The performance of quantum dot light-emitting diodes (QD-LEDs) was investigated for different hole transport layers with small molecules and polymers: poly(4-butyl-phenyl-diphenyl-amine), poly-N-vinylcarbazole (PVK), N,N'-diphenyl-N,N'-bis(3-methylphenyl)-1,1'-diphenyl-4,4'-diamine, 4,4',4″-tris(N-carbazolyl)-triphenyl-amine (TCTA), and 4,4'-bis(carbazole-9-yl)biphenyl (CBP). The electroluminescence performance of QD-LEDs was considerably improved by adding small molecules (TCTA or CBP) having high hole mobilily to the polymer hole transport material (PVK). The maximal current efficiency of QD-LED-based PVK was improved by 27% upon addition of 20 wt % TCTA due to the hole injection improvement. The lower turn-on voltage, the higher current density, and the higher luminance were achieved by addition of TCTA. The maximal luminance of 40900 cd/m(2) and the highest current efficiency of 14.0 cd/A with the narrow full width at half-maximum (<35 nm) were achieved by the best hole transport layer.

The recently developed technique of reductive amination, followed by gold labeling, was applied to visualize the reducing ends of cellulose microcrystals from cellulose I, cellulose II, and cellulose III(I). In these crystals, which were also characterized by electron diffraction, the labeling proved that the chains were organized in a parallel fashion in cellulose I from ramie and Valonia and also in cellulose III(I) from Valonia. In microcrystals of cellulose II from mercerized ramie, the labeling method showed that the chains were packed into an antiparallel mode. These results are discussed in terms of the fine structure of cellulose I where neighboring microfibrils of opposite polarity are visualized. The mercerization process whereby cellulose I is converted into cellulose II is therefore best described in terms of an intermingling of the cellulose chains from neighboring microfibrils of opposite polarity. As opposed to the case of mercerization the conversion of cellulose I into cellulose III(I) does not require the participation of neighboring microfibrils since the crystalline domains are converted individually.

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High quality graphene was obtained though microwave irradiated expansion following a solution process. This method is facile, inexpensive, and produces usable results. Ultrathin, uniform graphene films were fabricated at room temperature by a vacuum filtration method. Combining carbon nanotubes (CNTs) as bridges between graphene flakes allowed the fabrication of high-performance conductive films for flexible applications, with conductivities and optical properties comparable to commercial ITO: 181 Omega sq(-1) at 82.2% transmittance after chemical treatment and doping. With future work, this versatile material could well provide an appropriate transparent electrode for flexible optical electronics.

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