfaces: custom-made samples where CVD-grown graphene layers are transferred onto a Si/SiO 2 substrate by us and common commercially transferred CVD graphene on Si/SiO 2 . Pristine Si/SiO 2 substrates are used as a reference. The NaT2 crystal structure and orientation depend strongly on the underlying surface, with the molecules predominantly lying-down on the graphene surface (face-on orientation) and standing nearly out-of-plane (edge-on orientation) on the Si/SiO 2 reference surface. Post growth GIXRD and AFM measurements reveal that the crystalline structure and grain morphology differ depending on whether there is polymer residue left on the graphene surface. In situ GIXRD measurements show that the thickness dependence of the intensity of the (111) reflection from the crystalline edge-on phase does not intersect zero at the beginning of the deposition process, suggesting that an initial wetting layer, corresponding to 1-2 molecular layers, is formed at the surface-film interface. By contrast, the (111) reflection intensity from the crystalline face-on phase grows at a constant rate as a function of film thickness during the entire deposition.
M. (2018). Structural basis for a naphthyl end-capped oligothiophene with embedded metallic nanoparticles for organic field-effect transistors. Applied Physics Letters, 113(25), [251903]. https://doi.
The structure of two naphthylene-capped oligothiophene, 5,5 -bis(naphth-2-yl)-2,2bi-and tri-thiophene, thin-film field-effect transistor assemblies has been studied using modeling in conjunction with grazing incidence x-ray diffraction. Although the well known herringbone molecular packing motif is observed in these films for both compounds, density functional calculations and molecular mechanics modeling give evidence for a local polymorphic ordering in which these molecules can be flipped 180 • about the long axis. In one case, that of the oligothiophene trimer, a disordered surface induced phase is observed. Prospective structural models are tested and refined using 1
Organic semiconductors have seen widespread application in thin‐film devices, such as organic field‐effect transistors (OFETs), whose performance is closely linked to the molecular‐level microstructure and crystalline orientation. In actual OFETs, the microstructure varies significantly based on the local environment, for example, in the proximity of contact electrodes. This account highlights recent examples where microfocused grazing‐incidence wide‐angle X‐ray scattering (μGIWAXS) maps structural information in between the OFET electrodes. Also shown are results where μGIWAXS is used to study the microstructure of naphthyl end‐capped oligothiophenes across interdigitated electrode arrays in a bottom‐contact OFET identifying lateral proximity effects of the contact electrodes in terms of crystalline misorientation, crystallite size, and disorder. The results together with those highlighted, classify essential structural parameters on and in between the electrodes and demonstrate capabilities of microfocused X‐rays to map microstructures in actual devices. The ideas presented herein bring us toward guidelines for understanding electrode proximity and device performance in molecular semiconductors. It is also believed that they are readily expanded from OFETs to other devices and from small molecules to polymers and other materials.
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