Abstract:
A floating body germanium (Ge) phototransistor and associated fabrication process are presented. The method includes: providing a silicon (Si) substrate; selectively forming an insulator layer overlying the Si substrate; forming an epitaxial Ge layer overlying the insulator layer using a liquid phase epitaxy (LPE) process; forming a channel region in the Ge layer; forming a gate dielectric, gate electrode, and gate spacers overlying the channel region; and, forming source/drain regions in the Ge layer. The LPE process involves encapsulating the Ge with materials having a melting temperature greater than a first temperature, and melting the Ge using a temperature lower than the first temperature. The LPE process includes: forming a dielectric layer overlying deposited Ge; melting the Ge; and, in response to cooling the Ge, laterally propagating an epitaxial growth front into the Ge from an underlying Si substrate surface.
Abstract:
A method is disclosed for passivating and contacting a surface of a germanium substrate. A passivation layer of amorphous silicon material is formed on the germanium surface. A contact layer of metal, e.g., aluminum, is then formed on the passivation layer. The structure is heated so that the germanium surface makes contact with the contact layer. The aluminum contact layer can be configured for use as a mirroring surface for the back surface of the device. Thus, a passivated germanium surface is disclosed, as well as a solar cell comprising such a structure.
Abstract:
Thin semiconductor films of compounds from groups III-V of the periodic table suitable for solar cells are formed on low cost substrates by forming on the substrate an intermediate film that is chemically related to but has a lower melting point than the desired semiconductor. The desired semiconductor film is then grown on this intermediate film while it is in a molten condition. The molten intermediate layer isolates the substrate from the desired semiconductor layer so that as that layer grows, large area crystals result. The intermediate film may be a semiconductor III-V compound or may be a group III metal alloy.
Abstract:
The invention relates to a method for producing a desired thin semiconductor film for use in solar cells. The desired semiconductor is grown epitaxially on a second semiconductor film which may be epitaxial on a third semiconductor. The second semiconductor has a lower melting point than the desired semiconductor. The temperature of the second semiconductor is increased. This creates a molten state in the second semiconductor and the desired semiconductor is stripped away from the second semiconductor. The desired film may be detached by dissolving the second semiconductor with a chemical agent that dissolves the second semiconductor.
Abstract:
The present disclosure provides a semiconductor structure. The semiconductor structure includes a waveguide structure, a photoelectric material, and a transistor. The waveguide structure is disposed on a substrate and includes a first doping region having a first type of dopant and a second doping region having a second type of dopant different from the first type. The photoelectric material is disposed proximal to a junction of the first doping region and the second doping region. The transistor is disposed on the substrate at a level same as a level of the waveguide structure. A method of manufacturing the semiconductor structure is also provided.
Abstract:
A silicon nitride core is formed on a silicon core via a first silicon oxide layer, and a germanium pattern caused to selectively grow in an opening penetrating through a second silicon oxide layer formed on the silicon nitride core and the first silicon oxide layer is formed on a lower silicon pattern formed to be continuous with the silicon core, thereby constituting a Ge photodiode.
Abstract:
A photodiode structure including a silicon substrate, an oxide layer on the silicon substrate, a silicon on insulator region on the oxide layer, a germanium absorption region, a silicon nitride waveguide, a cathode region, and an anode region is provided. The germanium absorption region is at least partially disposed in a recess of the silicon on insulator region. The germanium absorption region includes a top surface having a first width and a bottom surface having a second width, the first width being greater than the second width. The cathode region is formed at a first side of the germanium absorption region, and the anode region is formed at a second side of the germanium absorption region that is opposite the first side.
Abstract:
Techniques for enhancing the absorption of photons in semiconductors with the use of microstructures are described. The microstructures, such as pillars and/or holes, effectively increase the effective absorption length resulting in a greater absorption of the photons. Using microstructures for absorption enhancement for silicon photodiodes and silicon avalanche photodiodes can result in bandwidths in excess of 10 Gb/s at photons with wavelengths of 850 nm, and with quantum efficiencies of approximately 90% or more.
Abstract:
There is provided a transparent semiconductor substrate and a method for manufacturing same includes a semiconductor substrate including a first surface and a second surface opposite to the first surface; and a through-hole penetrating the semiconductor substrate, wherein the through-hole includes an inclined portion inclined with respect to the first surface and second surface.
Abstract:
A semiconductor, such as crystallized silicon or germanium, features top-mounted ridges. Circuits are capable of being integrated onto the ridges using modified photolithographic processes. The ridged architecture increases the usable surface area per given footprint of semiconductors. Specifically, if the preferred embodiment is adopted, the ridges increase relative surface area by 41.42%. Such an increase in surface area has numerous advantages. One advantage is that microchip footprints can be 29.29% smaller, allowing 1.41 times more microchips to be produced per wafer. Another advantage is that solar panels can contain 1.41 times more electron-shuttling junctions, thereby increasing overall sunlight harnessing, electrical conversion, and panel efficiency by 41.42%.