scholarly journals Superconductivity and strong anharmonicity in novel Nb-S phases

Author(s):  
Roman Lucrezi ◽  
Christoph Heil
Keyword(s):  
1990 ◽  
Vol 105 (1) ◽  
pp. 9-14 ◽  
Author(s):  
J. Schreiber ◽  
P. Haertwich
Keyword(s):  

1994 ◽  
Vol 49 (6) ◽  
pp. 663-670
Author(s):  
S. Sh. Soulayman ◽  
C. Ch. Marti ◽  
Ch. Ch. Guilpin

Abstract In this paper we apply the method developed in part I for describing the crystalline state of two and three dimensional inert gases. For strong anharmonicity of fourth order, the equations of state of these gases are obtained. This way we calculate the thermoelastic properties of two and three dimensional argon, krypton and xenon using the Lennard-Jones potential. The corrections to the Helmholtz free energy and thermodynamic properties due to quantum effects are considered. The results are compared with the available experimental data.


2018 ◽  
Vol 97 (1) ◽  
Author(s):  
Guilherme A. S. Ribeiro ◽  
Lorenzo Paulatto ◽  
Raffaello Bianco ◽  
Ion Errea ◽  
Francesco Mauri ◽  
...  

2019 ◽  
Vol 100 (21) ◽  
Author(s):  
Unai Aseginolaza ◽  
Raffaello Bianco ◽  
Lorenzo Monacelli ◽  
Lorenzo Paulatto ◽  
Matteo Calandra ◽  
...  

1992 ◽  
Vol 291 ◽  
Author(s):  
J. Gryko ◽  
R. E. Allen

ABSTRACTIn our first-principles-based molecular dynamics simulations for Si(100), we have found that the total energy U(θ) is rather flat with respect to the bond-rotation angle θ for |θ| <10°, with shallow minima at the positions θ = ± θ0 corresponding to a tilted-dimer geometry. Here we calculate the Fourier transform of the atomic displacements, u(ω), and find a characteristic bond-rotation mode with v − 5 THz. This mode is primarily associated with the upper atom in a dimer, and appears to be a signature of the tilted-dimer reconstruction. At low temperature the vibrations are nearly harmonic, but at high temperature there is strong anharmonicity, and θ appears to exhibit chaotic behavior.


1995 ◽  
Vol 09 (04n05) ◽  
pp. 585-597 ◽  
Author(s):  
V.I. ZUBOV ◽  
M.P. LOBO ◽  
J.N.T. RABELO

The correlative method of the unsymmetrized self-consistent field is used to study the atomic properties of a simple model of an anharmonic crystal with strong anisotropy, namely, a crystal with primitive hexagonal (PH) lattice. The self-consistent potential, Helmholtz free energy and mean-square atomic displacements are obtained in the case of weak anharmonicity. Equations of state are derived and solved. The internal energy and specific heats are calculated. The first quantum corrections are expressed in terms of the de Boer parameter included. An influence of anharmonicity is analyzed. The thermal expansion of the model considered is very anisotropic but the quantum corrections to the lattice parameters are isotropic. The results of calculations are compared with those for one- and two-dimensional models and for the isotropic crystal with the same coordination number as in the PH lattice, i.e. a body-centered cubic crystal. Other things being equal, the coefficient of volume expansion and specific heats of anisotropic crystals are greater than those of isotropic ones. A possibility of studying the strong anharmonicity in anisotropic crystals is discussed.


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