Kalyan Raidongia

Graphene Analogues of BN: Novel Synthesis and Properties

Enthused by the fascinating properties of graphene, we have prepared graphene analogues of BN by a chemical method with a control on the number of layers. The method involves the reaction of boric acid with urea, wherein the relative proportions of the two have been varied over a wide range. Synthesis with a high proportion of urea yields a product with a majority of 1-4 layers. The surface area of BN increases progressively with the decreasing number of layers, and the high surface area BN exhibits high CO(2) adsorption, but negligible H(2) adsorption. Few-layer BN has been solubilized by interaction with Lewis bases. We have used first-principles simulations to determine structure, phonon dispersion, and elastic properties of BN with planar honeycomb lattice-based n-layer forms. We find that the mechanical stability of BN with respect to out-of-plane deformation is quite different from that of graphene, as evident in the dispersion of their flexural modes. BN is softer than graphene and exhibits signatures of long-range ionic interactions in its optical phonons. Finally, structures with different stacking sequences of BN have comparable energies, suggesting relative abundance of slip faults, stacking faults, and structural inhomogeneities in multilayer BN.

On the origin of the stability of graphene oxide membranes in water

Graphene oxide (GO) films are known to be highly stable in water and this property has made their use in membrane applications in solution possible. However, this state of affairs is somewhat counterintuitive because GO sheets become negatively charged on hydration and the membrane should disintegrate owing to electrostatic repulsion. We have now discovered a long-overlooked reason behind this apparent contradiction. Our findings show that neat GO membranes do, indeed, readily disintegrate in water, but the films become stable if they are crosslinked by multivalent cationic metal contaminants. Such metal contaminants can be introduced unintentionally during the synthesis and processing of GO, most notably on filtration with anodized aluminium oxide filter discs that corrode to release significant amounts of aluminium ions. This finding has wide implications in interpreting the processing-structure-property relationships of GO and other lamellar membranes. We also discuss strategies to avoid and mitigate metal contamination and demonstrate that this effect can be exploited to synthesize new membrane materials.

BCN: A Graphene Analogue with Remarkable Adsorptive Properties

A new analogue of graphene containing boron, carbon and nitrogen (BCN) has been obtained by the reaction of high-surface-area activated charcoal with a mixture of boric acid and urea at 900 degrees C. X-ray photoelectron spectroscopy and electron energy-loss spectroscopy reveal the composition to be close to BCN. The X-ray diffraction pattern, high-resolution electron microscopy images and Raman spectrum indicate the presence of graphite-type layers with low sheet-to-sheet registry. Atomic force microscopy reveals the sample to consist of two to three layers of BCN, as in a few-layer graphene. BCN exhibits more electrical resistivity than graphene, but weaker magnetic features. BCN exhibits a surface area of 2911 m(2) g(-1), which is the highest value known for a B(x)C(y)N(z) composition. It exhibits high propensity for adsorbing CO(2) ( approximately 100 wt %) at 195 K and a hydrogen uptake of 2.6 wt % at 77 K. A first-principles pseudopotential-based DFT study shows the stable structure to consist of BN(3) and NB(3) motifs. The calculations also suggest the strongest CO(2) adsorption to occur with a binding energy of 3.7 kJ mol(-1) compared with 2.0 kJ mol(-1) on graphene.

Nanofluidic Ion Transport through Reconstructed Layered Materials

Electrolytes confined in nanochannels with characteristic dimensions comparable to the Debye length show transport behaviors deviating from their bulk counterparts. Fabrication of nanofluidic devices typically relies on expensive lithography techniques or the use of sacrificial templates with sophisticated growth and processing steps. Here we demonstrate an alternative approach where unprecedentedly massive arrays of nanochannels are readily formed by restacking exfoliated sheets of layered materials, such as graphene oxide (GO). Nanochannels between GO sheets are successfully constructed as manifested by surface-charge-governed ion transport for electrolyte concentrations up to 50 mM. Nanofluidic devices based on reconstructed layer materials have distinct advantages such as low cost, facile fabrication, ease of scaling up to support high ionic currents, and flexibility. Given the rich chemical, physical, and mechanical properties of layered materials, they should offer many exciting new opportunities for studying and even manufacturing nanofluidic devices.

Multiferroic and magnetoelectric properties of core-shell CoFe2O4@BaTiO3 nanocomposites

Core-shell CoFe2O4@BaTiO3 nanoparticles and nanotubes have been prepared using a combination of solution processing and high temperature calcination. Both the core-shell nanostructures exhibit magnetic and dielectric hysteresis at room temperature and magnetoelectric effect. The dielectric constant of both the nanocomposites decreases upon application of magnetic field. The core-shell nanoparticles exhibit 1.7% change in magnetocapacitance around 134 K at 1 T, while the core-shell nanotubes show a remarkable 4.5% change in magnetocapacitance around 310 K at 2 T.

Graphene oxide assisted hydrothermal carbonization of carbon hydrates.

Hydrothermal carbonization (HTC) of biomass such as glucose and cellulose typically produces micrometer-sized carbon spheres that are insulating. Adding a very small amount of Graphene oxide (GO) to glucose (e.g., 1:800 weight ratio) can significantly alter the morphology of its HTC product, resulting in more conductive carbon materials with higher degree of carbonization. At low mass loading level of GO, HTC treatment results in dispersed carbon platelets of tens of nanometers in thickness, while at high mass loading levels, free-standing carbon monoliths are obtained. Control experiments with other carbon materials such as graphite, carbon nanotubes, carbon black, and reduced GO show that only GO has significant effect in promoting HTC conversion, likely due to its good water processability, amphiphilicity, and two-dimensional structure that may help to template the initially carbonized materials. GO offers an additional advantage in that its graphene product can act as an in situ heating element to enable further carbonization of the HTC products very rapidly upon microwave irradiation. Similar effect of GO is also observed for the HTC treatment of cellulose.

Synthesis, structure and properties of homogeneous BC4N nanotubes

BCN nanotube brushes have been obtained by the high temperature reaction of amorphous carbon nanotube (a-CNT) brushes with a mixture of boric acid and urea. The a-CNT brushes themselves were obtained by the pyrolysis of glucose in a polycarbonate membrane. The BCN nanotubes have been characterized by EELS, XPS, electron microscopy, Raman spectroscopy and other techniques. The composition of these nanotubes is found to be BC4N. The nanotubes, which are stable up to 900 °C, are insulating and nonmagnetic. They exhibit a selective uptake of CO2 up to 23.5 wt%. In order to understand the structure and properties, we have carried out first-principles density functional theory based calculations on (6,0), (6,6) and (8,0) nanotubes with the composition BC4N. While (8,0) BC4N nanotubes exhibit a semiconducting gap, the (6,0) BC4N nanotube remains metallic if ordered BN bonds are present in all the six-membered rings. The (6,6) BC4N nanotubes, however, exhibit a small semiconducting gap unlike the carbon nanotubes. The most stable structure is predicted to be the one where BN3 and NB3 units connected by a B–N bond are present in the graphite matrix, the structure with ordered B–N bonds in the six-membered rings of graphite being less stable. In the former structure, (6,0) nanotubes also exhibit a gap. The calculations predict BC4N nanotubes to be overall nonmagnetic, as is indeed observed.

Self-assembled two-dimensional nanofluidic proton channels with high thermal stability

Exfoliated two-dimensional (2D) sheets can readily stack to form flexible, free-standing films with lamellar microstructure. The interlayer spaces in such lamellar films form a percolated network of molecularly sized, 2D nanochannels that could be used to regulate molecular transport. Here we report self-assembled clay-based 2D nanofluidic channels with surface charge-governed proton conductivity. Proton conductivity of these 2D channels exceeds that of acid solution for concentrations up to 0.1 M, and remains stable as the reservoir concentration is varied by orders of magnitude. Proton transport occurs through a Grotthuss mechanism, with activation energy and mobility of 0.19 eV and 1.2 × 10(-3) cm(2) V(-1) s(-1), respectively. Vermiculite nanochannels exhibit extraordinary thermal stability, maintaining their proton conduction functions even after annealing at 500 °C in air. The ease of constructing massive arrays of stable 2D nanochannels without lithography should prove useful to the study of confined ionic transport, and will enable new ionic device designs.

Remarkable uptake of CO2 and CH4 by graphene-Like borocarbonitrides, BxCyNz.

The surface areas and uptake of CO(2) and CH(4) by four graphene samples are measured and compared with activated charcoal. The surface areas are in the range of 5-640 m(2) g(-1), whereas the CO(2) and CH(4) uptake values are in the range of 18-45 wt % (at 195 K, 0.1 MPa) and 0-2.8 wt % (at 273 K, 5 MPa), respectively. The CO(2) and CH(4) uptake values of the graphene samples vary linearly with the surface area. In contrast, graphene-like B(x)C(y)N(z) samples with compositions close to BC(2)N exhibit surface areas in the range of 1500-1990 m(2) g(-1) and CO(2) and CH(4) uptake values in the ranges 97-128 wt % (at 195 K, 0.1 MPa) and 7.5-17.3 wt %, respectively. The uptake of these gases varies exponentially with the surface area of the B(x)C(y)Z(n) samples, and the uptake of CH(4) varies proportionally with that of CO(2). The uptake of CO(2) for the best BC(2)N sample is 64 wt % at 298 K. The large uptake of both CO(2) and CH(4) gases by BC(2)N betters the performance of graphenes and activated charcoal. First-principles calculations show that the adsorption of CO(2) and CH(4) is more favored on BCN samples compared to graphene.

Graphene Oxide: Some New Insights into an Old Material

Abstract Graphite oxide sheets, now called graphene oxide (GO), can be made from chemical exfoliation of graphite by reactions that have been known for more than 150 years with the first instance carried out by B.C. Brodie in 1859. With oxygenated functional groups attached to its basal plane and edges, GO is insulating but can be readily dispersed in water. GO is commonly “reduced” by thermal annealing or chemical reducing agents to partially restore some of the favourable electrical, mechanical and thermal properties of the pristine graphitic sheets. Therefore, following the landmark discovery of graphene in 2004, there has been resurgent interest in this old material as a promising precursor for the large-scale chemical production of graphene. However, apart from making graphene, GO itself has many intriguing properties. For example, GO can be viewed as an unconventional soft material such as a two-dimensional (2D) polymer, anisotropic colloid, membrane, liquid crystal or amphiphile. In this chapter, some new insights into this old material will be discussed. (1) To start, GO has been reported as a flammable material in old literature decades ago, but as a flame retardant in recent studies. Therefore, is GO a flame retardant or fuel for combustion? This conflict is reconciled by examining the synthesis and purification of GO in conjunction with the thermal instability of GO, which also inspired a new facile photothermal technique for reducing and patterning GO, and an improved purification method that can speed up post-synthetic material processing. (2) A new imaging technique named fluorescence quenching microscopy (FQM) is introduced that allows high throughput, high contrast visualization of GO and graphene-based single atomic sheets on arbitrary substrates and even in solution. (3) Unlike commonly described as hydrophilic in literature, GO is actually amphiphilic and can act as surfactant to disperse oil and insoluble solid materials in water. This unveils intriguing pH and size dependent solution properties of GO, and inspires various interfacial assembly techniques for creating GO and graphene superstructures, including some all-carbon composites useful for photovoltaic devices. Effort towards solution processed all-carbon solar cells is introduced. (4) GO sheets can be squeezed into a crumpled paper-ball structure by the isotropic compression field generated by evaporating aerosol droplets. The crumpled GO or graphene balls have unprecedented morphology and properties for ultrafine particles, such as resistance to further compression and aggregation. (5) GO sheets can be viewed as negatively charged walls for constructing massive arrays of nanofluidic ion channels by simply stacking up to a lamellar membrane through filtration. This provides a simple material solution to solve the lithographical challenges for making nanofluidic systems and devices.