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Pavel Rubin

Publications and source records attributed to Pavel Rubin.

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Gas sensing potential of stacked graphene/h-BN structures: a DFT-based investigation

Using periodic DFT, we examined the adsorption of NO2, NH3, and O3 on the h-BN side of a graphene/h-BN heterostructure designed as a model gas sensor material. The h-BN overlayer serves both as an active adsorption surface and as protection that may reduce irreversible processes such as graphene oxidation. Two model systems were considered: an extended graphene/h-BN bilayer (B36N36C72) and a graphene sheet partially covered by a smaller h-BN island (B11N11C72). Their electronic structures differ strongly near the Dirac point. In the extended bilayer, the Fermi level remains aligned with that of pristine graphene, indicating negligible charge transfer. In the island-covered system, the Fermi level shifts to lower energies, reflecting electron transfer from graphene to h-BN. These differences lead to distinct adsorption behavior. NO2 binds much more strongly to B11N11C72, forming a chemical bond, while O3 dissociates on this surface but remains intact on the extended bilayer. NH3 unusually acts as an electron acceptor in the island system. Overall, NO2 and O3 substantially increase graphene conductivity, whereas NH3 induces much weaker changes. These results highlight the potential of graphene/h-BN heterostructures for gas sensing.

cond-mat.mtrl-sci

Magnetic phase diagram of the spin-1 two-dimensional J1-J3 Heisenberg model on a triangular lattice

The spin-1 Heisenberg model on a triangular lattice with the ferromagnetic nearest, $J_1=-(1-p)J,$ $J>0$, and antiferromagnetic third-nearest-neighbor, $J_3=pJ$, exchange interactions is studied in the range of the parameter $0 \leqslant p \leqslant 1$. Mori's projection operator technique is used as a method, which retains the rotation symmetry of spin components and does not anticipate any magnetic ordering. For zero temperature several phase transitions are observed. At $p\approx 0.2$ the ground state is transformed from the ferromagnetic spin structure into a disordered state, which in its turn is changed to an antiferromagnetic long-range ordered state with the incommensurate ordering vector ${\bf Q = Q^\prime} \approx (1.16, 0)$ at $p\approx 0.31$. With the further growth of $p$ the ordering vector moves along the line ${\bf Q^\prime-Q_c}$ to the commensurate point ${\bf Q_c}=(\frac{2π}{3}, 0)$, which is reached at $p = 1$. The final state with an antiferromagnetic long-range order can be conceived as four interpenetrating sublattices with the $120^\circ$ spin structure on each of them. Obtained results are used for interpretation of the incommensurate magnetic ordering observed in NiGa$_2$S$_4$.

cond-mat.str-el