Increasingly, two-dimensional (2D) materials are being investigated for their potential use as surface-enhanced Raman spectroscopy (SERS) active substrates. Hexagonal Boron Nitride (hBN), a layered 2D material analogous to graphene, is mostly used as a passivation layer/dielectric substrate for nanoelectronics application. We have investigated the SERS activity of few-layer hBN film synthesized on copper foil using atmospheric pressure chemical vapor deposition. We have drop casted the probe molecules onto the hBN substrate and measured the enhancement effect due to the substrate using a 532 nm excitation laser. We observed an enhancement of ≈10³ for malachite green and ≈10⁴ for methylene blue and rhodamine 6G dyes, respectively. The observed enhancement factors are consistent with the theoretically calculated interaction energies of MB > R6G > MG with a single layer of hBN. We also observed that the enhancement is independent of the film thickness and surface morphology. We demonstrate that the hBN films are highly stable, and even for older hBN films prepared 7 months earlier, we were able to achieve similar enhancements when compared to freshly prepared films. Our detailed results and analyses demonstrate the versatility and durability of hBN films for SERS applications.

Clean energy is one of the immediate requirements all over the world to tackle the global energy demands. Natural gas hydrates (NGHs) are one of the proposed alternatives that could be used to extract methane as clean energy and simultaneously sequestrate carbon dioxide. However, the formation of CH₄–CO₂ mixed hydrates and the first hydrate layer besides the interface reduces the rate of CO₂ sequestration and methane extraction in NGHs, and thus, multistep extraction of methane is one of the proposed solutions. We report the atomic level factors that could enhance CO₂ sequestration in the newly formed first hydrate layer besides the interface in the presence of flue and noble gases using DFT calculations and molecular dynamics simulations at 250 K and 0.15 kbar. The simulations show the formation of stable dual cages (large-large or small-large) that lead to the formation of a four-caged, Y-shaped cluster (growth synthon) which leads to the formation of a hydrate unit cell in heterogeneous medium. Among the flue and noble gases, only argon forms energetically favorable dual cages with itself and CO₂ due to which enhanced CO₂ sequestration is observed at different concentrations of Ar and CO₂ where the CO₂ : Ar (2.5 : 1.5) system shows the best CO₂ sequestration in the first layer besides the interface. The results also provide understanding into the previously reported concentration dependent CO₂ selectivity in sI hydrates in the presence of third gases (N₂ and H₂S).

Odd–even alternation is observed in the calorimetric properties ( T _t , Δ H _t and Δ S _t ) in N n –O16s, but not in N n –O15s. This is explained on the basis of differences in terminal methyl group packing.

In some binary alloys, the solute exhibits high or fast diffusion with low activation energy. In order to understand this, diffusion of solute atoms through a lattice of body centered cubic solvent atoms has been investigated with molecular dynamics technique. Surprisingly, solutes exhibit two distinct diffusivity maxima. Solutes migrate through the lattice mainly by diffusion from one tetrahedral void to another (tt) and, less frequently, by diffusion from a tetrahedral to an octahedral void (to) or reverse jumps (ot). Solutes with maximum diffusivity show smooth decay of the velocity autocorrelation function without backscattering. The average force on the solutes of various diameters correlates well with the position and intensity of the diffusivity maxima exhibited by the solutes. This suggests that the explanation for the diffusivity maxima lies in the levitation effect, which suggests a lowered force on the solute at the diffusivity maxima. The activation energy computed for the solutes of different sizes confirms this interpretation as it is lower for the solutes at the diffusivity maxima. Calculations with blocking of octahedral voids show that the second diffusivity maximum has significant contributions from the to diffusion path. These findings obtained here explain the fast solute/impurity atom diffusivity and low activation energies seen in the literature in many of the alloys, such as Co in γ-U and β-Zr, Cu in Pr, or Au in Th.