3.0a program. The results are presented in Additional file 1: Table S1. The dependence of the interlayer distance (d 002) on the degree of unidimensional disorder, γ, in graphite-like BN was determined. Fludarabine clinical trial It was established that in the perfectly ordered structure with γ = 0, d 002 is equal to 0.333 nm. The value of d 002 increased uniformly with an increase in γ; for γ = 1, the determined value of d 002 is 0.343 nm [41]. The MoS2, WS2, and g-C3N4 interlayer spacing was 0.313 nm. The h-BCN interlayer spacing was determined to be approximately 0.335 nm [42] or approximately 0.35 nm [43], which is close

to the typical d 002 spacing in hexagonal structures and slightly longer than the distance in h-BN and graphite. In our case, the interlayer spacing was calculated to be 0.349 nm for bulk h-BN (1:3) and 0.341 nm for bulk h-BCN. After exfoliation, wider interlayer spacings were expected, as was observed in the exfoliation of graphite [29]. However, as is evident from Additional file 1: Table S1, the value of d 002, depending upon the number

of layers, decreases to a value of approximately 0.31 nm. Banhart [44] observed a similar check details reduction in the spacing of graphene layers in carbon onions and interpreted the reduction as a compression and the transition of orbitals from sp2 to sp3. In the Fe3C encapsulated inside chain-like carbon nanocapsules, the smaller Thiazovivin nmr spacing of the graphene layers is related to the Fe3C particle. The bonding between the graphene layers and the Fe3C particle may contribute to the transition of orbitals from sp2 to sp3. The same effect – decreasing of d-spacing – was due to the interaction of the energetic particles with the carbon nanostructures [45]. In our case, the reduction of d-spacing is most likely due to the compression pressure caused by the collapse of the cavitation bubbles. Additional file 1: Figures S1 and S3 show high-resolution transmission

electron microscopy (HRTEM) micrographs of exfoliated MoS2 and WS2 sheets that were obtained using Reverse transcriptase ultrasound-assisted exfoliation. The d-spacing of MoS2 (0.639 nm) and WS2 (1.195 nm) corresponds with the (002) plane of the PDF 02-1133 card and the (205) plane of the PDF 08-0237 card, respectively. Using the Miller-Bravais indices (hkil) for layered materials such as graphene, each set of diffraction spots exhibited an inner hexagon that corresponds with a (1-110) index and an outer hexagon that corresponds with a (1-210) index. The intensity profiles of the graphene diffraction patterns could therefore be used to determine the number of layers in the graphite sheet.