Patent classifications
H10D62/8325
SEMICONDUCTOR DEVICE AND MANUFACTURING METHOD THEREOF
A semiconductor device includes an isolation layer, first and second fin structures, a gate structure and a source/drain structure. The isolation layer is disposed over a substrate. The first and second fin structures are disposed over the substrate, and extend in a first direction in plan view. Upper portions of the first and second fin structures are exposed from the isolation layer. The gate structure is disposed over parts of the first and second fin structures, and extends in a second direction crossing the first direction. The source/drain structure is formed on the upper portions of the first and second fin structures, which are not covered by the first gate structure and exposed from the isolation layer, and wraps side surfaces and a top surface of each of the exposed first and second fin structures. A void is formed between the source/drain structure and the isolation layer.
MPS DIODE
There is provided an MPS diode comprising a first semiconductor layer that is an N type; P-type semiconductor regions and N-type semiconductor regions that are arranged alternately on one surface of the first semiconductor layer; and a Schottky electrode that is in Schottky junction with the N-type semiconductor regions and is arranged to be adjacent to and in contact with at least part of the P-type semiconductor regions. A donor concentration in an area of the N-type semiconductor region that is adjacent to and in contact with the first semiconductor layer is lower than the donor concentration in an area of the first semiconductor layer that is adjacent to and in contact with the N-type semiconductor region and is lower than the donor concentration in an area of the N-type semiconductor region that is adjacent to and in contact with the Schottky electrode. This configuration improves a breakdown voltage under applying a reverse bias voltage and reduces a rising voltage under applying a forward bias voltage.
Tunneling Field Effect Transistor
A tunneling field-effect transistor with an insulated planar gate adjacent to a heterojunction between wide-bandgap semiconductor, such as silicon carbide, and either a narrow band gap material or a high work function metal. The heterojunction may be formed by filling a recess on a silicon carbide planar substrate, for example by etched into an epitaxially grown drift region atop the planar substrate. The low band gap material may be silicon which is deposited heterogeneously and, optionally, annealed via laser treatment and/or doped. The high work function metal may be tungsten, platinum, titanium, nickel, tantalum, or gold, or an alloy containing such a metal. The plane of the gate may be lateral or vertical. A blocking region of opposite doping type from the drift prevents conduction from the filled recess to the drift other than the conduction though the heterojunction.
PLASMA-ENHANCED CHEMICAL VAPOR DEPOSITION METHODS FOR GRAPHENE DEPOSITION
A graphene deposition process. The process includes the steps of placing a substrate into a deposition chamber and heating the chamber, generating radio frequency plasma at a location proximate to the substrate while flowing a precursor gas containing carbon through the plasma and over the substrate.
INTEGRATED CIRCUIT DEVICE AND METHOD OF MANUFACTURING THE SAME
An integrated circuit (IC) device includes a pair of fin-shaped active areas that are adjacent to each other with a fin separation area therebetween, the pair of fin-shaped active areas extend in a line, and a fin separation insulating structure in the fin separation area, wherein the pair of fin-shaped active areas includes a first fin-shaped active area having a first corner defining part of the fin separation area, and wherein the fin separation insulating structure includes a lower insulating pattern that covers sidewalls of the pair of fin-shaped active areas, and an upper insulating pattern on the lower insulating pattern to cover at least part of the first corner, the upper insulating pattern having a top surface at a level higher than a top surface of each of the pair of fin-shaped active areas.
Bipolar junction transistor structure for reduced current crowding
The present disclosure relates to a bipolar junction transistor (BJT) structure that significantly reduces current crowding while improving the current gain relative to conventional BJTs. The BJT includes a collector, a base region, and an emitter. The base region is formed over the collector and includes at least one extrinsic base region and an intrinsic base region that extends above the at least one extrinsic base region to provide a mesa. The emitter is formed over the mesa. The BJT may be formed from various material systems, such as the silicon carbide (SiC) material system. In one embodiment, the emitter is formed over the mesa such that essentially none of the emitter is formed over the extrinsic base regions. Typically, but not necessarily, the intrinsic base region is directly laterally adjacent the at least one extrinsic base region.
Solid-state circuit breakers and related circuits
Various solid-state circuit breakers and related circuits are presented herein. These include, among other things, a common node bidirectional solid-state circuit breaker (BDSSCB) having diodes connected between terminals of its switches, a shunt voltage actuated driver (SVAD) circuit for use with a BDSSCB, a SVAD circuit for use with a unidirectional solid-state circuit breaker (UDSSCB), a bipolar current actuated driver (BCAD) for use with a BDSSCB, and a multi-directional solid-state circuit breaker (MDSSCB).
Semiconductor device with substantially equal impurity concentration JTE regions in a vicinity of a junction depth
A highly reliable semiconductor device with high withstand voltage is provided. As means therefor, an impurity concentration in a first JTE region is set to 4.410.sup.17 cm.sup.3 or higher and 610.sup.17 cm.sup.3 or lower and an impurity concentration in a second JTE region is set to 210.sup.17 cm.sup.3 or lower in a case of a Schottky diode, and an impurity concentration in the first JTE region is set to 610.sup.17 cm.sup.3 or higher and 810.sup.17 cm.sup.3 or lower and an impurity concentration in the second JTE region is set to 210.sup.17 cm.sup.3 or lower in a case of a junction barrier Schottky diode.
High efficiency FinFET diode
Disclosed are methods to form a FinFET diode of high efficiency, designed to resolve the degradation problem with a conventional FinFET diode arising from reduced active area, and a method of fabrication. The FinFET diode has a doped substrate, two spaced-apart groups of semiconductor fin structures, dielectric layers formed between the two groups and among the fin structures for insulation, a plurality of gate structures perpendicularly traversing both groups of the fin structures, and two groups of semiconductor strips respectively formed lengthwise upon the two groups of the fin structures. The two groups of semiconductor strips are doped to have opposite conductivity types, p-type and n-type. In an embodiment, the FinFET diode further has metal contacts formed upon the semiconductor strips. In another embodiment, the semiconductor strips may be integrally formed with the fin structures by epitaxial growth and in-situ doped.
Method for treating a semiconductor wafer
A Magnetic Czochralski semiconductor wafer having opposing first and second sides arranged distant from one another in a first vertical direction is treated by implanting first particles into the semiconductor wafer via the second side to form crystal defects in the semiconductor wafer. The crystal defects have a maximum defect concentration at a first depth. The semiconductor wafer is heated in a first thermal process to form radiation induced donors. Implantation energy and dose are chosen such that the semiconductor wafer has, after the first thermal process, an n-doped semiconductor region arranged between the second side and first depth, and the n-doped semiconductor region has, in the first vertical direction, a local maximum of a net doping concentration between the first depth and second side and a local minimum of the net doping concentration between the first depth and first maximum.