Patent classifications
H01L29/882
Method for making a semiconductor device including a resonant tunneling diode structure having a superlattice
A method for making a semiconductor device may include forming at least one double-barrier resonant tunneling diode (DBRTD) by forming a first doped semiconductor layer, and forming a first barrier layer on the first doped semiconductor layer and including a superlattice. The superlattice may include stacked groups of layers, each group of layers including stacked base semiconductor monolayers defining a base semiconductor portion, and at least one non-semiconductor monolayer constrained within a crystal lattice of adjacent base semiconductor portions. The method may further include forming an intrinsic semiconductor layer on the first barrier layer, forming a second barrier layer on the intrinsic semiconductor layer, and forming a second doped semiconductor layer on the second superlattice layer.
SEMICONDUCTOR DEVICE AND METHOD OF MANUFACTURING THE SAME
Provided is a semiconductor device including a substrate, a diode, a channel layer, a barrier layer, a first dielectric layer, a source, a drain, and a gate. The diode is disposed over the substrate or in the substrate. The channel layer is disposed over the diode. The barrier layer is disposed over the channel layer. The first dielectric layer is disposed over the barrier layer. The source is electrically connected to a first region of the diode by a first conductive via through the first dielectric layer, the barrier layer, and the channel layer. The drain is electrically connected to a second region of the diode by a second conductive via through the first dielectric layer, the barrier layer, and the channel layer. The gate is disposed over the channel layer between the source and the drain.
Methods for using remote plasma chemical vapor deposition (RP-CVD) and sputtering deposition to grow layers in light emitting devices
Described herein are methods for using remote plasma chemical vapor deposition (RP-CVD) and sputtering deposition to grow layers for light emitting devices. A method includes growing a light emitting device structure on a growth substrate, and growing a tunnel junction on the light emitting device structure using at least one of RP-CVD and sputtering deposition. The tunnel junction includes a p++ layer in direct contact with a p-type region, where the p++ layer is grown by using at least one of RP-CVD and sputtering deposition. Another method for growing a device includes growing a p-type region over a growth substrate using at least one of RP-CVD and sputtering deposition, and growing further layers over the p-type region. Another method for growing a device includes growing a light emitting region and an n-type region using at least one of RP-CVD and sputtering deposition over a p-type region.
Graphene double-barrier resonant tunneling device
An apparatus comprising: a fermion source nanolayer (90); a first insulating nanolayer (92); a fermion transport nanolayer (94); a second insulating nanolayer (96); a fermion sink nanolayer (98); a first contact for applying a first voltage to the fermion source nanolayer; a second contact for applying a second voltage to the fermion sink nanolayer; and a transport contact for enabling an electric current via the fermion transport nanolayer. In a particular example, the apparatus comprises three graphene sheets (90, 94, 98) interleaved with two-dimensional Boron-Nitride (hBN) layers (92, 96).
GALLIUM NITRIDE CROSS-GAP LIGHT EMITTERS BASED ON UNIPOLAR-DOPED TUNNELING STRUCTURES
Gallium nitride based devices and, more particularly to the generation of holes in gallium nitride based devices lacking p-type doping, and their use in light emitting diodes and lasers, both edge emitting and vertical emitting. By tailoring the intrinsic design, a wide range of wavelengths can be emitted from near-infrared to mid ultraviolet, depending upon the design of the adjacent cross-gap recombination zone. The innovation also provides for novel circuits and unique applications, particularly for water sterilization.
Semiconductor device including a resonant tunneling diode structure with electron mean free path control layers
A semiconductor device including at least one double-barrier resonant tunneling diode (DBRTD) is provided. The at least one DBRTD may include a first doped semiconductor layer, and a first barrier layer on the first doped semiconductor layer and including a superlattice. The DBRTD may further include a first intrinsic semiconductor layer on the first barrier layer, a second barrier layer on the first intrinsic semiconductor layer and also including the superlattice, a second intrinsic semiconductor layer on the second barrier layer, a third barrier layer on the second intrinsic semiconductor layer and also including the superlattice. A third intrinsic semiconductor layer may be on the third barrier layer, a fourth barrier layer may be on the third intrinsic semiconductor layer and also including the superlattice, a second doped semiconductor layer on the fourth barrier layer.
Method for making a semiconductor device including a resonant tunneling diode with electron mean free path control layers
A method for making a semiconductor device may include forming at least one a double-barrier resonant tunneling diode (DBRTD) by forming a first doped semiconductor layer, and a forming first barrier layer on the first doped semiconductor layer and including a superlattice. The method may further include forming a first intrinsic semiconductor layer on the first barrier layer, forming a second barrier layer on the first intrinsic semiconductor layer and also comprising the superlattice, forming a second intrinsic semiconductor layer on the second barrier layer, and forming a third barrier layer on the second intrinsic semiconductor layer and also comprising the superlattice. The method may further include forming a third intrinsic semiconductor layer on the third barrier layer, forming a fourth barrier layer on the third intrinsic semiconductor layer, and forming a second doped semiconductor layer on the fourth barrier layer.
ENERGY-FILTERED COLD ELECTRON DEVICES AND METHODS
Energy-filtered cold electron devices use electron energy filtering through discrete energy levels of quantum wells or quantum dots that are formed through band bending of tunneling barrier conduction band. These devices can obtain low effective electron temperatures of less than or equal to 45K at room temperature, steep electrical current turn-on/turn-off capabilities with a steepness of less than or equal to 10 mV/decade at room temperature, subthreshold swings of less than or equal to 10 mV/decade at room temperature, and/or supply voltages of less than or equal to 0.1 V.
ULTRAVIOLET LIGHT EMITTING DIODE WITH TUNNEL JUNCTION
A light emitting diode (LED) to emit ultraviolet (UV) light includes a first n-type semiconductor region and a first p-type semiconductor region. The LED also includes an active region disposed between the first n-type semiconductor region and the first p-type semiconductor region, and in response to a bias applied across the light emitting diode, the active region emits UV light. A tunnel junction is disposed in the LED so the first p-type semiconductor region is disposed between the active region and the tunnel junction. The tunnel junction is electrically coupled to inject charge carriers into the active region through the first p-type semiconductor region. A second n-type semiconductor region is also disposed in the LED so the tunnel junction is disposed between the second n-type semiconductor region and the first p-type semiconductor region.
Energy-filtered cold electron devices and methods
Energy-filtered cold electron devices use electron energy filtering through discrete energy levels of quantum wells or quantum dots that are formed through band bending of tunneling barrier conduction band. These devices can obtain low effective electron temperatures of less than or equal to 45K at room temperature, steep electrical current turn-on/turn-off capabilities with a steepness of less than or equal to 10 mV/decade at room temperature, subthreshold swings of less than or equal to 10 mV/decade at room temperature, and/or supply voltages of less than or equal to 0.1 V.