Abstract:
A microelectronic photomultiplier device is fabricated by discrete proceds to provide a photocathode-anode and dynode chain arrangement which is analogous in operation to conventional photomultiplier tubes. This microelectronic photomultiplier device provides for low level photon detection and realizes the advantages of high reliability, small size and fast response, plus lower cost, weight and power consumption compared to conventional photomultiplier tubes. In addition, the fabrication on an SOI substrate permits integration of logic and control circuitry with detectors. The insulating substrate also permits the integration of an on-chip high voltage supply and may easily be extended to a plurality of detectors offering improved performance and design flexibility.
Abstract:
A muitilayer microelectronic photomultiplier device is fabricated by disce procedures to provide a photocathodeanode and dynode chain arrangement which is analogous in operation to conventional photomultiplier tubes. This multilayer microelectronic photomultiplier device provides for low level photon detection and realizes the advantages of high reliability, small size and fast response, plus lower cost, weight and power consumption compared to conventional photomultiplier tubes. In addition, the fabrication on an SOI substrate permits integration of logic and control circuitry with detectors. The insulating substrate also permits the integration of an on-chip high voltage supply and may easily be extended to a plurality of detectors with high packing densities due to the inherently stacked geometry offering improved performance and design flexibility.
Abstract:
A microelectronic photomultiplier device is fabricated by discrete proceds to provide a photocathode-anode and dynode chain arrangement which is analogous in operation to conventional photomultiplier tubes. This microelectronic photomultiplier device provides for low level photon detection and realizes the advantages of high reliability, small size and fast response, plus lower cost, weight and power consumption compared to conventional photomultiplier tubes. In addition, the fabrication on an SOI substrate permits integration of logic and control circuitry with detectors. The insulating substrate also permits the integration of an on-chip high voltage supply and may easily be extended to a plurality of detectors offering improved performance and design flexibility.
Abstract:
To assure detection of fluorescence produced from continuously supplied fine particles such as DNA bases with accuracy and excellent efficiency, fine particles supplied from a flow cell are introduced into a through-hole of a hollow photomultiplier. An optical fiber is disposed in axial alignment with the through-hole of the photomultiplier and irradiates an exciting light beam onto the fine particles staying in the through-hole. Light-induced fluorescence is thus detected by the photomultiplier which has a photocathode on an inner circumference of the through-hole.
Abstract:
A photomultiplier tube includes a tube, a focussing electrode unit formed with a photoelectron transmission hole whose center is positioned offset from a central axis of the tube and a dynode positioned in confrontation with the transmission hole. A center of the dynode is also offset from the central axis of the tube. A grid type electrodes array are positioned at the same axial position of the dynode and positioned beside the dynode in a radial direction of the tube. The focussing electrode provides desirable uniformity in distribution of photoelectronics over the dynode even by the deviating position of the photoelectron transmission hole and the dynode. By positioning the dynode away from the central axis in the radial direction of the tube, the grid type electrode array can be positioned beside the dynode. Thus, entire length of the tube can be reduced without any change in a diameter of the tube because of the fact that a length of the dynode in the axial direction of the tube only influences the axial length of the tube.
Abstract:
A parallel plate electron multiplier employing active dynode surfaces in confronting spaced relationship for effecting electron multiplication between the input and the output thereof in the active dynode area. Electron multiplication occurs in response to an accelerating biasing field extending between the input and the output. Electrostatic elements laterally of the dynode area establish lateral biasing fields in a direction transverse of the dynodes for containing electrons in the dynode area and for attracting positively charged species away from the dynode area in order to reduce spurious signals.
Abstract:
In an apparatus for counting ions, a double-collector electron multiplier comprises a first and a second collector for receiving secondary electrons from an exit end of a dynode member of the electron multiplier. The first and the second collectors have a first and a second electron receiving surface, respectively, wherein the second electron receiving surface has a narrower area than the first electron receiving surface. A first and a second amplifier are separately used in amplifying a first and a second electric current produced from the first and the second collectors, respectively. An ammeter is connected through a switch selectively to the first and the second amplifiers to provide a selected measuring range for the number of ions which enter the electron multiplier.
Abstract:
A light detector which can be gated on and off over an ultrashort time window, such as in picoseconds or femtoseconds, is disclosed. The light detector includes, in one embodiment, an input slit for receiving a light signal, relay optics, a sweep generator and a tubular housing, the tubular housing having therein a photocathode, an accelerating mesh, a pair of sweeping electrodes, a microchannel plate, a variable aperture and a dynode chain. Light received at the input slit is imaged by the relay optics onto the photocathode. Electrons emitted by the photocathode are conducted by the accelerating mesh to the sweeping electrodes where they are swept transversely across the tubular housing at a rate defined by the sweep generator over an angular distance defined by the sweeping electrodes, in a similar manner as in a streak camera. Swept electrons strike the microchannel plate where electron multiplication is accomplished. Exiting electrons which pass through the variable aperture and which strike the first dynode (cathode) in the dynode chain are further multiplied and outputted from the last dynode anode in the dynode chain as an analog electrical signal, the analog electrical signal corresponding to the intensity of the light signal during the time window over which swept electrons are picked up by the first dynode. In another embodiment of the invention all of the dynodes in the chain except for the last dynode are replaced by a second microchannel plate.
Abstract:
An electron discharge device, such as a photomultiplier tube, has an evacuated envelope with an alkali-antimonide photoemissive cathode therein. A thermionic emission-reduction coating is disposed within the envelope. The coating alloys with the constituents of the photoemissive cathode to reduce thermionic emission. The thermionic emission reduction coating is formed preferably of indium; however, indium oxide may also be used.
Abstract:
A photomultiplier tube (PMT) converts a received light signal to an output electrical signal of substantially greater intensity by employing a photocathode to convert incident light to free electrons, a plural dynode accelerating structure for effectively multiplying said free electrons, and an impact ionization diode (IID) for further multiplying and collecting said free electrons to provide a corresponding electrical output signal. The PMT can be an electrostatic device, in which the photocathode and the dynodes are mounted in opposed staggered positions, or a static crossed field device, in which the photocathode and the dynodes all are mounted opposite an accelerating rail and a magnetic field is provided to urge the electrons laterally along the tube. The IID''s junction is reverse biased and the entire diode is maintained at a substantially higher potential than the last dynode. The PMT can be gain controlled or turned off without affecting dynode potentials by controlling the IID''s potential. Due to the gain provided by the IID, dynode current can be reduced greatly, thereby to increase substantially the tube''s life without affecting its overall gain.