H10D62/815

DUAL WAVELENGTH HYBRID DEVICE

A Dual-wavelength hybrid (DWH) device includes an n-type ohmic contact layer, cathode and anode terminal electrodes, first and second injector terminal electrodes, p-type and n-type modulation doped QW structures, and first through sixth ion implant regions. The first injector terminal electrode is formed on the third ion implant region that contacts the p-type modulation doped QW structure and the second injector terminal electrode is formed on the fourth ion implant region that contacts the n-type modulation doped QW structure. The DWH device operates in at least one of a vertical cavity mode and a whispering gallery mode. In the vertical cavity mode, the DWH device converts an in-plane optical mode signal to a vertical optical mode signal, whereas in the whispering gallery mode the DWH device converts a vertical optical mode signal to an in-plane optical mode signal.

APPARATUS FOR ADJUSTING SPACING BETWEEN MOIRE SUPERLATTICES OF TWO-DIMENSIONAL MATERIALS

Disclosed is an apparatus for adjusting spacing between Moir superlattices of two-dimensional (2-D) materials. A heterostructure 2-D material includes a first insulator, a first 2-D material having one surface coming into contact with the first insulator, a second 2-D material having one surface coming into contact with the first 2-D material and forming a van der Waals layered bond, a second insulator having one surface coming into contact with the second 2-D material, and an electrode configured to come into contact with the other surface of the second insulator and rotated by electrostatic attraction from the outside.

Lateral gate material arrangements for quantum dot devices

Disclosed herein are lateral gate material arrangements for quantum dot devices, as well as related computing devices and methods. For example, in some embodiments, a quantum dot device may include: a quantum well stack; and a gate above the quantum well stack, wherein the gate includes a gate electrode, the gate electrode includes a first material proximate to side faces of the gate and a second material proximate to a center of the gate, and the first material has a different material composition than the second material.

Quantum structure getter for radiation hardened transistors

A microelectronic device that is radiation hardened through the incorporation of a quantum structure getter (QSG) is provided. The device, such as a field effect transistor (FET) includes a conductive channel and a material stack comprising: a capping layer, one or more barrier layers comprising a high band gap, one or more quantum structures comprising a small band gap, and a substrate. The quantum structures are positioned in close proximity to the conductive channel to form a quantum well charge getter. The getter forms a low energy area beneath the FET, which traps and confines electron-hole pair wave functions produced from ionizing radiation, causing the wave functions overlap, recombine, and produce light emission. The quantum structures getter the wave functions, which reduces the ionized photocurrent that reaches the conducting channel, thereby hardening the microelectronic device against ionizing radiation.

Method for making nanostructure transistors with source/drain trench contact liners
12230694 · 2025-02-18 · ·

A method for making a semiconductor device may include forming spaced apart gate stacks on a substrate with adjacent gate stacks defining a respective trench therebetween. Each gate stack may include alternating layers of first and second semiconductor materials, with the layers of the second semiconductor material defining nanostructures. The method may further include forming respective source/drain regions within the trenches, respective insulating regions adjacent lateral ends of the layers of the first semiconductor material, and respective conductive contact liners in the trenches.

Method for making nanostructure transistors with source/drain trench contact liners
12230694 · 2025-02-18 · ·

A method for making a semiconductor device may include forming spaced apart gate stacks on a substrate with adjacent gate stacks defining a respective trench therebetween. Each gate stack may include alternating layers of first and second semiconductor materials, with the layers of the second semiconductor material defining nanostructures. The method may further include forming respective source/drain regions within the trenches, respective insulating regions adjacent lateral ends of the layers of the first semiconductor material, and respective conductive contact liners in the trenches.

METHOD FOR MAKING NANOSTRUCTURE TRANSISTORS WITH FLUSH SOURCE/DRAIN DOPANT BLOCKING STRUCTURES INCLUDING A SUPERLATTICE
20250056824 · 2025-02-13 ·

A method for making a semiconductor device may include forming spaced apart gate stacks on a substrate defining respective trenches therebetween. Each gate stack may include alternating layers of first and second semiconductor materials, with the layers of the second semiconductor material defining nanostructures. The method may further include forming respective source/drain regions within the trenches, forming respective insulating regions adjacent lateral ends of the layers of the first semiconductor material, and forming respective dopant blocking superlattices adjacent lateral ends of the nanostructures and flush with adjacent surfaces of the insulating regions. Each dopant blocking superlattice may include stacked groups of layers, with each group of layers including a plurality of 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.

METHOD FOR MAKING NANOSTRUCTURE TRANSISTORS WITH OFFSET SOURCE/DRAIN DOPANT BLOCKING STRUCTURES INCLUDING A SUPERLATTICE
20250056825 · 2025-02-13 ·

A method for making semiconductor device may include forming spaced apart gate stacks on a substrate defining respective trenches therebetween. Each gate stack may include alternating layers of first and second semiconductor materials, with the layers of the second semiconductor material defining nanostructures. The method may further include forming respective source/drain regions within the trenches, forming respective insulating regions adjacent lateral ends of the layers of the first semiconductor material, and forming respective dopant blocking superlattices adjacent lateral ends of the nanostructures and offset outwardly from adjacent surfaces of the insulating regions. Each dopant blocking superlattice may include a plurality of stacked groups of layers, with each group of layers comprising 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.

High electron mobility transistor

An HEMT includes an aluminum gallium nitride layer. A gallium nitride layer is disposed below the aluminum gallium nitride layer. A zinc oxide layer is disposed under the gallium nitride layer. A source electrode and a drain electrode are disposed on the aluminum gallium nitride layer. A gate electrode is disposed on the aluminum gallium nitride layer and between the drain electrode and the source electrode.

Semiconductor material doping

A solution for designing and/or fabricating a structure including a quantum well and an adjacent barrier is provided. A target band discontinuity between the quantum well and the adjacent barrier is selected to coincide with an activation energy of a dopant for the quantum well and/or barrier. For example, a target valence band discontinuity can be selected such that a dopant energy level of a dopant in the adjacent barrier coincides with a valence energy band edge for the quantum well and/or a ground state energy for free carriers in a valence energy band for the quantum well. Additionally, a target doping level for the quantum well and/or adjacent barrier can be selected to facilitate a real space transfer of holes across the barrier. The quantum well and the adjacent barrier can be formed such that the actual band discontinuity and/or actual doping level(s) correspond to the relevant target(s).