Abstract: Methods for forming a buried p-n junction and avalanche photodiodes incorporating same are disclosed. The method includes forming a well in a semiconductor layer, wherein a depth of the well is selected as a function of the desired shape of the p-n junction in the edge region of the avalanche photodiode. A diffusion mask is then formed on the semiconductor layer, wherein the diffusion mask includes at least two openings per APD formed, wherein one opening is a diffusion window and the other is a diffusion sink. The depth of the p-n junction in the active region of the APD is based, in part, on an attribute of the diffusion mask relating to the diffusion sink.

Abstract: A single photon avalanche diode for use in a CMOS integrated circuit includes a deep n-well region formed above a p-type substrate and an n-well region formed above and in contact with the deep n-well region. A cathode contact is connected to the n-well region via a heavily doped n-type implant. A lightly doped region forms a guard ring around the n-well and deep n-well regions. A p-well region is adjacent to the lightly doped region. An anode contact is connected to the p-well region via a heavily doped p-type implant. The junction between the bottom of the deep n-well region and the substrate forms a multiplication region when an appropriate bias voltage is applied between the anode and cathode and the guard ring breakdown voltage is controlled with appropriate control of the lateral doping concentration gradient such that the breakdown voltage is higher than that of the multiplication region.

Abstract: A photodiode array has a plurality of photodetector channels formed on an n-type substrate having an n-type semiconductor layer, with a light to be detected being incident to the photodetector channels. The array comprises: a p?-type semiconductor layer on the n-type semiconductor layer of the substrate; resistors is provided to each of the photodetector channels and is connected to a signal conductor at one end thereof; and an n-type separating part between the plurality of photodetector channels. The p?-type semiconductor layer forms a pn junction at the interface between the substrate, and comprises a plurality of multiplication regions for avalanche multiplication of carriers produced by the incidence of the light to be detected so that each of the multiplication regions corresponds to each of the photodetector channels.

Abstract: Provided are a silicon photomultiplier and method for fabricating silicon photomultiplier. The silicon photomultiplier includes a first conductive type semiconductor layer; a first conductive type buried layer disposed in a lower portion of the first conductive type semiconductor layer, and having a higher impurity concentration than the first conductive type semiconductor layer; quench resistors spaced from each other and disposed on the first conductive type semiconductor layer; a transparent insulator formed on the first conductive type semiconductor layer, and exposing the quench resistors; second conductive type doped layers disposed under the quench resistors to contact the first conductive type semiconductor layer; and a transparent electrode commonly connected to the quench resistors electrically.

Abstract: An APD is provided with the semi-insulating substrate, a first mesa having a first laminate constitution in which a p-type electrode layer, a p-type light absorbing layer, a light absorbing layer with a low impurity concentration, a band gap inclined layer, a p-type electric field control layer, an avalanche multiplier layer, an n-type electric field control layer, and an electron transit layer with a low impurity concentration are stacked in this order on a surface of the semi-insulating substrate, a second mesa having an outer circumference provided inside an outer circumference of the first mesa as viewed from the laminating direction and having a second laminate constitution in which an n-type electrode buffer layer and an n-type electrode layer are stacked in this order on a surface on the electron transit layer side, and a depletion control region that is provided in layers on the second mesa side relative to the p-type electric field control layer, formed in an encircling portion provided inside an out

Abstract: An embodiment of an array of Geiger-mode avalanche photodiodes, wherein each photodiode is formed by a body of semiconductor material, having a first conductivity type, housing a first cathode region, of the second conductivity type, and facing a surface of the body, an anode region, having the first conductivity type and a higher doping level than the body, extending inside the body, and facing the surface laterally to the first cathode region and at a distance therefrom, and an insulation region extending through the body and insulating an active area from the rest of the body, the active area housing the first cathode region and the anode region. The insulation region is formed by a mirror region of metal material, a channel-stopper region having the second conductivity type, surrounding the mirror region, and a coating region, of dielectric material, arranged between the mirror region and the channel-stopper region.

Abstract: An APD is provided with a semi-insulating substrate, a first mesa having a first laminate constitution in which a p-type electrode layer, a p-type light absorbing layer, a light absorbing layer with a low impurity concentration, a band gap inclined layer, a p-type electric field control layer, an avalanche multiplier layer, an n-type electric field control layer, and an electron transit layer with a low impurity concentration are stacked in this order on a surface of the semi-insulating substrate, a second mesa having an outer circumference provided inside an outer circumference of the first mesa as viewed from the laminating direction and having a second laminate constitution in which an n-type electrode buffer layer and an n-type electrode layer are stacked in this order on a surface on the electron transit layer side of the first mesa, and in the APD, a total donor concentration of the n-type electric field control layer is lower than a total acceptor concentration of the p-type electric field control laye

Abstract: A single-photon avalanche diode assembly, the diode including a central terminal and a peripheral terminal, the peripheral terminal being connected to an input of a comparator and to a first power supply terminal by a first resistor, the central terminal being connected by a conductive track to a second power supply terminal, a second resistor being arranged in series on said conductive track.

Abstract: A system and method providing for the detection of an input signal, either optical or electrical, by using a single independent discrete amplifier or by distributing the input signal into independent signal components that are independently amplified. The input signal can either be the result of photoabsorption process in the wavelengths greater than 950 nm or a low-level electrical signal. The discrete amplifier is an avalanche amplifier operable in a non-gated mode while biased in or above the breakdown region, and includes a composite dielectric feedback layer monolithically integrated with input signal detection and amplification semiconductor layers.

Abstract: Silicon photomultiplier and readout method A silicon photomultiplier device is provided which comprises a first electrode arranged to provide a bias voltage to the device, a second electrode arranged as a ground electrode for the device, and a third electrode arranged to provide an output signal from the device using the second electrode as the output signal ground.

Abstract: A semiconductor device that may include an avalanche photodiode (APD), the APD may include: a first doped region of a first polarity; a buried guard ring of a second polarity, the second polarity is opposite to the first polarity, the buried guard ring is spaced apart from the first doped region and is positioned below the first doped region; a well of the second polarity, wherein the well interfaces the first doped region to form a p-n junction; and a second doped region of the second polarity, the second doped region is spaced apart from the first doped region.

Abstract: The present invention provides a semiconductor device including a semiconductor substrate having a first conductive type, at least one high-side transistor device and at least one low-side transistor device. The high-side transistor device includes a doped high-side base region having a second conductive type, a doped high-side source region having the first conductive type and a doped drain region having the first conductive type. The doped high-side base region is disposed within the semiconductor substrate, and the doped high-side source region and the doped drain region are disposed within the doped high-side base region. The doped high-side source region is electrically connected to the semiconductor substrate, and the semiconductor substrate is regarded as a drain of the low-side transistor device.

Abstract: A semiconductor photodetector may provide charge carrier avalanche multiplication at high field regions of a semiconductor material layer. A semiconductor current amplifier may provide current amplification by impact ionization near a high field region. A plurality of metal electrodes are formed on a surface of a semiconductor material layer and electrically biased to produce a non-uniform high electric field in which the high electric field strength accelerates avalanche electron-hole pair generation, which is employed as an effective avalanche multiplication photodetection mechanism or as an avalanche impact ionization current amplification mechanism.

Abstract: Provided are a photomultiplier and a manufacturing method thereof. The manufacturing method thereof may include forming a mask layer on an active region of a substrate doped with a first conductive type, ion implanting a second conductive type impurity opposite to the first conductive type into the substrate to form a first doped region in the active region under the mask layer and an non-active region exposed from the mask layer, forming a device isolation layer on the non-active region, removing the mask layer, and ion implanting the second conductive type impurity having a concentration higher than that of the first doped region into an upper portion of the first doped region in the active region to form a second doped region shallower than the first doped region.

Abstract: Photonic power switch and method of controlling current flow in the photonic power switch, the photonic power switch comprising an avalanche photo diode installed on a switch element, the switch element comprising a carrier donor layer and a channel layer. Photons are injected in the avalanche photo diode for generating electrical charge carriers by photoeffect, and the generated charge carriers are accelerated the by an electric field so as to produce an avalanche effect and are injected from the avalanche photo diode into the carrier donor layer of the switch element. A conduction layer built between the donor layer and the channel layer of the switch element is modulated, thereby modulating a current flow between a drain and a source of the power switch through said conduction layer.

Abstract: An avalanche photodiode (APD) has a first semiconductor substrate having a first doping type. A first semiconductor layer is on top of the first semiconductor substrate. The first semiconductor layer is doped with the first doping type. A second epitaxial layer is on top of the first semiconductor layer. The second epitaxial layer is in-situ doped with the first doping type at a concentration higher than a concentration of the first doping type in the first semiconductor layer. A third epitaxial layer is on top of the second epitaxial layer. The third epitaxial layer is in-situ doped with a second doping type. The doping of the third epitaxial region forms a first p-n junction with the doping of the second epitaxial layer, wherein a carrier multiplication region includes the first p-n junction, and wherein the third epitaxial layer forms an absorption region for photons. A first implanted region is within the third epitaxial layer. The implanted region is doped with the second doping type.

Abstract: A layout structure of a semiconductor integrated circuit is provided with which narrowing and breaking of metal interconnects near a cell boundary can be prevented without increasing the data amount and processing time for OPC. A cell A and a cell B are adjacent to each other along a cell boundary. The interconnect regions of metal interconnects from which to the cell boundary no other interconnect region exists are placed to be substantially axisymmetric with respect to the cell boundary, while sides of diffusion regions facing the cell boundary are asymmetric with respect to the cell boundary.

Abstract: A spectrometer including: a photodiode having a depleted region and generating an electrical detection signal indicating instants of detection of optical pulses; a converter generating an electrical delay signal, indicating delays between the instants of detection and corresponding instants of emission of the optical pulses; a memory, storing a theoretical function corresponding to the probability of triggering an avalanche by a charge carrier generated in the depleted region; and a computing stage which determines a statistical distribution of the delays between the instants of detection and the corresponding instants of emission; selects a Gaussian portion of the statistical distribution; calculates the ratio between the sum of the number of delays of the Gaussian portion and the sum of the number of delays of the statistical distribution; and determines an estimate of the wavelength of the optical pulses on the basis of the theoretical function and of the sample value.

Abstract: An avalanche photodiode (APD) has a first semiconductor substrate having a first doping type. A first semiconductor layer is on top of the first semiconductor substrate. The first semiconductor layer is doped with the first doping type. A second epitaxial layer is on top of the first semiconductor layer. The second epitaxial layer is in-situ doped with the first doping type at a concentration higher than a concentration of the first doping type in the first semiconductor layer. A third epitaxial layer is on top of the second epitaxial layer. The third epitaxial layer is in-situ doped with a second doping type. The doping of the third epitaxial region forms a first p-n junction with the doping of the second epitaxial layer, wherein a carrier multiplication region includes the first p-n junction, and wherein the third epitaxial layer forms an absorption region for photons. A first implanted region is within the third epitaxial layer. The implanted region is doped with the second doping type.

Abstract: A reverse bias voltage is applied to a photodiode array provided with a plurality of avalanche photodiodes operated in Geiger mode and with quenching resistors connected in series to the respective avalanche photodiodes. Electric current is measured with change of the reverse bias voltage applied, and the reverse bias voltage at an inflection point in change of electric current measured is determined as a reference voltage. A voltage obtained by adding a predetermined value to the determined reference voltage is determined as a recommended operating voltage.

Abstract: A solid-state imaging device includes: an avalanche photodiode having a structure including an n+ region, a p+ region, and an avalanche region interposed between the n+ region and the p+ region, all of which are formed to extend in a thickness direction of a semiconductor base; and a pixel repeatedly having the structure of the avalanche photodiode.

Abstract: The present invention enables the detection of light using an APD that has high gain and/or a wide range of operating temperature. A first APD is biased with a voltage bias that is controlled based on the breakdown voltage of a second APD, which is thermally coupled with the first APD. Changes in the breakdown voltage of the second APD due to aging, temperature chances, and the like, are reflective of changes in the breakdown voltage of the first APD. As a result, the first APD can be operated with greater stability and reliability at high gain and over larger temperature excursions than APDs known in the prior art.

Abstract: Avalanche photodiodes having special lateral doping concentration that reduces dark current without causing any loss of optical signals and method for the fabrication thereof are described. In one aspect, an avalanche photodiode comprises: a substrate, a first contact layer coupled to at least one metal contract of a first electrical polarity, an absorption layer, a doped electric control layer having a central region and a circumferential region surrounding the central region, a multiplication layer having a partially doped central region, and a second contract layer coupled to at least one metal contract of a second electrical polarity. Doping concentration in the central section is lower than that of the circumferential region. The absorption layer can be formed by selective epitaxial growth.

Abstract: A semiconductor waveguide based optical receiver is disclosed. An apparatus according to aspects of the present invention includes an absorption region including a first type of semiconductor region proximate to a second type of semiconductor region. The first type of semiconductor is to absorb light in a first range of wavelengths and the second type of semiconductor to absorb light in a second range of wavelengths. A multiplication region is defined proximate to and separate from the absorption region. The multiplication region includes an intrinsic semiconductor region in which there is an electric field to multiply the electrons created in the absorption region.

Abstract: An in situ approach toward connecting and electrically contacting vertically aligned nanowire arrays using conductive nanoparticles is provided. The utility of the approach is demonstrated by development of a gas sensing device employing the nanowire assembly. Well-aligned, single-crystalline zinc oxide nanowires were grown through a direct thermal evaporation process at 550° C. on gold catalyst layers. Electrical contact to the top of the nanowire array was established by creating a contiguous nanoparticle film through electrostatic attachment of conductive gold nanoparticles exclusively onto the tips of nanowires. A gas sensing device was constructed using such an arrangement and the nanowire assembly was found to be sensitive to both reducing (methanol) and oxidizing (nitrous oxides) gases. This assembly approach is amenable to any nanowire array for which a top contact electrode is needed.

Abstract: An avalanche photodiode including a semiconductor substrate of a first conductivity type, an avalanche multiplication layer, an electric field control layer, a light absorption layer, and a window layer wherein the layers are laid one on another in this order on a major surface of the semiconductor substrate, an impurity region of a second conductivity type in a portion of the window layer, and a straight electrode on the impurity region and connected to the impurity region, the straight electrode being straight as viewed in a plan view facing the major surface of the semiconductor substrate.

Abstract: An electro-optic device is provided. The electro-optic device includes a junction layer disposed between a first conductivity type semiconductor layer and a second conductivity type semiconductor layer to which a reverse vias voltage is applied. The first conductivity type semiconductor layer and the second conductivity type semiconductor layer have an about 2 to 4-time doping concentration difference therebetween, thus making it possible to provide the electro-optic device optimized for high speed, low power consumption and high integration.

Abstract: A single-photon avalanche detector is disclosed that is operable at wavelengths greater than 1000 nm and at operating speeds greater than 10 MHz. The single-photon avalanche detector comprises a thin-film resistor and avalanche photodiode that are monolithically integrated such that little or no additional capacitance is associated with the addition of the resistor.

Abstract: The photo detector array is configured to generate pulses with short rise and fall times because each Geiger mode avalanche photodiode includes an anode contact, a cathode contact, an output contact electrically insulated from the anode and cathode contacts, a semiconductor layer, and at least one shield or metal structure in the semiconductor layer capacitively coupled to the semiconductor layer and coupled to the output contact. The output contacts of all Geiger mode avalanche photodiodes are connected in common and are configured to provide for detection of spikes correlated to avalanche events on any avalanche photodiode of the array.

Abstract: Techniques and apparatus for using single photon avalanche diode (SPAD) devices in various applications.

Abstract: Semiconductor photodetectors are provided that may enable optimized usage of an active detector array. The semiconductor photodetectors may have a structure that can be produced and/or configured as simply as possible. A radiation detector system is also provided.

Abstract: Avalanche amplification structures including electrodes, an avalanche region, a quantifier, an integrator, a governor, and a substrate arranged to detect a weak signal composed of as few as several electrons are presented. Quantifier regulates the avalanche process. Integrator accumulates a signal charge. Governor drains the integrator and controls the quantifier. Avalanche amplifying structures include: normal quantifier, reverse bias designs; normal quantifier, normal bias designs; lateral quantifier, normal bias designs; changeable quantifier, normal bias, adjusting electrode designs; normal quantifier, normal bias, adjusting electrode designs; and lateral quantifier, normal bias, annular integrator designs. Avalanche amplification structures are likewise arranged to provide arrays of multi-channel devices. The described invention is expected to be used within photodetectors, electron amplifiers, chemical and biological sensors, and chemical and biological chips with lab-on-a-chip applications.

Abstract: A photodetector/imaging device comprises a layer of photoconductive material converting incident electromagnetic radiation into electrical charges, the layer of photoconductive material being capable of avalanche multiplication when an electric field of sufficient magnitude is applied thereacross; a readout layer detecting the electrical charge; and at least one interface layer between the layer of photoconductive material and the readout layer, the interface layer coupling electrical charge to or from the layer of photoconductive material and being configured to inhibit uncontrolled rises in current in the photoconductive material during avalanche multiplication.

Abstract: A semiconductor photodetector may provide charge carrier avalanche multiplication at high field regions of a semiconductor material layer. A semiconductor current amplifier may provide current amplification by impact ionization near a high field region. A plurality of metal electrodes are formed on a surface of a semiconductor material layer and electrically biased to produce a non-uniform high electric field in which the high electric field strength accelerates avalanche electron-hole pair generation, which is employed as an effective avalanche multiplication photodetection mechanism or as an avalanche impact ionization current amplification mechanism.

Abstract: Quantum avalanche photodiodes are disclosed. An avalanche photodiode in accordance with one or more embodiments of the present invention comprises an absorption region having a first dopant type, a collection region, having a second dopant type, and a multiplication region, coupled between the absorption region and the collection region, wherein a distance of the multiplication region between the absorption region and the collection region is a plurality of avalanche lengths.

Abstract: A semiconductor photodetector may provide charge carrier avalanche multiplication at high field regions of a semiconductor material layer. A semiconductor current amplifier may provide current amplification by impact ionization near a high field region. A plurality of metal electrodes are formed on a surface of a semiconductor material layer and electrically biased to produce a non-uniform high electric field in which the high electric field strength accelerates avalanche electron-hole pair generation, which is employed as an effective avalanche multiplication photodetection mechanism or as an avalanche impact ionization current amplification mechanism.

Abstract: A gate electrode structure of a transistor may be formed so as to exhibit a high crystalline quality at the interface formed with a gate dielectric material, while upper portions of the gate electrode may have an inferior crystalline quality. In a later manufacturing stage after implementing one or more strain-inducing mechanisms, the gate electrode may be re-crystallized, thereby providing increased stress transfer efficiency, which in turn results in an enhanced transistor performance.

Abstract: A semiconductor device is disclosed. The semiconductor device comprises, a first region of a first conductivity type, a second region of a second conductivity type disposed adjacent to the first region to form a p-n junction structure, a resistance modification region of the second conductivity type, and a field response modification region of the second conductivity type disposed between the resistance modification region and the second region, wherein the field response modification region comprises a varying dopant concentration distribution along a thickness direction of the field response modification region.

Abstract: Provided are a silicon photomultiplier and method for fabricating silicon photomultiplier. The silicon photomultiplier includes a first conductive type semiconductor layer; a first conductive type buried layer disposed in a lower portion of the first conductive type semiconductor layer, and having a higher impurity concentration than the first conductive type semiconductor layer; quench resistors spaced from each other and disposed on the first conductive type semiconductor layer; a transparent insulator formed on the first conductive type semiconductor layer, and exposing the quench resistors; second conductive type doped layers disposed under the quench resistors to contact the first conductive type semiconductor layer; and a transparent electrode commonly connected to the quench resistors electrically.

Abstract: An imaging sensor having sensitivity at the single-photon level is disclosed. The sensor comprises an array of pixels, each of which comprises a negative-feedback avalanche diode and a read-out circuit that includes a counter. The counter keeps track of the number of photons detected by the diode during a given time period.

Abstract: An embodiment of a photomultiplier device is formed by a base substrate of insulating organic material forming a plurality of conductive paths and carrying a plurality of chips of semiconductor material. Each chip integrates a plurality of photon detecting elements, such as Geiger-mode avalanche diodes, and is bonded on a first side of the base substrate. Couplings for photon-counting and image-reconstruction units are formed on a second side of the base substrate. The first side of the base substrate is covered with a transparent encapsulating layer of silicone resin, which, together with the base substrate, bestows stiffness on the photomultiplier device, preventing warpage, and covers and protects the chips.

Abstract: Avalanche photodiodes and methods for forming them are disclosed. The breakdown voltage of an avalanche photodiode is controlled through the inclusion of a diffusion sink that is formed at the same time as the device region of the photodiode. The device region and diffusion sink are formed by diffusing a dopant into a semiconductor to form a p-n junction in the device region. The dopant is diffused through a first diffusion window to form the device region and a second diffusion window to form the diffusion sink. The depth of the p-n junction is based on an attribute of the second diffusion window.

Abstract: Techniques and apparatus for using single photon avalanche diode (SPAD) devices in various applications.

Abstract: Several detailed layout designs are disclosed, for the monolithic integration of avalanche devices in large arrays, that can be operated as Avalanche Photo-Diodes (APDs) or Avalanche Light Emitting Diodes (ALEDs) depending only on the applied bias conditions, which can be software-controlled from peripheral circuitry. If the deposited films have direct bandgaps, then the devices can emit light even in the absence of avalanche operation. In particular, the layouts according to the invention comprise a sensor/emitter matrix achieved through the replication of basic Pixel/Lixel cells.

Abstract: A multi-pixel photodetector array may include a semiconductor substrate having a back side and a front side, Geiger mode avalanche photodiodes (GM-APDs) on the semiconductor substrate, each including an anode contact, and a common cathode for the GM-APDs and having a first connection lead on the backside of the semiconductor substrate. The multi-pixel photodetector array may include a second connection lead, and a common anode on the front side of the semiconductor substrate and configured to couple in common the anode contacts of the GM-APDs to the second connection lead. Each GM-APD may be configured to generate, when a photon impinges thereon, a current pulse of different shape for discrimination by an external circuit connected to the common cathode and the common anode.

Abstract: An imaging apparatus having a function of enabling focus detection at high speed while exposing an image sensor to light. Imaging apparatus 1 has: a first photoelectric converting element (image sensor 10) that converts an optical image formed on an imaging plane into an electrical signal for forming an image signal; and a second photoelectric converting element (phase difference detecting sensor 20) that receives light having passed through the first photoelectric converting element and converts light into an electrical signal for distance measurement.

Abstract: A method of fabricating multi-spectral photo-sensors including photo-diodes incorporating stacked epitaxial superlattices monolithically integrated with CMOS devices on a common semiconductor substrate.

Abstract: An adhesive layer, an insulating layer and a copper foil are laminated together on both surfaces of a metallic base material by way of for example thermal press molding. In this case, openings (window holes) are formed in opposed positions on a portion of the adhesive layer. A circuit pattern is formed by etching on the copper foil in this state, followed by an external shape machining step of executing separation treatment reaching the metallic base material in predetermined positions including the openings. After that, a part of the insulating layer is cut off along the edge of the opening to obtain a circuit board with the end of the metallic base material exposed.

Abstract: An avalanche photodiode semiconductor device (20) for converting an impinging photon (22) includes a base n+ doped material layer (52) formed having a window section (72) for passing the photon (22). An n? doped material layer (30) is formed on the n+ doped material layer (52) having a portion of a lower surface (74) suitably exposed. An n+ doped material layer (32) is formed on the n? doped material (30). A p+ layer (24) formed on top of the n+ doped layer (32). At least one guard ring (26) is formed in the n? doped layer (30).

Abstract: A method for encoding information that is encoded in spatial variations of the intensity of light characterized by a first wavelength in light characterized by a second wavelength, the method comprising: transmitting the first wavelength light through a photo-conducting material in which electron-hole pairs are generated by absorbing photons from the first wavelength light to generate a first density distribution of electrons homologous with the spatial variations in intensity of the first wavelength light; trapping electrons from the first electron density distributions in a trapping region to generate an electric field homologous with the density distribution in a material that modulates a characteristic of light that passes therethrough responsive to an electric field therein; transmitting a pulse of light having sufficient energy to generate electron-hole pairs in the photo-conducting material through the modulating material and thereafter through the photo-conducting layer to generate a second additional