2022
DOI: 10.1103/physrevapplied.17.024013
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Nonvolatile Ferroelastic Strain from Flexoelectric Internal Bias Engineering

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Cited by 10 publications
(7 citation statements)
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“…Considering possible existence of multiple sub-coercive electric states, the single domain state with the accompanied remanent tension along the polarization direction can be favourable for larger PV response in a poled direction. Taking into account that internal bias field giving rise to opposite remanent stresses can be also formed by growth conditions, thermal/electrical [76,77] history or doping [78], our results on the well-controlled model material can explain differences or lack of reproducibility in the literature. Regardless the way of stress introduction: either material fabrication [79,80] or post-processing techniques, the strain engineering can be considered as a key enabling strategy for tuning and optimizing PV properties in FEs.…”
Section: Discussionmentioning
confidence: 81%
“…Considering possible existence of multiple sub-coercive electric states, the single domain state with the accompanied remanent tension along the polarization direction can be favourable for larger PV response in a poled direction. Taking into account that internal bias field giving rise to opposite remanent stresses can be also formed by growth conditions, thermal/electrical [76,77] history or doping [78], our results on the well-controlled model material can explain differences or lack of reproducibility in the literature. Regardless the way of stress introduction: either material fabrication [79,80] or post-processing techniques, the strain engineering can be considered as a key enabling strategy for tuning and optimizing PV properties in FEs.…”
Section: Discussionmentioning
confidence: 81%
“…We use the framework of generalized gradient approximation (GGA) , embodied in the Quantum Espresso open-source package for conducting this calculation. The GGA, along with the Perdew–Burke–Ernzerhof (PBE) form, serves as the exchange-correlation functional with ultrasoft pseudopotentials. , We account for the van der Waals interaction using the semiempirical Grimme functional (DFT-D2 (Grimme-D2)), also employed in earlier works. The wave functions are expanded by using a plane wave basis set with a kinetic energy cutoff of 40 Ry (544 eV) and an energy cutoff of 450 Ry (6123 eV) for charge density (and the self-consistent field potential). It is important to note that the energy cutoff defines the maximum energy for the plane wave basis set, ensuring that the basis set contains sufficient wave functions to accurately describe the electronic structure of the system.…”
Section: Methodsmentioning
confidence: 99%
“… 41 , 42 We account for the van der Waals interaction using the semiempirical Grimme functional (DFT-D2 (Grimme-D2)), 43 also employed in earlier works. 44 47 The wave functions are expanded by using a plane wave basis set with a kinetic energy cutoff of 40 Ry (544 eV) and an energy cutoff of 450 Ry (6123 eV) for charge density (and the self-consistent field potential). It is important to note that the energy cutoff defines the maximum energy for the plane wave basis set, ensuring that the basis set contains sufficient wave functions to accurately describe the electronic structure of the system.…”
Section: Methodsmentioning
confidence: 99%
“…The real space lattices of TBG systems were constructed using the ATOMISTIX TOOLKIT (QuantumATK) package . All the first-principles simulations were conducted with generalized gradient approximation (GGA) assimilated in the Quantum Espresso open source package. , The Perdew–Burke–Ernzerhof (PBE) form and GGA have been used as the exchange-correlation functional .…”
Section: Methodsmentioning
confidence: 99%