scholarly journals Lattice parameters and electronic bandgap of orthorhombic potassium sodium niobate K$$_{0.5}$$Na$$_{0.5}$$NbO$$_{3}$$ from density-functional theory

2021 ◽  
Vol 94 (8) ◽  
Author(s):  
Nithin Bidaraguppe Ramesh ◽  
Falko Schmidt ◽  
Arno Schindlmayr

Abstract We perform a theoretical analysis of the structural and electronic properties of sodium potassium niobate K$$_{1-x}$$ 1 - x Na$$_{x}$$ x NbO$$_{3}$$ 3 in the orthorhombic room-temperature phase, based on density-functional theory in combination with the supercell approach. Our results for $$x=0$$ x = 0 and $$x=0.5$$ x = 0.5 are in very good agreement with experimental measurements and establish that the lattice parameters decrease linearly with increasing Na contents, disproving earlier theoretical studies based on the virtual-crystal approximation that claimed a highly nonlinear behavior with a significant structural distortion and volume reduction in K$$_{0.5}$$ 0.5 Na$$_{0.5}$$ 0.5 NbO$$_{3}$$ 3 compared to both end members of the solid solution. Furthermore, we find that the electronic bandgap varies very little between $$x=0$$ x = 0 and $$x=0.5$$ x = 0.5 , reflecting the small changes in the lattice parameters. Graphic abstract

2016 ◽  
Vol 18 (44) ◽  
pp. 30686-30695 ◽  
Author(s):  
Pablo Rivero ◽  
Claudio Cazorla

By using first-principles methods based on density functional theory we revisited the zero-temperature phase diagram of stoichiometric SrCoO3, a ferromagnetic metallic perovskite that undergoes significant structural, electronic, and magnetic changes as its content of oxygen is decreased.


2021 ◽  
Vol 252 ◽  
pp. 03039
Author(s):  
Qiang Wei-rong ◽  
Wang Xiao-mei ◽  
Liu Wei-qi

Based on density functional theory(DFT), using virtual crystal approximation and generalized gradient approximation(GGA)with pseudopotential method, the lattices and energies for five crystallines of vanadium hydrides are optimized and calculated. The phonon densities of states are calculated based on density functional perturbation theory(DFPT). The standard Heat capacities, Entropies, Helmholtz free energies and Gibbs functions of vanadium and its hydride are deduced at 298.15K. The calculated results are discussed and compared with experimental data.


2020 ◽  
Vol 11 (24) ◽  
pp. 10463-10468
Author(s):  
Chuan-Jia Tong ◽  
Holly J. Edwards ◽  
Theodore D. C. Hobson ◽  
Ken Durose ◽  
Vinod R. Dhanak ◽  
...  

2016 ◽  
Vol 18 (27) ◽  
pp. 18323-18335 ◽  
Author(s):  
Anouar Benali ◽  
Luke Shulenburger ◽  
Jaron T. Krogel ◽  
Xiaoliang Zhong ◽  
Paul R. C. Kent ◽  
...  

Spin density surfaces in the low temperature phase of Ti4O7: the ferromagnetic state (left panel), and the lowest-energy antiferromagnetic state (right panel). The figures were generated using self-interaction corrected density functional theory.


2008 ◽  
Vol 52 ◽  
pp. 165-174 ◽  
Author(s):  
Aparna Chakrabarti ◽  
S.R. Barman

The electronic and structural properties of different members of the Ni-Mn-Ga family calculated by ab initio density functional theory are discussed. From total energy calculations, we show that the martensitic phase is the stable low temperature phase. Moreover, occurrence of ferromagnetic and paramagnetic martensitic phases for Ni2MnGa and Ni2.25Mn0.75Ga, respectively, are explained. Modifications in the density of states near the Fermi level EF are observed across the martensitic transition for Ni2MnGa, as well as in Mn2NiGa. While Ni2MnGa is ferromagnetic, we find Mn2NiGa to be ferrimagnetic. The calculated lattice constants and the magnetic moments are in good agreement with experiment.


2019 ◽  
Vol 234 (4) ◽  
pp. 211-217
Author(s):  
Hans Grimmer ◽  
Bernard Delley

Abstract Density functional theory (DFT) calculations have been performed on five models of periodic, polysynthetic twin interfaces in the ambient-temperature phase of KLiSO4, which has space group P63. The models represent the three merohedric twin laws (m||z, 2⊥z and 1̅) with boundary plane (1 0 1̅ 0), also with boundary plane (0 0 0 1) in case of m, and with boundary plane (1 2̅ 1 0) in case of 1̅. The models satisfy stoichiometry at the boundary plane and maintain the fourfold coordination of the Li and S atoms and the twofold coordination of the oxygen atoms. Relaxed lattice parameters and atomic positions were determined by DFT, using the DMol3 code with functional PBEsol. The energy difference between polysynthetic twin and single crystal per primitive cell of the twin is 0.0009 eV for m(0 0 0 1), 0.09 eV for 1̅(1 0 1̅ 0), 0.58 eV for m(1 0 1̅ 0) and 0.55 eV for 2(1 0 1̅ 0). In KLiSO4 crystals grown from aqueous solutions the first twin was frequently observed, similarly also the second twin in Cr-doped crystals, whereas the third twin appeared only rarely and the fourth was not observed. Not only for KLiSO4 but also for quartz, the energy of twins and the frequency of their occurrence are closely connected for crystals grown from aqueous solutions, whereas for the formation of transformation twins the availability of twin nuclei plays a major role.


2018 ◽  
Vol 60 (5) ◽  
pp. 864
Author(s):  
Ю.В. Луняков

AbstractAs a result of an evolutionary search based on the density functional theory, a new low-symmetry structure of silicide Mg_2Si under pressure was discovered. This structure can exist along with the known structures of the symmetry Pnma and P63/mmc and is stable at a pressure of about 20 GPa. The lattice parameters of the discovered structure are in better agreement with the experimental values than the lattice parameters of the known structures.


2008 ◽  
Vol 1079 ◽  
Author(s):  
Dae-Hee Kim ◽  
Hwa-Il Seo ◽  
Yeong-Cheol Kim

ABSTRACTPd segregation at (001) B2-NiSi/Si epitaxial interface was studied by using density functional theory (DFT). An epitaxial interface between 2×2×4 (001) B2-NiSi supercell and 1×1×2 (001) Si supercell was first constructed by adjusting the lattice parameters of B2-NiSi structure to be matched with those of Si structure. We chose Ni atoms as terminating layer of the B2-NiSi, and an equilibrium gap between the B2-NiSi and Si was calculated to be 1.1 Å. The Ni atoms in the structure moved away from the original positions along z-direction in a systematic way during the energy minimization. Two different Ni sites were identified at the interface and the bulk, respectively. The Ni sites at the interface farther away from the interface were more favorable for Pd substitution.


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