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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Ceresoli, Davide
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (13/13 displayed)
- 2024Weyl semimetallic phase in high pressure CrSb 2 and structural compression studies of its high pressure polymorphs
- 2024Weyl semimetallic phase in high pressure CrSb$_2$ and structural compression studies of its high pressure polymorphs
- 2024Weyl semimetallic phase in high pressure CrSb2 and structural compression studies of its high pressure polymorphs
- 2023Elucidating the superexchange mechanisms in magnetic coordination polymer [Co(HCOO) 2 (H2O) 2 ] ∞ through chemical bonding analysiscitations
- 2022Anharmonic motion and aspherical nuclear probability density functions in cesium halidescitations
- 2021Electronic Polarizability Induced Cooper-like Pairing and Energy Gap in High-Tc superconductors
- 2021High pressure structure studies of three SrGeO3 polymorphs – Amorphization under pressurecitations
- 2020First-principles evaluation of the secondary electron yield γN from polyethylene surfacecitations
- 2018Magnetic Moments and Electron Transport through Chromium-Based Antiferromagnetic Nanojunctionscitations
- 2017High-pressure phase diagram, structural transitions, and persistent non-metallicity of BaBiO$_3$: theory and experiment
- 2017Ab initio study of properties of BaBiO<SUB>3</SUB> at high pressure
- 2008Pressure-induced insulator-metal and structural transitions of BaBiO<SUB>3</SUB> from first principles LDA+U
- 2004Non-melting and self-wetting of alkali halide surfaces at high temperatures
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document
Non-melting and self-wetting of alkali halide surfaces at high temperatures
Abstract
We investigated theoretically the high temperature thermodynamic properties and the (lack of) self-wetting of ionic crystal surfaces, with NaCl(100) as a prototype case. We found by classical molecular dynamics simulations that NaCl(100) is a non-melting crystal surface and can be overheated to a spinodal temperature T<SUB>S</SUB> 150 K above the bulk melting temperature (T_M). While surface non-melting is in itself well known, and is observed on semiconductors as well as on close packed metal surfaces, the basic mechanism for NaCl appears to be different from either of them. Moreover, there appear to be two distinct metastability regimes of solid NaCl(100) above T_M. The first regime T<SUB>M</SUB> < T < T_1, (T<SUB>1</SUB> - T<SUB>M</SUB> = 60 K) the metastable solid surface is strongly protected by a nucleation barrier of large thickness. This thickness decreases with temperature, until it drops to a lattice spacing a at T_1. In the second regime T<SUB>1</SUB> < T < T<SUB>S</SUB> is characterized by a ``fragile'' metastability, with a nucleation barrier one lattice spacing thick. Here, the smallest seed is able to cause melting, i.e., it is enough to melt the first monolayer for the liquid to break through and melt the whole system. A basic explanation of these facts and of the two regimes is given, based on a short-range oscillatory interaction between the solid-liquid and the liquid-vapor interfaces. In addition, we also simulated a liquid NaCl nanodroplet, deposited on a solid NaCl surface in the vicinity of the bulk melting point. The anomalously large contact angle measured long ago by Mutaftschiev [1] is well reproduced by this realistic molecular dynamics droplet simulation. Based on these results, and on independent determinations of the liquid-vapor (γ_LV) and the solid-vapor interface free energy (γ_SV) an estimate of the solid-liquid interface free energy (γ_SL) is extracted. The solid-vapor surface free energy turns out to be anomalously small and similar to the liquid-vapor one, providing a direct thermodynamic explanation of the reduced wetting ability of the ionic melt. <P />G. Grange and B. Mutaftschiev, Surf. Sci. 47, 723 (1975)....