H10D62/165

ENERGY-FILTERED COLD ELECTRON DEVICES AND METHODS
20170338331 · 2017-11-23 ·

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.

Systems and methods for filtering and computation using tunneling transistors

An electrical circuit is disclosed that comprises plurality of tunneling field-effect transistors (TFETs) arranged in a diffusion network matrix having a plurality of nodes wherein, for each of the TFETs that is not on an end of the matrix, a drain of the TFET is electrically coupled with the source of at least one of the other TFETs at a node of the matrix and a source of the TFET is electrically coupled with the drain of at least one of the other TFETs at another node of the matrix. The electrical circuit further comprises a plurality of capacitors, wherein a respective one of the plurality of capacitors is electrically coupled with each node that includes the source of at least one TFET and the drain of at least one TFET. The TFETs may be symmetrical graphene-insulator-graphene field-effect transistors (SymFETs), for example.

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.

JUNCTION INTERLAYER DIELECTRIC FOR REDUCING LEAKAGE CURRENT IN SEMICONDUCTOR DEVICES

A semiconductor device includes a substrate and a p-doped layer including a doped III-V material on the substrate. A dielectric interlayer is formed on the p-doped layer. An n-type layer is formed on the dielectric interlayer, the n-type layer including a high band gap II-VI material to form an electronic device.

SEMICONDUCTOR DEVICE CONTACTS

Techniques are disclosed for forming contacts in silicon semiconductor devices. In some embodiments, a transition layer forms a non-reactive interface with the silicon semiconductor contact surface. In some such cases, a conductive material provides the contacts and the material forming a non-reactive interface with the silicon surface. In other cases, a thin semiconducting or insulating layer provides the non-reactive interface with the silicon surface and is coupled to conductive material of the contacts. The techniques can be embodied, for instance, in planar or non-planar (e.g., double-gate and tri-gate FinFETs) transistor devices.

SBFET TRANSISTOR AND CORRESPONDING FABRICATION PROCESS

A process for manufacturing a Schottky barrier field-effect transistor is provided. The process includes: providing a structure including a control gate and a semiconductive layer positioned under the gate and having protrusions that protrude laterally with respect to the gate; anisotropically etching at least one of the protrusions by using the control gate as a mask, so as to form a recess in this protrusion, this recess defining a lateral face of the semiconductive layer; depositing a layer of insulator on the lateral face of the semiconductive layer; and depositing a metal in the recess on the layer of insulator so as to form a contact of metal/insulator/semiconductor type between the deposit of metal and the lateral face of the semiconductive layer.

EPITAXIAL OXIDE MATERIALS, STRUCTURES, AND DEVICES
20250056927 · 2025-02-13 · ·

A transistor can include a substrate, an epitaxial oxide layer on the substrate, and a gate layer. The substrate can include a first crystalline material. The epitaxial oxide layer can include a second oxide material including: Li and one of Ni, Al, Ga, Mg, Zn and Ge; or Ni and one of Li, Al, Ga, Mg, Zn and Ge; or Mg and one of Ni, Al, Ga, and Ge; or Zn and one of Ni, Al, Ga, and Ge. The gate layer can include a third oxide material. A bandgap of the third oxide material of the gate can be wider than a bandgap of the second oxide material of the epitaxial oxide layer. The transistor can also include a source electrical contact coupled to the epitaxial oxide layer, a drain electrical contact coupled to the epitaxial oxide layer, and a first gate electrical contact coupled to the gate layer.

Junction interlayer dielectric for reducing leakage current in semiconductor devices

A semiconductor device includes a substrate and a p-doped layer including a doped III-V material on the substrate. A dielectric interlayer is formed on the p-doped layer. An n-type layer is formed on the dielectric interlayer, the n-type layer including a high band gap II-VI material to form an electronic device.

Semiconductor device, method for manufacturing same, and nonvolatile semiconductor memory device

Provided is a semiconductor element having, while maintaining the same integratability as a conventional MOSFET, excellent switch characteristics compared with the MOSFET, that is, having the S-value less than 60 mV/order at room temperature. Combining the MOSFET and a tunnel bipolar transistor having a tunnel junction configures a semiconductor element that shows an abrupt change in the drain current with respect to a change in the gate voltage (an S-value of less than 60 mV/order) even at a low voltage.

INSULATED GATE FIELD EFFECT TRANSISTOR HAVING PASSIVATED SCHOTTKY BARRIERS TO THE CHANNEL
20170133476 · 2017-05-11 ·

A transistor having at least one passivated Schottky barrier to a channel includes an insulated gate structure on a p-type substrate in which the channel is located beneath the insulated gate structure. The channel and the insulated gate structure define a first and second undercut void regions that extend underneath the insulated gate structure toward the channel from a first and a second side of the insulated gate structure, respectively. A passivation layer is included on at least one exposed sidewall surface of the channel and metal source and drain terminals are located on respective first and second sides of the channel, including on the passivation layer and within the undercut void regions beneath the insulated gate structure. At least one of the metal source and drain terminals comprises a metal that has a work function near a valence band of the p-type substrate.