imported>John R. Brews |
|
(4 intermediate revisions by one other user not shown) |
Line 1: |
Line 1: |
| | {{AccountNotLive}} |
| {{TOC|right}} | | {{TOC|right}} |
| ==Devices== | | ==Devices== |
Line 27: |
Line 28: |
| |Fermi function.PNG|Fermi occupancy function ''vs''. energy departure from Fermi level in volts for three temperatures | | |Fermi function.PNG|Fermi occupancy function ''vs''. energy departure from Fermi level in volts for three temperatures |
| |FCC Fermi surface.PNG|Fermi surface in '''k'''-space for a nearly filled band in the face-centered cubic lattice | | |FCC Fermi surface.PNG|Fermi surface in '''k'''-space for a nearly filled band in the face-centered cubic lattice |
| | |Electron probabilities in GaAs quantum well.png|Electron probabilities in lowest two quantum states of a 160Ǻ GaAs quantum well in a GaAs-GaAlAs quantum heterostructure. |
| }} | | }} |
| | |
| ==More devices== | | ==More devices== |
| {{Gallery-mixed | | {{Gallery-mixed |
Line 42: |
Line 45: |
| |Schottky barrier vs. electronegativity.PNG|Schottky barrier height ''vs.'' metal electronegativity for some selected metals on ''n''-type silicon. | | |Schottky barrier vs. electronegativity.PNG|Schottky barrier height ''vs.'' metal electronegativity for some selected metals on ''n''-type silicon. |
| |Schottky barrier on p-SiC.PNG|Theoretical dependence of Schottky barrier heights for diodes using ''p''-SiC ''vs.'' electronegativity of the metal according to Mönch | | |Schottky barrier on p-SiC.PNG|Theoretical dependence of Schottky barrier heights for diodes using ''p''-SiC ''vs.'' electronegativity of the metal according to Mönch |
| | |Three-phase CCD.PNG|Three phase CCD. ''Top'': illumination ''Bottom'': Charge transfer |
| }} | | }} |
Latest revision as of 03:07, 22 November 2023
The account of this former contributor was not re-activated after the server upgrade of March 2022.
Devices
Devices
|
|
(PD) Image: John R. Brews
|
Mesa diode structure (top) and planar diode structure with guard-ring (bottom).
|
|
(PD) Image: John R. Brews
|
|
|
(PD) Image: John R. Brews
|
Gummel plot and current gain for a GaAs/AlGaAs heterostructure bipolar transistor.
|
|
(PD) Image: John R. Brews
|
Quasi-Fermi levels and carrier densities in forward biased pn-diode.
|
|
(PD) Image: John R. Brews
|
Cross section of MOS capacitor showing charge layers
|
|
(PD) Image: John R. Brews
|
Three types of MOS capacitance vs. voltage curves. VTH = threshold, VFB = flatbands
|
|
(PD) Image: John R. Brews
|
Small-signal equivalent circuit of the MOS capacitor in inversion with a single trap level
|
|
(PD) Image: John R. Brews
|
A modern MOSFET
|
|
(PD) Image: John R. Brews
|
A power MOSFET; source and body share a contact.
|
|
(PD) Image: John R. Brews
|
Two bipolar transistor modes, showing extrapolation of asymptotes to the Early voltage.
|
|
(PD) Image: John R. Brews
|
Channel length modulation in 3/4μm technology.
|
|
(PD) Image: John R. Brews
|
Early voltage for MOSFETs from a 0.18μm process as a function of channel strength.
|
|
(CC) Image: John R. Brews
|
Calculated density of states for crystalline silicon.
|
|
(CC) Image: John R. Brews
|
Field effect: At a gate voltage above threshold a surface inversion layer of electrons forms at a semiconductor surface.
|
|
(PD) Image: John R. Brews
|
Occupancy comparison between n-type, intrinsic and p-type semiconductors.
|
|
(PD) Image: John R. Brews
|
Nonideal pn-diode current-voltage characteristics
|
|
(PD) Image: John R. Brews
|
Band-bending diagram for pn-junction diode at zero applied voltage
|
|
(PD) Image: John R. Brews
|
Band-bending for pn-diode in reverse bias
|
|
(PD) Image: John R. Brews
|
Quasi-Fermi levels in reverse-biased pn-junction diode
|
|
(PD) Image: John R. Brews
|
Band-bending diagram for pn-diode in forward bias
|
|
(PD) Image: John R. Brews
|
Fermi occupancy function vs. energy departure from Fermi level in volts for three temperatures
|
|
(PD) Image: John R. Brews
|
Fermi surface in k-space for a nearly filled band in the face-centered cubic lattice
|
|
(PD) Image: John R. Brews
|
Electron probabilities in lowest two quantum states of a 160Ǻ GaAs quantum well in a GaAs-GaAlAs quantum heterostructure.
|
|
More devices
More devices
|
|
(PD) Image: John R. Brews
|
A constant energy surface in the silicon conduction band consists of six ellipsoids.
|
|
(PD) Image: John R. Brews
|
Planar Schottky diode with n+-guard rings and tapered oxide.
|
|
(PD) Image: John R. Brews
|
Comparison of Schottky and pn-diode current voltage curves.
|
|
(PD) Image: John R. Brews
|
Schottky barrier formation on p-type semiconductor. Energies are in eV.
|
|
(PD) Image: John R. Brews
|
Schottky diode under forward bias VF.
|
|
(PD) Image: John R. Brews
|
Schottky diode under reverse bias VR.
|
|
(PD) Image: John R. Brews
|
Critical electric field for breakdown versus bandgap energy in several materials.
|
|
(PD) Image: John R. Brews
|
Schottky barrier height vs. metal electronegativity for some selected metals on n-type silicon.
|
|
(PD) Image: John R. Brews
|
Theoretical dependence of Schottky barrier heights for diodes using p-SiC vs. electronegativity of the metal according to Mönch
|
|
(PD) Image: John R. Brews
|
Three phase CCD. Top: illumination Bottom: Charge transfer
|
|