2020
DOI: 10.1103/physrevb.102.134101
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Negative capacitance regime in ferroelectrics demystified from nonequilibrium molecular dynamics

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Cited by 5 publications
(4 citation statements)
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“…Although the applied field favors the parallel alignment of dipoles, the applied field of 40 kV cm −1 and thermal fluctuations are too small to overcome the energy barrier for homogeneous polarization switching; see Figure . Fast field changes however drive the system out of thermodynamic equilibrium [ 63,64 ] and as soon as the field is applied, up to 4 % of the dipoles in the negative domain spontaneously align with the field direction. The larger the applied field, the more the dipoles have enough energy to overcome the energy barrier to switch, and we find an increase in the amount of reversed dipoles up to 2% for 20 kV mm −1 , 2.6% for 30 kV mm −1 , and up to 4% for 40 kV mm −1 by initial switching, see also Figure F1a, Supporting Information.…”
Section: Resultsmentioning
confidence: 99%
“…Although the applied field favors the parallel alignment of dipoles, the applied field of 40 kV cm −1 and thermal fluctuations are too small to overcome the energy barrier for homogeneous polarization switching; see Figure . Fast field changes however drive the system out of thermodynamic equilibrium [ 63,64 ] and as soon as the field is applied, up to 4 % of the dipoles in the negative domain spontaneously align with the field direction. The larger the applied field, the more the dipoles have enough energy to overcome the energy barrier to switch, and we find an increase in the amount of reversed dipoles up to 2% for 20 kV mm −1 , 2.6% for 30 kV mm −1 , and up to 4% for 40 kV mm −1 by initial switching, see also Figure F1a, Supporting Information.…”
Section: Resultsmentioning
confidence: 99%
“…The negative slope in the P(E) loop without entering the NC region is theoretically investigated on a single FE capacitor by incorporating the depolarization and stray fields due to the multidomain structure [92]. First-principles nonequilibrium molecular dynamics simulations indicate that the negative slope originates from the partial screening of the polarization and is more likely to occur when a significant electric field is applied to the FE layer [93]. By introducing the term internal electric field, Eint, which is the applied electric field, Eapp, subtracting the depolarization field, the negative slope is obtained in the P(Eint) curves but does not appear in the P(Eapp) curves (Fig.…”
Section: Possible Origins Of Steep Ssmentioning
confidence: 99%
“…This lack of knowledge becomes increasingly important in the case of ultra-fast field applications which drive the system out of equilibrium [9] and may induce new functional properties. For example, a giant electrocaloric response [35] and a negative coupling between field and polarization [10] including transient negative capacitance (NC) [36,37] have already been reported.…”
Section: Introductionmentioning
confidence: 99%
“…Although being counter-intuitive at the first glance NC could be related to the switching of dipoles against the applied field and has been related to antiparallel local depolarization fields which may overcompensate the applied electric field [9,39]. Indeed NC has already been reported during the nucleation of reversed domains [40] or DW propagation [11,37,41,42]. In spite of the progress in this field, the microscopic picture of NC as well as its impact on DW propagation is not yet well investigated.…”
Section: Introductionmentioning
confidence: 99%