Electron field emission is a quantum tunneling phenomenon whereby electrons are emitted from a solid surface due to a strong electric field. Graphene and its derivatives are expected to be efficient field emitters due to their unique geometry and electrical properties. So far, electron field emission has only been achieved from the edges of graphene and graphene oxide sheets. We have supported graphene oxide sheets on nickel nanotip arrays to produce a high density of sharp protrusions within the sheets and then applied electric fields perpendicular to the sheets. Highly efficient and stable field emission with low turn-on fields was observed for these graphene oxide sheets, because the protrusions appear to locally enhance the electric field and dramatically increase field emission. Our simple and robust approach provides prospects for the development of practical electron sources and advanced devices based on graphene and graphene oxide field emitters.

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A composite surface was prepared on cyclic olefin copolymer (COC) microchannels by UV-photografting of polyethylene glycol acrylate (PEGA) and poly(acrylic acid) (PAA) films. A PEGA layer of globular particles with average thickness of 60 nm was formed after 15 min of polymerization. Real time monitoring by pulsed streaming potentials demonstrated the ability of the PEGA layer to inhibit the adhesion of five different nonspecific adsorbing proteins when compared with pristine COC. Roughness determined by atomic force microscopy (AFM) after PAA grafting on COC-PEGA at different UV illumination times suggests that PAA formation is initiated at the free space in between the PEGA particles. Carboxylic groups activated with N-hydroxysuccinimide and N-ethyl-N'-(3-dimethylaminopropyl) carbodiimide were used to bind anti-lysozyme polyclonal antibodies. The composite COC-PEGA-PAA-anti-lysozyme surface demonstrated its ability to detect lysozyme with a dynamic range between 140 and 860 nM. Linearity was maintained even when samples were spiked with 250 nM of cytochrome as interfering species. The equilibrium constant K(eq) for the adsorption of Ly on COC-PEGA-PAA-anti-Ly was estimated to be 2.7 × 10(6) M(-1), and it shows that this kinetic approach of monitoring the surface charge is also useful to estimate affinity interactions for proteins in label free fashion. The regeneration of the surface exhibited an average percentage of recovery of ∼97% for each of six adsorption-regeneration cycles. This feature enables curve calibration on a single microfluidic chip because each point of the curve has a reproducible and renewable surface.

The effects of polarity and surface treatment on the morphological, electrical, and optical behaviors in bulk GaN have been investigated. Kelvin probe, atomic force microscopy (AFM), and photoluminescence (PL) techniques were utilized to examine a set of freestanding, bulk GaN samples, which were grown by halide vapor phase epitaxy. The Ga- and N-polar surfaces were treated with either a mechanical polish (MP) or chemical mechanical polish (CMP), which influences the morphology, surface photovoltage (SPV), and PL behaviors. Topography studies indicate that the CMP-treated, Ga-polar surface is the smoothest of the sample set, whereas the MP-treated, N-polar surface has the highest root mean square roughness. Local current–voltage spectra obtained with conducting AFM reveal a higher forward-bias, turn-on voltage for the N-polar versus Ga-polar surfaces. Using a Kelvin probe, intensity-dependent SPV measurements are performed on samples with CMP-treated, Ga- and N-polar surfaces, and provide band bending values of 0.83 and 0.70 eV, respectively. The restoration of the SPV from CMP-treated surfaces behaves as predicted by a thermionic model, whereas restoration from MP-treated surfaces has a faster rate than expected. This result is possibly due to enhanced electron conduction via hopping between defect states to the surface. The quantum efficiency of the PL from the CMP- and MP-treated surfaces at room temperature is ∼1% and 1 × 10−5%, respectively, suggesting high quenching of the PL for MP-treated surfaces by near-surface defects. Therefore, AFM, PL, and SPV data indicate that the MP-treated surfaces have a significantly higher density of surface defects.