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The structure of amorphous materials-continuous random networks (CRN) vs. CRN containing randomly dispersed crystallites-has been debated for decades. In two-dimensional (2D) materials, this question can be addressed more directly. Recently, controlled experimental conditions and atomic-resolution imaging found that monolayer amorphous carbon (MAC) is a CRN containing random graphene nanocrystallites. Here we report Monte Carlo simulations of the structure evolution of monolayer amorphous boron nitride (ma-BN) and demonstrate that it also features distorted sp2-bonding, but it has a purely CRN structure. The key difference is that, at low temperatures, C atoms easily form hexagons, whereas the probability to form canonical B-N-B-N-B-N hexagons is very low. On the other hand, hexagons have lower energy than non-hexagons, which results in hexagonal CRN regions that grow much like nanocrystallites in MAC. The net conclusion is that two distinct forms of amorphous structure are possible in 2D materials. The as-generated ma-BN is stable at room-temperature and insulating.
While crystalline two-dimensional materials have become an experimental reality during the past few years, an amorphous 2-D material has not been reported before. Here, using electron irradiation we create an sp2-hybridized one-atom-thick flat carbon
Recently amorphous oxide semiconductors (AOS) have gained commercial interest due to their low-temperature processability, high mobility and areal uniformity for display backplanes and other large area applications. A multi-cation amorphous oxide (a-
Bulk amorphous materials have been studied extensively and are widely used, yet their atomic arrangement remains an open issue. Although they are generally believed to be Zachariasen continuous random networks, recent experimental evidence favours th
In this study we present a theoretical investigation of structural, electronic and mechanical properties of pentagonal monolayers of carbon (p-graphene), boron nitride (p-B$_{2}$N$_{4}$ and p-B$_{4}$N$_{2}$) and silver azide (p-AgN$_{3}$) by performi
We present a general picture of the exciton properties of layered materials in terms of the excitations of their single-layer building blocks. To this end, we derive a model excitonic hamiltonian by drawing an analogy with molecular crystals, which a