Structure and properties of implanted steels

The “Generalized Skettrup Model” and Lattice Thermal Capacity of Graphene, h-BN, MoS2, and WS2 Flakes

“…In this article, temperature dependencies of both harmonic and anharmonic components the C p (T) function are simulated for square flakes of graphene, hexagonal layered boron nitride (h-BN), molybdenum disulphide (MoS 2 ) and tungsten disulphide (WS 2 ) based on the static and essentially many-body "Generalized Skettrup Model" (GSM), introduced and implemented in its original 3-dimensional (3D) version for realistic simulations on the near-band-gap and intra-gap electronic as well as corresponding optical spectra (bandtails) of 3D polycrystalline and spatially inhomogeneous amorphous semiconductors and insulators elsewhere in Refs. [12][13][14][15]16; see also Ref. 17 for more details.…”

“…17 for more details. The unique many-body statistical approach becomes a distinctive feature of the 3D GSM: original singleparticle statistics (and DOS function) of bulk solids (of formally infinite sizes) implemented essentially within framework of the famous Debye's model might be replaced with their many-particle counterparts (though still based on very similar set of the plane-wave basis functions) for the polycrystalline, 15,17 spatially non-homogeneous amorphous, [12][13][14]17,16 and nano-structured solids with finite critical sizes (spatial extents): see second chapter of Ref. 17 and its Appendix D for more details.…”

Structural-and-Phase Transformations in Fe-4.10 and 7.25 at.% Mn Alloys under Intensity External Actions

“…In [2,[4][5][6][7][8], impressive processes of structural-phase transformations with the formation of strongly nonequilibrium states were recorded. There are a large number of examples of the formation of nonequilibrium highly defect states under the action of continuous and powerful pulsed ion beams [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26]. In works [1,3,[27][28][29][30][31][32], reverse processes of instantaneous rearrangement of nonequilibrium (metastable) media during ion bombardment at anomalously low temperatures with the transition of these media to states approaching equilibrium as much as possible were found.…”