Carrier relaxation in epitaxial graphene photoexcited near the Dirac point

We study the carrier dynamics in epitaxially grown graphene in the range of photon energies from 10 to 250 meV. The experiments complemented by microscopic modeling reveal that the carrier relaxation is significantly slowed down as the photon energy is tuned to values below the optical-phonon frequency; however, owing to the presence of hot carriers, optical-phonon emission is still the predominant relaxation process. For photon energies about twice the value of the Fermi energy, a transition from pump-induced transmission to pump-induced absorption occurs due to the interplay of interband and intraband processes.     

Epitaxial graphene: the material for graphene electronics

The search for an ideal graphene sheet has been a quest driving graphene research. While most research has focused on exfoliated graphene, intrinsic substrate interactions and mechanical disorder have precluded the observation of a number of graphene's expected physical properties in this material. The only graphene candidate that has demonstrated all the essential properties of an ideal sheet is multilayer graphene grown on the SiC(000 ) surface. Its unique stacking allows nearly all the sheets in the stack to behave like isolated graphene, while the weak graphene‐graphene interaction prevents any significant doping or distortion in the band near the Fermi level. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)     

Electron Transfer Binding Site of Cytochrome c to Carboxylic Acid-Terminated Alkanethiol Self-assembled Monolayers Immobilized on Gold Electrode

It is proposed that Lys-13 of mammalian cytochrome cfacilitates the most efficient electron transfer (ET) pathway to the carboxylate terminus of alkanethiol self-assembled monolayers (SAM) on gold electrodes. In order to confirm the proposed ET pathway, the ET reaction rate of a rat cytochrome c mutant (RC9K13A), in which lysine-13 is replaced by alanine, is measured at a 3-mercaptopropionate SAM on a gold electrode. The ET rate of K13A is more than six orders of magnitude smaller than that of the native one. In the mutant, Ala-13 can no longer facilitate the ET pathway. Based on the measurements, the potential candidate for the binding site of RC9K13A is Lys-8.     

Why multilayer graphene on 4H-SiC(0001[over ]) behaves like a single sheet of graphene

We show experimentally that multilayer graphene grown on the carbon terminated SiC(0001[over ]) surface contains rotational stacking faults related to the epitaxial condition at the graphene-SiC interface. Via first-principles calculation, we demonstrate that such faults produce an electronic structure indistinguishable from an isolated single graphene sheet in the vicinity of the Dirac point. This explains prior experimental results that showed single-layer electronic properties, even for epitaxial graphene films tens of layers thick.     

Intermolecular biological electron transfer: an electrochemical approach.

We investigated the electron transfer (ET) rates between a well-defined gold electrode and cytochrome c immobilized at the carboxylic acid terminus of alkanethiol self-assembled monolayers (SAMs) by using the potential modulated electroreflectance technique. A logarithmic plot of ET rates against the chain length of the alkanethiol is linear with long chain alkanethiols. The ET rates become independent of the chain length with short alkanethiols. It is proposed that the rate-limiting ET step through short alkyl chains results from a configurational rearrangement process preceding the ET event. This "gating" process arises from a rearrangement of the cytochrome c from a thermodynamically stable binding form on the carboxylic acid terminus to a configuration, which facilitates the most efficient ET pathways (surface diffusion process). We propose that the lysine-13 of mammalian cytochrome c facilitates the most efficient ET pathway to the carboxylate terminus and this proposal is supported by the ET reaction rate of a rat cytochrome c mutant (RC9-K13A) [Elektrokhimiya (2001) in press], in which lysine-13 is replaced by alanine. The ET rate of K13A is more than six orders of magnitude smaller than that of the native protein.     

Amperometric measuring cell for the determination of putrescine oxidase activity

A microfabricated, flat form, amperometric microcell (microchip) is used in a simple, two-electrode arrangement for putrescine oxidase enzyme activity determinations. The cell contains a platinum microdisk working electrode and an Ag/AgCl reference electrode covered by a porous, hydrophilic membrane. An electrochemically-prepared size-exclusion layer is applied on the working electrode surface, to avoid the effect of electroactive interferences in the sample. The hydrophilic membrane, resting on the bottom of the cell, is soaked with a small volume of buffered substrate solution and a few mul enzyme containing sample solution is dispensed over the electrodes. During the enzyme activity measurement a catalytic reaction takes place in the membrane-supported liquid film over the working electrode surface. The hydrogen peroxide produced in the reaction is detected amperometrically. The amperometric current-time curves are used for evaluation. In our work putrescine was used as a substrate to determine the unknown putrescine oxidase enzyme activity of the sample. Elevated diamine oxidase enzyme activity in the vaginal milieu can indicate premature rupture of the amniotic membrane. Results with membrane discs, containing all the necessary chemicals in solid or lyophilized form, are very encouraging with respect of a single use, 'reagentless' biosensor for home care.     

Development of a diamine biosensor

An amperometric diamine sensor is developed for clinical applications in diagnosis of bacterial vaginosis (BV). The sensor is based on crosslinked putrescine oxidase (PUO) which catalyzes the conversion of diamines (mainly putrescine and cadaverine) to products including hydrogen peroxide. The hydrogen peroxide is detected anodically at platinum electrode polarized at 0.5 V versus Ag/AgCl. Platinum-plated gold electrodes used as a substrate for the sensor construction, are batch-fabricated on a flexible polyimide foil (Kapton(R), DuPont). A three-electrode cell configuration is used in all amperometric measurements. The sensor construction is based on three layers: an inner layer to reject the interference effect of oxidizable molecules, an outer diffusion controlling layer, and in addition, an enzyme middle layer. The enzyme layer was immobilized by crosslinking PUO with bovine serum albumin (BSA) using glutaraldehyde (GA). An optimization study of the enzyme solution composition was carried out. With the optimized enzyme layer, the biosensor showed a very high sensitivity and fast response time of ca. 20 s. The sensor has a linear dynamic range from (0.5-300 muM) for putrescine that covers the expected biological levels of the analyte. Details on sensor fabrication and characterization are given in the present work.     

Epitaxial-graphene/graphene-oxide junction: an essential step towards epitaxial graphene electronics

Graphene-oxide (GO) flakes have been deposited to bridge the gap between two epitaxial-graphene electrodes to produce all-graphene devices. Electrical measurements indicate the presence of Schottky barriers at the graphene/graphene-oxide junctions, as a consequence of the band gap in GO. The barrier height is found to be about 0.7 eV, and is reduced after annealing at 180 degrees C, implying that the gap can be tuned by changing the degree of oxidation. A lower limit of the GO mobility was found to be 850 cm2/V s, rivaling silicon. In situ local oxidation of patterned epitaxial graphene has been achieved.