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| 001 | 279893 | ||
| 005 | 20210129221151.0 | ||
| 024 | 7 | _ | |a 10.1063/1.4936575 |2 doi |
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| 024 | 7 | _ | |a 1089-7690 |2 ISSN |
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| 037 | _ | _ | |a FZJ-2015-07769 |
| 082 | _ | _ | |a 540 |
| 100 | 1 | _ | |a Sukhomlinov, Sergey |0 P:(DE-Juel1)161468 |b 0 |e Corresponding author |u fzj |
| 245 | _ | _ | |a Charge-transfer potentials for ionic crystals: Cauchy violation, LO-TO splitting, and the necessity of an ionic reference state |
| 260 | _ | _ | |a Melville, NY |c 2015 |b American Institute of Physics |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 520 | _ | _ | |a In this work, we study how including charge transfer into force fields affects the predicted elastic and vibrational Γ-point properties of ionic crystals, in particular those of rock salt. In both analytical and numerical calculations, we find that charge transfer generally leads to a negative contribution to the Cauchy pressure, PC ≡ C12 − C66, where C12 and C66 are elements of the elastictensor. This contribution increases in magnitude with pressure for different charge-transfer approaches in agreement with results obtained with density functional theory(DFT). However, details of the charge-transfer models determine the pressure dependence of the longitudinal optical-transverse optical splitting and that for partial charges. These last two quantities increase with density as long as the chemical hardness depends at most weakly on the environment while experiments and DFT find a decrease. In order to reflect the correct trends, the charge-transfer expansion has to be made around ions and the chemical (bond)hardness has to increase roughly exponentially with inverse density or bond lengths. Finally, the adjustable force-field parameters only turn out meaningful, when the expansion is made around ions. |
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| 700 | 1 | _ | |a Müser, Martin |0 P:(DE-Juel1)144442 |b 1 |e Corresponding author |
| 773 | _ | _ | |a 10.1063/1.4936575 |g Vol. 143, no. 22, p. 224101 - |0 PERI:(DE-600)1473050-9 |n 22 |p 224101 - |t The journal of chemical physics |v 143 |y 2015 |x 1089-7690 |
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