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Published: March 2023
FIG. 7.7 Schematic of (a) basic parallel plate electrostatic actuator ( Errando-Herranz et al., 2020 ) and (b) a comb drive for linear motion. Schematic of (c) a basic scratch drive actuator (SDA) ( Akiyama and Fujita, 1995 ). Step by step crawling motion of the actuator under pulse voltage input. (d) Pressing down of plate with rising voltage pushing the bushing forward. (e) Releasing of the SDA by falling voltage resulting in pulling the plate to right while pinning down the bush due to its shape. (f) Negative rise of voltage resulting in another pressing down of the beam resulting in the bushing moving to the left resulting in net rightward motion of the plate from the starting point. This process repeats for each half cycle. More about this image found in Schematic of (a) basic parallel plate electrostatic actuator ( Errando-Herr...
Images
Published: February 2023
FIG. 1.16 (a) Vertical β-Ga2O3 Schottky diodes with field plate, (b) corresponding electric field profile showing the peak field (in red) redistributed by field plate ( Konishi et al., 2017 ), and (c) bevel field plate Schottky diodes with sidewall angles of 55.7° ( Joishi et al., 2018 ). More about this image found in (a) Vertical β-Ga2O3 Schottky diodes with field plate...
Images
Published: February 2023
FIG. 8.3 Conception of the field-plate termination technique for a vertical diode structure, implemented here in a pn junction diode. The surface electric field at the edge of the junction is modulated by an externally applied gate voltage (VG). Reprinted with permission from Grove et al., IEEE Trans. Electron Devices 14 (3), 157–162 (1967). Copyright 1967 IEEE. More about this image found in Conception of the field-plate termination technique for a vertical diode st...
Images
Published: February 2023
FIG. 8.4 Schematic of an SBD with a single-step field plate with length LFP and height hFP connected to the Schottky electrode. The × and ∗ symbols indicate the positions of peak off-state electric fields, whose intensities are determined by both LFP and hFP. More about this image found in Schematic of an SBD with a single-step field plate with length L...
Images
Images
Published: February 2023
FIG. 8.6 (a) Schematic of the first field-plated β-Ga2O3 SBD. (b) Forward current–voltage (IV) characteristics of the device. (c) Reverse breakdown characteristics of the device. Reprinted with permission from Konishi et al., Appl. Phys. Lett. 110 (10), 103506 (2017). Copyright 2017 AIP Publishing LLC. More about this image found in (a) Schematic of the first field-plated β-Ga2O3 SBD. ...
Images
Published: February 2023
FIG. 8.25 (a) Schematic of a field-plated β-Ga2O3 trench SBD. (b) Cross-sectional scanning electron microscopy image of a fin channel. (c) Reverse breakdown characteristics of field-plated β-Ga2O3 trench SBDs. In comparison with regular β-Ga2O3 SBDs employing both mesa and field-plate terminations, the field-plated trench devices have a much lower leakage current and a much higher Vbr. (d) Forward IV characteristics and differential RON,sp of field-plated β-Ga2O3 trench SBDs under DC and pulsed conditions. A base voltage of 0 V, a pulse width of 1 µs, and a duty cycle of 0.1% are used for the pulsed measurements. Reprinted with permission from Li et al., IEEE Electron Device Lett. 41 (1), 107–110 (2020a). Copyright 2020 IEEE. More about this image found in (a) Schematic of a field-plated β-Ga2O3 trench SBD. (...
Images
Published: February 2023
FIG. 8.28 (a) Schematic of a field-plated β-Ga2O3 SBD with a double-side-cooling flip-chip package. (b) IV waveforms of the double-side-cooled device in surge current tests. (c) IV loops of the double-side-cooled device. Reprinted with permission from Xiao et al., IEEE Trans. Power Electron. 36 (8), 8565–8569 (2021). Copyright 2021 IEEE. More about this image found in (a) Schematic of a field-plated β-Ga2O3 SBD with a do...
Images
Published: February 2023
FIG. 8.7 (a) Schematic of a β-Ga2O3 SBD with an ultrahigh-permittivity field-plate dielectric, where S1 corresponds to a 15-period BaTiO3/SrTiO3 superlattice as the field-plate oxide [(BTO/STO)15 FP] and S2 corresponds to BaTiO3 as the field-plate oxide (BTO FP). The cross-sectional transmission electron microscopy (TEM) image depicts the field-plated region of the S1 structure. (b) Forward IV characteristics and differential RON,sp of a β-Ga2O3 SBD with (BTO/STO)15 FP, a β-Ga2O3 SBD with BTO FP, and a reference SBD without a field plate. (c) Reverse breakdown characteristics of the three different SBD structures. Reprinted with permission from Roy et al., IEEE Electron Device Lett. 42 (8), 1140–1143 (2021). Copyright 2021 IEEE. More about this image found in (a) Schematic of a β-Ga2O3 SBD with an ultrahigh-perm...
Images
Published: February 2023
FIG. 1.21 Lateral β-Ga2O3 power transistors (a) MESFET ( Higashiwaki et al., 2012 ), (b) MOSFET ( Higashiwaki et al., 2013 ) and (c) Field-plate β-Ga2O3 MESFET with breakdown voltage ∼4.4 kV with gate-pad-connected field plate ( Bhattacharyya et al., 2022 ). More about this image found in Lateral β-Ga2O3 power transistors (a) MESFET ( Higash...
Images
Published: March 2023
FIG. 8.7 Microheater geometries of different shapes: (a) meander, (b) S-meander, (c) curved, (d) S-curved, (e) double spiral, (f) drive wheel, (g) elliptical, (h) circular, (i) plane plate, (j) fin shape, (k) honeycomb, and (l) irregular. Reproduced with permission Çakır et al., Sensors 16 (10), 1612 (2016). Copyright 2016 Author(s), licensed under a Creative Commons Attribution 3.0 Unported License. More about this image found in Microheater geometries of different shapes: (a) meander, (b) S-meander, (c)...
Images
Published: February 2023
FIG. 8.9 (a) Schematics of beveled-mesa β-Ga2O3 SBDs with a ∼45° beveled field plate (BFP) and with a small-angle (∼1°) beveled field plate (SABFP). (b) Reverse breakdown characteristics of the BFP-SBD and SABFP-SBD showing higher Vbr than those of mesa-free β-Ga2O3 SBDs that are either unterminated or terminated with a ∼45° beveled surface field plate (SFP; similar to Fig. 8.5 ). (c) Forward IV characteristics and differential RON,sp of SABFP-SBDs with different anode diameters. Reprinted with permission from Allen et al., IEEE Electron Device Lett. 40 (9), 1399–1402 (2019). Copyright 2019 IEEE. More about this image found in (a) Schematics of beveled-mesa β-Ga2O3 SBDs with a ∼4...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425590_008
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
... be the contribution from the interfacial energy. Hence, the interfacial energy sets the lower wavelength limit for the break-up. Perturbative analysis Let us consider a single misfitting plate (of misfit εTδij) inside a matrix as shown in Fig. 8.4 . Assume that the misfitting plate...
Book Chapter
Series: AIPP Books, Professional
Published: March 2023
10.1063/9780735425477_005
EISBN: 978-0-7354-2547-7
ISBN: 978-0-7354-2544-6
... the electric field due to two infinite charged sheets at a 45° angle. Working within the conceptual blending framework, they pointed out that the material and conceptual aspects of the representation may clash, as was the case with a student who drew smaller arrows near the intersection of the two plates...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735425613_007
EISBN: 978-0-7354-2561-3
ISBN: 978-0-7354-2560-6
... performance Two important factors that affect the silicon flat-plate PV module performance are irradiance and solar cell temperature. Likewise, irradiance is also an important factor that affects the CPV performance. On the other hand, the solar cell temperature is relatively less important to the CPV...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735424395_009
EISBN: 978-0-7354-2439-5
ISBN: 978-0-7354-2436-4
... sandwiched between two electrodes. In a bimorph, two separate piezoelectric plates are bonded together to form series or parallel generators. When the two layers are polarized in such a way that the voltage across the two layers increases, a series operation is obtained. Alternatively, they might be poled...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
0
EISBN: 978-0-7354-2559-0
ISBN: 978-0-7354-2556-9
...—Piezoelectric plate structure ,” Phys. Metals Metallogr.   120 , 1304 – 1308 ( 2019 ). 10.1134/S0031918X19130052 Fitzpatrick , M. E. , Fry , A. T. , Holdway , P. , Kandil , F. A. , Shackleton , J. , and Suominen , L. , ▪ ( NPL , Teddington , 2002 ), Vol. 52. Freund...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735424395_002
EISBN: 978-0-7354-2439-5
ISBN: 978-0-7354-2436-4
... A is given by R = L ρ A = [ l 1 ] × [ l 2 ] − 1 = l − 1 For any kind of given material, the electrical resistance can be scaled as l−1 (Fig. 2.9 ). FIG. 2.10 Parallel plate capacitor. Capacitance In the case of a parallel plate capacitor...
Book Chapter
Series: AIPP Books, Principles
Published: March 2023
10.1063/9780735424395_004
EISBN: 978-0-7354-2439-5
ISBN: 978-0-7354-2436-4
... patterned depending on the requirements imposed by the actuation and sensing techniques. One of the most well-known fabricated devices with this technique is DMD, which was fabricated by Texas Instruments ( Van Kessel et al., 1998 ). DMD comprises tilting mirror plates with the electrodes to drive...