Abstract:
Transmission mode negative electron affinity gallium arsenide (GaAs) photthodes and dynodes and techniques for the fabrication thereof, utilizing multilayers of GaAs and gallium alluminum arsenide (GaAlAs) wherein the GaAs layer serves as the emitting layer and the GaAlAs serves as an intermediate construction layer and/or as an integral part of the component.
Abstract:
Semiconductor photoelectron emission device comprising mixed crystals of two or more different semiconductors forming a heterojunction with direct transition type defining a first region in which may be excited by photoelectrons and an indirect transition type defining a second region whose forbidden band gap is wider than that of the first region and the surface of which is a photoelectron emission surface.
Abstract:
A transmission photocathode comprising a crystal substrate transparent to the radiation to be detected, at least one epitaxial crystalline intermediate layer having a lattice constant close to that of the detector layer and transparent to the radiation to be detected, and a p-type group III-V compound detector layer. Preferably the intermediate layer is p-type.
Abstract:
A semiconductor photocathode is described in which the electron emission is obtained from a P-type semiconductor into which free electrons are injected from the source or drain of an FET whose channel is normally blocked. Incident photons absorbed in the channel region unblock the FET causing electron emission. Preferably, the device comprises an imaging array of FET's and associated electron emitters.
Abstract:
A transmission photocathode device of the negative-electronaffinity type is disclosed. The device comprises epitaxially grown P type semiconductor layers and an alkali metal or alkali metal-oxygen work-function-reducing activation layer. Also disclosed is a novel method for making a negative-electronaffinity transmission photocathode device. The method enables a photocathode device to be made by the serial epitaxial growth of p type layers of a II-VI or III-V semiconductor on a semiconductor substrate. The method provides for a virtually perfect lattice match between the semiconductor layers thereby increasing the efficiency of the photocathode by eliminating lattice defects which would otherwise exist at the interface between the transmitting material and the absorbing material.
Abstract:
A photoemitter having a high quantum efficiency and a low work function for photoemission, i.e. photoelectric threshold, is formed by depositing a 10-100A film of a wide bandgap Group III-V compound, e.g. gallium phosphide, atop a 0.5-10 micron thick layer of a second Group III-V compound, e.g. gallium antimonide, having a bandgap matching the desired photoelectric threshold. The film surface then is treated with cesium (or cesium and oxygen) to reduce the surface work function of the composite structure to the desired photoelectric threshold. When the Group III-V layer forming the photoemitter is epitaxially grown atop an oriented substrate of a semiconductive material such as gallium arsenide having a bandgap wider than the bandgap of the overlying layer, the resulting photoemitter is transparent only in a range between the bandgap of the substrate and the bandgap of the overlying layer.
Abstract:
A photocathode structure containing a photocathode material, comprising a plate of single crystal gallium indium phosphide having major surfaces and relative proportions of gallium and indium such that the lattice parameter thereof is substantially the same as that of said photocathode material, and, an epitaxial layer of photocathode material located on a first said major surface of said crystal, the thickness of said layer of photocathode material being of the order of the diffusion length of electrons therein and at least part of a second said major surface of the gallium indium phosphide plate being substantially free from contact by solid material.
Abstract:
A thin III-V photoemitter crystal having a thickness ranging from 1 micron to 5 microns as grown on a III-V substrate. The bandgap was determined in advance by proportioning the constituents of the crystal causing the peak of the response curve to occur at a predetermined energy and absorb incident photons of the desired wavelength. Due to the high quality of the crystal, the electron diffusion length thereof was comparable to the thickness allowing transmission optics to be employed. Lattice mismatch between the active crystal and the base was minimized by a transition layer, or a progression of transition layers, of intermediate composition. The presence of this strain relieving structure permitted the growth of the thin, high quality single crystals having a relatively long electron diffusion length. As a specific example, a 20 micron transition layer of GaAs.90Sb.10 was epitaxially grown on a GaAs substrate. A three micron active layer of GaAs.85Sb.15 was grown over the transition layers. This composition of the active layer exhibited a bandgap energy of 1.17 ev corresponding to an absorption wavelength of 1.06 microns.