2016
DOI: 10.4028/www.scientific.net/ssp.257.203
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Phonon Anharmonicity and Thermodynamic Properties of Strongly Correlated Iron Monosilicide

Abstract: Two computational approaches – a thermodynamic model based on results of ab initio calculations of the ground state and the self-consistent thermodynamic model have been applied to study thermal and elastic properties of iron monosilicide. It is shown that conventional DFT fails to reproduce experimental data for this strongly correlated compound. In addition, we have performed comparative analysis of anharmonicity of the acoustic and optical phonons in FeSi and their impact on the temperature dependencies of … Show more

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Cited by 3 publications
(3 citation statements)
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“…It manifests itself in band gap closure observed by photoemission spectroscopy [10]. The transition is accompanied by unusual temperature dependence of the elastic properties [11,12], heat capacity, unit-cell volume [13,14]. In particular, recent studies of the unit-cell volume as a function of temperature show that the quasiharmonic approximation does not provide a comprehensive description [13].…”
Section: Introductionmentioning
confidence: 99%
“…It manifests itself in band gap closure observed by photoemission spectroscopy [10]. The transition is accompanied by unusual temperature dependence of the elastic properties [11,12], heat capacity, unit-cell volume [13,14]. In particular, recent studies of the unit-cell volume as a function of temperature show that the quasiharmonic approximation does not provide a comprehensive description [13].…”
Section: Introductionmentioning
confidence: 99%
“…where E(V) is the total energy, PV denotes the constant pressure condition, A vib is the vibrational Helmholtz free energy. Using the Debye model of phonon density of states and allowing for the quasi-harmonic approximation, the vibrational contribution A vib can be written as [48] A vib θ D , T ð Þ= nKT 9 8…”
Section: Thermodynamic Propertiesmentioning
confidence: 99%
“…By virtue of the quasi‐harmonic Debye model, the nonequilibrium Gibbs function G* (V, P, T) is in the form of normalG*()normalV,normalP,normalT=normalE0.25em()V+PV+Avib0.25em()normalV,normalT where E(V) is the total energy, PV denotes the constant pressure condition, A vib is the vibrational Helmholtz free energy. Using the Debye model of phonon density of states and allowing for the quasi‐harmonic approximation, the vibrational contribution A vib can be written as Avib(),θDT=italicnKT[]98θDT+3ln()1eθD/TD()θD/T Here, θ D is the Debye temperature, n is the number of atoms, and D(θ D /T) denotes the Debye integral.…”
Section: Structural Electronic and Magnetic Propertiesmentioning
confidence: 99%