Abstract: An X-ray imaging array is described together with a method for its manufacture. The array is defined by a set of PN junctions in a silicon wafer that extend all the way through between the two surfaces of the wafer. The PN junctions are formed using neutron transmutation doping that is applied to P-type silicon through a mask, resulting in an array of N-type regions (that act as pixels) in a sea of P-type material. Through suitable placement of the biassing electrodes, a space charge region is formed that is narrower at the top surface, where X-rays enter the device, and wider at the lower surface. This ensures that most of the secondary electrons, generated by the X-ray as it passes through the wafer, get collected at the lower surface where they are passed to a charge readout circuit.

Abstract: A high-energy photon imaging system including an imaging head, a signal processor, a data acquisition system and an image processing computer. The imaging head includes a detector including a plurality of closely-packed detection modules. Each detection module includes a plurality of detection elements mounted to a circuit carrier. The detection elements produce electrical pulses having amplitudes indicative of the magnitude of radiation absorbed by the detection elements.

Abstract: A system for the detection of infrared light (IR with wavelength &lgr;>800 nm) of high sensitivity. It is based on the measurement of the capacitance in structures made of amorphous silicon, constituted of a junction having two electrodes connecting to outside and susceptible of being built using already-known technologies for the deposition of thin films. The p+ and n+ layers (FIG. 1) are made of materials strongly doped with boron and phosphorous atoms. During the fabrication process the temperatures are such as to permit its construction on various substrates. The technologies used make its fabrication possible on large areas and its conformation in two-dimensional matrices of high resolution.

Abstract: Multi-photon excitation fluorescence microscopy is carried out by focusing an excitation beam by an objective lens onto a specimen and collecting the multi-photon fluorescence light emitted from the specimen to the objective lens and directing the fluorescent light on an optical path to a detector. Fluorescent light emissions from the specimen collected by a condenser lens on the opposite side of the specimen from the objective lens are directed to a dichoic mirror, which reflects the light photons back into the condenser lens and thence into and through the objective lens where they are directed on an optical path to the detector. Significantly increased fluorescent photon collection efficiency is obtained as well as improved image intensity of the detected fluorescent light.

Abstract: An image sensing device including an imaging sensor, a package having opposing side portions, and an infrared light selective element coupled to the opposing side portions and overlying a top side portion of the imaging sensor, the selective element including a plastic element and a dye.

Abstract: A laser scanning microscope produces molecular excitation in a target material by simultaneous absorption of three or more photons to thereby provide intrinsic three-dimensional resolution. Fluorophores having single photon absorption in the short (ultraviolet or visible) wavelength range are excited by a beam of strongly focused subpicosecond pulses of laser light of relatively long (red or infrared) wavelength range. The fluorophores absorb at about one third, one fourth or an even smaller fraction of the laser wavelength to produce fluorescent images of living cells and other microscopic objects. The fluorescent emission from the fluorophores increases cubicly, quarticly or even higher power law with the excitation intensity so that by focusing the laser light, fluorescence as well as photobleaching are confined to the vicinity of the focal plane.

Abstract: A non-dispersive infrared gas analyzer for determining concentrations of carbon dioxide and/or carbon monoxide, hydrocarbons, and nitrogen oxides has two measuring cells 4, 6 consecutively traversed by a beam, with an optopneumatic detector 22 for carbon dioxide and an optopneumatic detector 23 for carbon monoxide arranged between them. Detectors 7, 8 for hydrocarbons and nitrogen oxides are arranged on the measuring cell 6 located downstream from detectors 22, 23 in the direction of the beam.

Abstract: An imaging system having an imaging sensor providing sensor signals in response to incident light and control signals, control circuitry configured to generate control signals for controlling said imaging sensor, signal processing circuitry for generating image data in response to said sensor signals, and a light selective element for selecting the incident light encountered by said imaging sensor, the light selective element comprising an ionically-colored glass having a surface that is treated with a chemical stabilizer.

Abstract: A gamma camera arrangement and method for imaging a patient without moving the patient from the regular hospital bed to a patient carrier bed.

Abstract: An energy dispersive X-ray detector assembly has a detector element of a high-purity silicon substrate with a pair of electrodes, one on either side of the silicon substrate, to create an depletion layer in the silicon substrate when an electric field is created between the electrodes to enable the detection of X-rays. The silicon substrate has a resistivity of at least 10 k.OMEGA..multidot.cm and a thickness in the incident direction of the X-rays of approximately 3 to 5 mm. A refrigerator system, such as a closed cycle gas circulation refrigerator, can be used to cool the detector element to enable the provision of a compact detector assembly.

Abstract: A method for inferring the photoelectric absorption of a formation by directly mapping spectroscopic measurements of gamma rays induced in the formation using a fast neutron source. The mapping is accomplished by creating a polynomial function based on counts of gamma-ray events in the gamma-ray energy spectrum; the coefficients of the polynomial function are determined in known calibration environments, and the value of the polynomial is the inferred photoelectric absorption parameter. The spectroscopic measurements are preferably generated by sorting gamma-ray counts of the gamma-ray spectrum into a plurality of energy-dependent channels, and measuring these gamma-ray energy distributions during different portions of the firing cycle where different types of dominant gamma-ray production reactions occur.

Abstract: A sensor device and a method for non-dispersive analysis of gas mixtures for determining the concentration of one gas component contained therein, whose absorbency may be influenced as a result of collision broadening by other components contained in a gas mixture (GC). The device includes: a measuring chamber (5), containing the gas mixture; a radiation source (4), emitting radiation (15) through the chamber; detector (10, 14, 16) for receiving radiation passed through the chamber; optical bandpass filters (9a-c) positioned between the detectors and the radiation source, the detectors being coupled with measuring ducts (1-3) or measuring cycles. An optical gas filter (11), contains said gas component or a mixture thereof and is located between the detector and the radiation source. From the first measuring duct is obtained a first signal (S1) and from the second measuring duct is obtained a second signal (S2) relating to radiation also passed through the optical gas filter.

Abstract: An infrared video camera system comprises an uncooled infrared sensor mounted and a thermally conductive thin walled radiation shield for shielding radiation from reaching an active surface of the uncooled infrared sensor. A TEC maintains the sensor active surface and the radiation shield at a substantially constant temperature. The uncooled infrared sensor and radiation shield are further housed in a hollow thermally conductive vacuum cover which is vacuum sealed with a base assembly and includes a vacuum sealed infrared transparent window in an aperture at a top end of the vacuum cover for allowing infrared radiation to reach the active surface and for forming a vacuum chamber enclosing the infrared sensor and radiation shield. A relay optical cell mounted to a camera body comprises at least one optical element for relaying an image formed at its entrance onto the active surface.

Abstract: A nuclear medical imaging system generates transmission and emission images simultaneously. The system includes a gamma camera and a linear transmission source disposed on opposite sides of an imaging region in which a patient lies. A plurality of views are taken at different rotational angles around a patient. At each angle, the view acquisition period is divided into two segments based on whether the transmission source is on or off. Emission image data is acquired either in both period segments or only while the transmission source is off. The transmission image data is acquired when the transmission source is on, and crosstalk image data is acquired when the transmission source is off.

Abstract: Broad spectrum ultraviolet inspection methods employ an achromatic catadioptric system to image the surface of an object, such as a semiconductor wafer or photomask, at multiple ultraviolet (UV) wavelengths over a large flat field (with a size on the order of 0.5 mm) in order to detect and identify defects. The imaging system provides broad band correction of primary and residual, longitudinal and lateral, chromatic aberrations for wavelengths extending into the deep UV. UV imaging applications include a method that illuminates an object with fluorescence-excitation radiation to stimulate fluorescent emission at a plurality of UV wavelengths, then images the fluorescent emissions and detects the images so formed in UV wavelength bands distributed over at least 50 nm (preferably 100-200 nm) wavelength. Photoresist patterns can be analyzed in this way.

Abstract: A gas volume concentration is determined. An electromagnetic radiation is emitted (state 1) through the gas volume. The radiation is filtered by temporally modulating the spectral transmission of said filter so as to obtain a temporal modulation of the energy of the radiation transmitted by the gas volume and this filter. This temporally modulated energy is detected and a signal E is extracted from it, the signal particularly depending on the concentration of the gas. The component Eac(1) of the time-variable signal and the component Edc(1) of the signal, which is not a time-variable signal are isolated. A radiation stops is emitted (state 0), and the component Eac(0) and the component Edc(0) of the signal received by the detector are isolated. The terms Eac(1)-Eac(0) and Edc(1)-Edc(0) are calculated, and the ratio (Eac(1)-Eac(0))/(Edc(1)-Edc(0)) is formed which then solely depends on the gas concentration c. From this, c is deduced.

Abstract: This detector comprises a gas chamber (2) containing plane electrodes (4, 6, 8) delimiting conversion (C) and amplification (A) gaps. One of the electrodes is perforated with holes (18) and forms the detector cathode (6). The distance between the detector cathode and the anode (8) is less than 500 .mu.m. The intensity of the electric field in the amplification gap is ten times higher than the intensity of the electric field in the conversion gap. Application in particle physics, medicine, biology.

Abstract: Extreme ultraviolet light (EUV) is detected using a precisely defined reference pattern formed over a shallow junction photodiode. The reference pattern is formed in an EUV absorber preferably comprising nickel or other material having EUV- and other spectral region attenuating characteristics. An EUV-transmissive energy filter is disposed between a passivation oxide layer of the photodiode and the EUV transmissive energy filter. The device is monolithically formed to provide robustness and compactness.

Abstract: The Laser Induced Fluorescence Attenuation Spectroscopy (LIFAS) method and apparatus preferably include a source adapted to emit radiation that is directed at a sample volume in a sample to produce return light from the sample, such return light including modulated return light resulting from modulation by the sample, a first sensor, displaced by a first distance from the sample volume for monitoring the return light and generating a first signal indicative of the intensity of return light, a second sensor, displaced by a second distance from the sample volume, for monitoring the return light and generating a second signal indicative of the intensity of return light, and a processor associated with the first sensor and the second sensor and adapted to process the first and second signals so as to determine the modulation of the sample.

Abstract: A night vision device includes an image intensifier tube having a photocathode responsive to light in the wavelength range extending from about 1 .mu.m to about 2 .mu.m. The photocathode releases photoelectrons in response to photons of light in this wavelength range. A photomultiplier tube includes such a photocathode to provide an image in response to light of such a wavelength. A method of making such a photocathode is set out.