A photosensor device includes a substrate, a graphene layer provided on the substrate, a pair of electrodes electrically connected to the graphene layer, and a passivation layer formed of a resin and configured to cover the graphene layer. The graphene layer has holes which are periodically arranged, and the passivation layer is provided with openings that communicate with the holes. The side surfaces of the holes and the inner walls of the openings are continuously covered with an insulating thin film.

An opto-electronic device includes a base portion, a first electrode and a second electrode formed on an upper surface of the base portion apart from each other, a quantum dot layer, and a bank structure. The quantum dot layer is between the first electrode and the second electrode on the base portion and includes a plurality of quantum dots. The bank structure covers at least partial regions of the first electrode and the second electrode, defines a region where the quantum dot layer is formed, and is formed of an inorganic material.

Germanium-based sensors are disclosed herein. An exemplary germanium-based sensor includes a germanium photodiode and a junction field effect transistor (JFET) formed from a germanium layer disposed in a silicon substrate, in some embodiments, or on a silicon substrate, in some embodiments. A doped silicon layer, which can be formed by in-situ doping epitaxially grown silicon, is disposed between the germanium layer and the silicon substrate. In embodiments where the germanium layer on the silicon substrate, the doped silicon layer is disposed between the germanium layer and an oxide layer. The JFET has a doped polysilicon gate, and in some embodiments, a gate diffusion region is disposed in the germanium layer under the doped polysilicon gate. In some embodiments, a pinned photodiode passivation layer is disposed in the germanium layer. In some embodiments, a pair doped region pair in the germanium layer is configured as an e-lens of the germanium-based sensor.

A photodetector includes a metal layer that shields incident light and generates surface plasmon polaritons (SPPs), a light absorbing layer that absorbs the generated SPPs and allows charges excited by the absorbed SPPs and a localized electric field effect to tunnel, a dielectric formed at nanoholes in which at least a part of the metal layer is opened, and a semiconductor layer that induces the photocurrent based on an electric field effect of tunneled electrons. The SPPs form localized surface plasmons (LSPs) at an interface where the metal layer meets the dielectric.

A photodetector which comprises a measurement layer (15) and at least a first photoactive layer (11) which covers the measurement layer (15). The measurement layer (15) may be a transistor channel or a charge accumulation electrode. The conductivity type of the measurement layer is n-type, p-type or ambipolar and the first photoactive layer (11) exhibits intrinsic semiconductivity.

An inexpensive IR photodetector assembly that can provide high performance in SWIR applications, such as LIDAR. The photodetector assembly can operate as a photodiode, a phototransistor, or can include both a photodiode and a phototransistor. The hybrid photodetector can be composed of one or more absorber layer materials from a first semiconductor family, e.g., p-type InGaAs, laying on one or more wide-band gap semiconductor transducer layer materials from a second semiconductor family, e.g., aluminum gallium nitride (AlGaN) and gallium nitride (GaN), or AlGaN/n-GaN. As such, the absorber layer material and the wide band gap materials can be from two different semiconductor families, making the IR photodetector a hybrid of semiconductor families. After shining IR light onto the absorber layer material, the photo-generated electron-hole pairs can be collected as photocurrent in the photo-voltaic mode.

Techniques to use energy band gap engineering (or band offset engineering) to produce a photodetector semiconductor assembly that can be tuned to absorb light in one or more wavelengths. For example, the assembly can be tuned to receive infrared (IR) and/or ultraviolet (UV) light. The photodetector assembly can operate as a photodiode, a phototransistor, or can include both a photodiode and a phototransistor.

The present disclosure provides a semiconductor heterojunction. The semiconductor heterojunction includes a bottom semiconductor, a top semiconductor and an electrode substrate. An upper surface of the bottom semiconductor includes a first facet. A lower surface of the top semiconductor includes a second facet, and the lower surface of the top semiconductor is contacted with the upper surface of the bottom semiconductor. The electrode substrate is disposed below the bottom semiconductor.

A plasmonic field-enhanced photodetector is disclosed. The photodetector absorbs surface plasmon polaritons (SPPs) by using a light absorbing layer having a conduction band and a valence band in which an energy is split, the SPPs being generated by combining surface plasmons (SPs) with photons of a light wave, and generates photocurrent based on the absorbed SPPs.

A terahertz detector circuit can include a high electron mobility transistor (HEMT) having multiple gates that can be controlled by gate signals to generate a gate-induced modulation pattern in a two-dimensional electron gas (2DEG) of the HEMT. When the gate induced modulation pattern substantially matches a signal induced modulation pattern generated by an incident terahertz signal then a detection efficiency of the incident terahertz signal is improved. Accordingly, an electronically tunable THz detector with high efficiency can be realized. When these THz detectors are arranged in an array and electrically coupled, THz images and/or multi-spectral THz images may be generated.