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(a) ADF-STEM images and (b) lattice parameter (c) maps under 0 kV/cm and ±13.8 kV/cm. (c) Relationship between Δa and electric field and (d) relationship between Δc and electric field (Sato et al., 2020). Δa and Δc correspond to the difference in the lattice parameters a and c from their average at 0 kV/cm, respectively.
Published: March 2023
FIG. 5.21 (a) ADF-STEM images and (b) lattice parameter (c) maps under 0 kV/cm and ±13.8 kV/cm. (c) Relationship between Δa and electric field and (d) relationship between Δc and electric field ( Sato et al., 2020 ). Δa and Δc correspond More about this image found in (a) ADF-STEM images and (b) lattice parameter (c) maps und...
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Images
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Solar flux distribution simulations using identified parameters at summer solstice solar noon based on the specific aiming strategies: (a) original aiming strategy; (b) improved aiming strategy; and (c) flux density performance.
Published: March 2023
FIG. 5.16 Solar flux distribution simulations using identified parameters at summer solstice solar noon based on the specific aiming strategies: (a) original aiming strategy; (b) improved aiming strategy; and (c) flux density performance. More about this image found in Solar flux distribution simulations using identified parameters at summer s...
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Solar flux distribution simulations using identified parameters at equinox 14:00 based on the specific aiming strategies: (a) original aiming strategy; (b) improved aiming strategy; and (c) flux density performance.
Published: March 2023
FIG. 5.17 Solar flux distribution simulations using identified parameters at equinox 14:00 based on the specific aiming strategies: (a) original aiming strategy; (b) improved aiming strategy; and (c) flux density performance. More about this image found in Solar flux distribution simulations using identified parameters at equinox ...
Images
(a) Substrate and film with lattice parameters as and a0, respectively, where as<a0. (b) Pseudomorphic growth with compressive strain. (c) Misfit dislocation of thin-film growth beyond critical thickness.
Published: March 2023
FIG. 3.13 (a) Substrate and film with lattice parameters a s and a 0 , respectively, where a s < a 0 . (b) Pseudomorphic growth with compressive strain. (c) Misfit dislocation of thin-film growth beyond critical thickness. More about this image found in (a) Substrate and film with lattice parameters a s and a 0...
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(a) Lattice parameters, a and c, and (b) sublattice spacing, dIL and dIS, of PZT and SRO measured from HRTEM image (Jia et al., 2007). The dotted lines indicate the location of the PZT/SRO interface. The open and filled symbols denote the experimental and calculated values, respectively. (c) Schematic illustration of PZT and SRO unit cells with the definition of dIL and dIS. Panels (a) and (b) were reproduced with permission from Jia et al., Nat. Mater. 6, 64–69 (2007).
Published: March 2023
FIG. 5.3 (a) Lattice parameters, a and c, and (b) sublattice spacing, dIL and dIS, of PZT and SRO measured from HRTEM image ( Jia et al., 2007 ). The dotted lines indicate the location of the PZT/SRO interface. The open and filled More about this image found in (a) Lattice parameters, a and c, and (b) ...
Book Chapter
Series: AIPP Books, Principles
Published: July 2022
10.1063/9780735424999_006
EISBN: 978-0-7354-2499-9
ISBN: 978-0-7354-2496-8
... parameters. For researchers and scientists, the PV cell model parameter estimation is a challenging issue owing to the unavailability of all their parameters ( Yousri et al., 2020 ). As the PV cells have nonlinear I–V characteristics, the PV cell model parameter estimation problem is considered...
Images
Closed-loop state trajectories under P control with K = −3 with a depolarizing error parameter of 0.05 in the simulations labeled “0.05, Noise” a depolarizing error parameter of 0.005 in the simulations labeled “0.005, Noise,” and a depolarizing error parameter of 0.0005 in the simulations labeled “0.0005, Noise.” 1 shot is used in all cases.
Published: March 2023
FIG. 8.20 Closed-loop state trajectories under P control with K = −3 with a depolarizing error parameter of 0.05 in the simulations labeled “0.05, Noise” a depolarizing error parameter of 0.005 in the simulations labeled “0.005, Noise,” and a depolarizing error parameter of 0.0005 More about this image found in Closed-loop state trajectories under P control with K = −3...
Images
Closed-loop state trajectories under P control with K = −3 with a depolarizing noise parameter of 0.05 in the simulation labeled “Quantum, Noise,” with 1 shot.
Published: March 2023
FIG. 8.16 Closed-loop state trajectories under P control with K = −3 with a depolarizing noise parameter of 0.05 in the simulation labeled “Quantum, Noise,” with 1 shot. More about this image found in Closed-loop state trajectories under P control with K = −3...
Images
Closed-loop input trajectories under P control with K = −3 with a depolarizing noise parameter of 0.05 in the simulation labeled “Quantum, Noise,” with 1 shot.
Published: March 2023
FIG. 8.17 Closed-loop input trajectories under P control with K = −3 with a depolarizing noise parameter of 0.05 in the simulation labeled “Quantum, Noise,” with 1 shot. More about this image found in Closed-loop input trajectories under P control with K = −3...
Images
Closed-loop state trajectories under P control with K = −2 with a depolarizing noise parameter of 0.05 in the simulation labeled “Quantum, Noise,” with 1 shot.
Published: March 2023
FIG. 8.18 Closed-loop state trajectories under P control with K = −2 with a depolarizing noise parameter of 0.05 in the simulation labeled “Quantum, Noise,” with 1 shot. More about this image found in Closed-loop state trajectories under P control with K = −2...
Images
HRTEM image of PZT/SRO interface (Jia et al., 2007) showing the measured lattice parameters in the film and substrate. The thick arrow denotes the interface. dIL and dIS are the shift parameters as defined in Fig. 5.3(c).
Published: March 2023
FIG. 5.2 HRTEM image of PZT/SRO interface ( Jia et al., 2007 ) showing the measured lattice parameters in the film and substrate. The thick arrow denotes the interface. dIL and dIS are the shift parameters as defined in Fig. 5.3(c) . Reproduced More about this image found in HRTEM image of PZT/SRO interface ( Jia et al., 2007 ) show...
Images
Solar flux distributions produced by a relatively good heliostat. (a) and (b) indicate the actual distribution. (c) and (d) compared the identification results through solar flux distribution simulations using identified and designed parameters.
Published: March 2023
FIG. 5.12 Solar flux distributions produced by a relatively good heliostat. (a) and (b) indicate the actual distribution. (c) and (d) compared the identification results through solar flux distribution simulations using identified and designed parameters. More about this image found in Solar flux distributions produced by a relatively good heliostat. (a) and (...
Images
Solar flux distributions produced by a badly deteriorated heliostat. (a) and (b) indicate the actual distribution. (c) and (d) compared the identification results through solar flux distribution simulations using identified and designed parameters.
Published: March 2023
FIG. 5.13 Solar flux distributions produced by a badly deteriorated heliostat. (a) and (b) indicate the actual distribution. (c) and (d) compared the identification results through solar flux distribution simulations using identified and designed parameters. More about this image found in Solar flux distributions produced by a badly deteriorated heliostat. (a) an...
Images
Closed-loop state trajectories under P control with K = −3 with a depolarizing error parameter of 0.05 in the simulations labeled “1 Shot, Noise” and “10 Shots, Noise.” These two simulations use 1 shot and 10 shots, respectively.
Published: March 2023
FIG. 8.19 Closed-loop state trajectories under P control with K = −3 with a depolarizing error parameter of 0.05 in the simulations labeled “1 Shot, Noise” and “10 Shots, Noise.” These two simulations use 1 shot and 10 shots, respectively. More about this image found in Closed-loop state trajectories under P control with K = −3...
Images
Comparison of semiconductor material parameters highlighting Ga2O3 main advantages: low conduction and switching losses, high-voltage capability, and high-temperature operation (low leakage).
Published: February 2023
FIG. 13.1 Comparison of semiconductor material parameters highlighting Ga2O3 main advantages: low conduction and switching losses, high-voltage capability, and high-temperature operation (low leakage). More about this image found in Comparison of semiconductor material parameters highlighting Ga2...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425613_frontmatter
EISBN: 978-0-7354-2561-3
ISBN: 978-0-7354-2560-6
...Front Matter Toward Better Photovoltaic Systems: Design, Simulation, Optimization, Analysis, and Operations is a comprehensive introduction to simulation and design with a particular focus on optimization, analysis, evaluation, parameter estimation, and defect detection. It offers...