Abstract:
The present invention relates in general to nanoparticles exhibiting luminescence such as photostimulated luminescence or photoluminescence and optical switching processes based upon such properties, in more particular, the use of such photostimulated luminescence exhibiting nanoparticles and switching nanoparticle for optical storage apparatuses and sensors as well as methods of making and using same.
Abstract:
The present invention relates in general to nanoparticles exhibiting luminescence such as photostimulated luminescence or photoluminescence and optical switching processes based upon such properties, in more particular, the use of such photostimulated luminescence exhibiting nanoparticles and switching nanoparticle for optical storage apparatuses and sensors as well as methods of making and using same.
Abstract:
The present invention concerns the use of a photovoltaic element as sensor for checking the functionality of transmitters in the infrared range.
Abstract:
An AlxGa1−xAs/GaAs/AlxGa1−xAs quantum well exhibiting a bound-to-quasibound intersubband absorptive transition is described. The bound-to-quasibound transition exists when the first excited state has the same energy as the “top” (i.e., the upper-most energy barrier) of the quantum well. The energy barrier for thermionic emission is thus equal to the energy required for intersubband absorption. Increasing the energy barrier in this way reduces dark current. The amount of photocurrent generated by the quantum well is maintained at a high level.
Abstract translation:描述了表现出界限对准的子带间吸收转变的Al x Ga 1-x As / GaAs / Al x Ga 1-x As量子阱。 当第一激发态具有与量子阱的“顶部”(即,最上面的能量势垒)相同的能量时,存在边界到准近渡的转变。 因此,热离子发射的能量势垒等于子带间吸收所需的能量。 以这种方式增加能量屏障可以减少暗电流。 由量子阱产生的光电流的量保持在高水平。
Abstract:
Disclosed is a radiation detector which includes at least one photoconductive detector and a modulator, which modulates in an on-off manner radiation passing to the photoconductive detector from a radiation source. A bias source is connected to one terminal of the photoconductive detector. A first amplifier is connected to the other terminal of the photoconductive detector, and a second amplifier receives an output of the first amplifier. A first phase detector detects the phase of modulation of the radiation source by the modulator and generates a reference signal relating thereto. A switch in the second amplifier changes, in response to the reference signal generated by the first phase detector, the second amplifier between an inverting state and a non-inverting state as the modulator changes the phase of modulation of the radiation.
Abstract:
A semiconductor crystal infrared detecting portion structure is provided in a photoconductive infrared detector and is provided at opposite ends with first and second electrodes so biased that the first and second electrodes have a positive potential and a ground potential respectively. The semiconductor crystal infrared detecting portion structure has an infrared receiving part so that the semiconductor crystal infrared detecting portion structure comprises a first half region defined between the infrared receiving part and the first electrode and a second half region defined between the infrared receiving part and the second electrode. At least the second half region reduces in section area toward the second electrode to increase a resistance of at least the second half region.
Abstract:
An infrared detector element includes a metallic patch which is positioned on the surface of an upper contact layer. A multiple quantum well ("MQW") infrared sensitive structure is positioned between the first contact layer and a second contact layer. The conductive contact layers are transparent to infrared radiation. A groundplane which is reflective to infrared radiation is positioned adjacent the second contact layer. A resonant cavity is formed between the metallic patch and the groundplane. The thickness of this cavity is not greater than approximately one eighth of the wavelength of the incident infrared radiation within the cavity. The metallic patch functions to couple the incident infrared radiation into the resonant cavity wherein the E-field is oriented substantially normal to the plane of the MQW structure. A plurality of the detector elements can be used to form a single pixel and an array of the pixels can be used to form a complete infrared radiation imager.
Abstract:
A focal plane array (30) for a thermal imaging system (20). The focal plane array (30) may include a number of thermal sensitive elements (42) formed by a first series of slots (78) and a second series of slots (80). The thermal sensors (40) may be bounded by a border (41). The thermal sensors (40) may provide a sensor signal output representative of thermal radiation incident to the focal plane array (30). The first series of slots (78) may include a leading first slot (82) and a trailing first slot (84). Additionally, the first series of slots (78) may include a number of substantially parallel first slots therebetween. The second series of slots (80) may include a leading second slot (86) in a trailing second slot (88). The second series of slots (80) may also include a number of substantially parallel second slots therebetween. One of the first slots may extend beyond the leading second slot (86). Additionally, one of the first slots may extend beyond the trailing second slot (88). A common electrode (36) may be coupled to the thermal sensitive elements (42) and to the border (41). An optical coating (34) sensitive to infrared radiation may be provided in communication with the common electrode (36).
Abstract:
A resonant, photoconductive detector for infrared radiation in which a reduced-volume pattern of the photoconductor permits impedance-matching to free space. The photoconductor pattern is a split-ring pattern, typically made of HgCdTe, which is virtually cylindrically symmetric, yielding a non-polarization-sensitive response. The region below the patterned photoconductor is a quarter-wavelength resonant cavity type structure. The ohmic contacts are conductively distanced from one another by use of the split-ring pattern. Spacing dimensions are slightly less than a wavelength for the infrared wavelengths to be absorbed; but ring-width dimensions of the photoconductor are substantially less to effect the volume reduction and the corresponding detectivity and radiation-hardness improvements. The essentially cylindrical isotropic pattern eases fabrication by averaging etching nonuniformities.
Abstract:
A method and apparatus for detecting infrared radiation is disclosed. The apparatus comprises a substrate (12) having readout and signal processing circuits (14) integrated therein. The substrate (12) is formed from a material selected from the group consisting of silicon, gallium arsenide, or germanium. A first semiconductor layer (28) is grown on the substrate (12) from a material selected from the group consisting of mercury-cadmium-telluride, mercury-zinc-telluride, mercury-cadmium-selenide, mercury-zinc-selenide, mercury-cadmium-sulfide, mercury-zinc-sulfide, lead-tin-telluride, lead-tin-selenide, lead-tin-sulfide, indium-arsenide-antimonide, gallium-indium-antimonide, or gallium-antimonide-arsenide. A second semiconductor layer (30) is then grown on the first semiconductor layer (28).