2019
Out‐of‐Plane Polarization in Bent Graphene‐Like Zinc Oxide and Nanogenerator Applications
Abstract: Highly efficient piezoelectric nanogenerator operation is demonstrated based on dynamic bending of graphene-like ZnO nanosheets. Energy is harvested by an external resistor by virtue of a strong time-varying piezoelectric polarization component perpendicular to the graphene-like ZnO plane. It is shown analytically and verified numerically using molecular dynamics simulations that the 6m2 point group of flat graphene-like ZnO is reduced to monoclinic m symmetry for bent graphene-like ZnO. The latter symmetry al…
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Cited by 31 publications
(20 citation statements)
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Flexoelectricity-Enhanced Photovoltaic Effect in Self-Polarized Flexible PZT Nanowire Array Devices
ACS Nano
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Abstract
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“…During the simulation, the crystal structure of tetragonal PZT ( P 4 mm ) was employed. Therefore, the polarization change P 3 can be described using polarization in both piezoelectricity and flexoelectricity, which can be expressed as follows: where P 3 = P z is the polarization change along the z direction; e 35 is the piezoelectric coefficient; S 5 = S z is the strain along the z -direction; μ 313 is the flexoelectric coefficient in longitudinal mode; and f 13 is the strain gradient along the z -direction. Figure d presents the flexoelectricity-induced polarization change P 3 at different curvatures.…”
Section: Results
supporting
confidence: 89%
Flexoelectricity-Enhanced Photovoltaic Effect in Self-Polarized Flexible PZT Nanowire Array Devices
ACS Nano
Self Cite
Abstract
Smart CitationsHow this paper cites the one you are viewing
“…During the simulation, the crystal structure of tetragonal PZT ( P 4 mm ) was employed. Therefore, the polarization change P 3 can be described using polarization in both piezoelectricity and flexoelectricity, which can be expressed as follows: where P 3 = P z is the polarization change along the z direction; e 35 is the piezoelectric coefficient; S 5 = S z is the strain along the z -direction; μ 313 is the flexoelectric coefficient in longitudinal mode; and f 13 is the strain gradient along the z -direction. Figure d presents the flexoelectricity-induced polarization change P 3 at different curvatures.…”
Section: Results
supporting
confidence: 89%
Abstract
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“…Similar conclusions are obtained for MX 2 . As shown in Figure S4, the results agree well with those in ref .…”
supporting
confidence: 91%
“…A BN nanoribbon was reported by López-Suárez et al as an energy harvester that can reach an output of 8 × 10 –12 W if the nanoribbon is pre-strained, which, however, is harder to control. The output of the graphene-like ZnO nanogenerator that we reported earlier is 2.11 × 10 –11 W . The cantilever nanogenerator structure that we study here is simpler, as only one side is fixed.…”
mentioning
confidence: 81%
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“…Using barium titanate (BaTiO 3 ) as a case study, it was observed that this compound exhibits a series of distinct crystal structures, namely cubic, tetragonal, orthorhombic, and rhombohedral phases, at specific temperatures, namely 1,460, 120, 0, and ‐90 °C, respectively. [ 151 ] The tetragonal phase of BaTiO 3 is prevalent at room temperature, with Ti 4+ cations exhibiting displacement from the center of a [TiO 6 ] octahedra. This displacement results in the formation of a net polarization along the [001] edge direction.…”
Section: Piezoelectric Biomaterials Designed For Bone and Articular C...
mentioning
confidence: 99%
