Abstract:
A radiation convertor for use in neutron imaging detectors includes apparatus for conversion of energetic primary charged particles resulting from neutron capture into low energy (eV) secondary electrons. The radiation convertor includes efficient secondary electron emitters, which are preferably alkali halide secondary electron emitters which are preferably CsI secondary electron emitters. The radiation convertor preferably combines at least one layer of Gd and an efficient secondary electron emitter preferably of alkali halide, preferably CsI. The layer of Gd may be at least one metallic layer selected from natural Gd and 157 Gd and this is used in combination with a layer of CsI. The neutron convertor may be alternatively 6Li, LiH or 177 Hf used in combination with an efficient secondary electron emitter, preferably alkali halide emitter, preferably CsI. A neutron imaging detector of the invention may combine a secondary emission composite neutron convertor including efficient secondary electron emitters and an electron multiplier which is sensitive to low energy secondary electrons emitted from the composite neutron convertor. In such a neutron imaging detector combination, the electron multiplier may be a vacuum micro channel plate (MCP) multiplier, a vacuum microsphere plate (MSP), or any other vacuum electron multiplier and imaging device, or a gaseous electron imaging multiplier, preferably a gaseous electron multiplier in which the secondary electron multiplication starts at their emission location from the convertor, preferably a low-pressure multistage electron multiplier.
Abstract:
An X-ray detector including a photocathode arranged to receive X-ray radiation and being operative to provide in response thereto an output of electrons, and at least one electron multiplier operative at subatmospheric pressure and in response to the output of electrons from the photocathode to provide an avalanche including an increased number of electrons.
Abstract:
Apparatus for digital imaging including at least one electron multiplier (16) arranged to receive beta radiation from a sample (12), apparatus for collimating the beta radiation without totally blocking all radiation from any location within a given region of interest on the sample (12), and readout electrodes operative in response to electrons from the electron multiplier (16) to provide a first output indication of the incidence and location of beta radiation from the sample (12).
Abstract:
The present invention may provide a particle or radiation detector or imager (1) which may be used for accurate recording of medical (2-D) X-ray images. The imager (1) includes at least one detector panel. The detector panel includes a microgap detector with an array of pixel electrodes (18) of a novel form. Each pixel electrode (18) is insulated from a planar cathode (16) by means of an insulating layer (17). Each pixel electrode (18) is connected to an underlying contact by means of a via hole in the insulating layer (17). The insulating layer (17) is preferably conformal with the pixel electrodes (18). The underlying contact is connected to an electronic measuring element (14) which preferably lies underneath the pixel electrode (18) and is about the same size as, or smaller than the pixel electrode (18). The measuring element (14) may be a storage device such as a capacitor, a digital counter or similar. A read-out circuit (13), e.g. a switching transistor, is connected to the measuring device (14). The switching transistor (13) may be a thin film transistor. Alternatively, both measuring element (14) and transistor (13) may be formed in a single crystal semiconductor, e.g. a VLSI, and a complete imager formed from several detector panels in an array. The drift electrode (19) of the microgap detector preferably includes a photocathode. The photocathode may be directly evaporated onto a phosphor.
Abstract:
An X-ray detector including a photocathode arranged to receive X-ray radiation and being operative to provide in response thereto an output of electrons, and at least one electron multiplier operative at subatmospheric pressure and in response to the output of electrons from the photocathode to provide an avalanche including an increased number of electrons.
Abstract:
A radiation convertor for use in neutron imaging detectors includes apparatus for conversion of energetic primary charged particles resulting from neutron capture into low energy (eV) secondary electrons. The radiation convertor includes efficient secondary electron emitters, which are preferably alkali halide secondary electron emitters which are preferably CsI secondary electron emitters. The radiation convertor preferably combines at least one layer of Gd and an efficient secondary electron emitter preferably of alkali halide, preferably CsI. The layer of Gd may be at least one metallic layer selected from natural Gd and 157 Gd and this is used in combination with a layer of CsI. The neutron convertor may be alternatively 6Li, LiH or 177 Hf used in combination with an efficient secondary electron emitter, preferably alkali halide emitter, preferably CsI. A neutron imaging detector of the invention may combine a secondary emission composite neutron convertor including efficient secondary electron emitters and an electron multiplier which is sensitive to low energy secondary electrons emitted from the composite neutron convertor. In such a neutron imaging detector combination, the electron multiplier may be a vacuum micro channel plate (MCP) multiplier, a vacuum microsphere plate (MSP), or any other vacuum electron multiplier and imaging device, or a gaseous electron imaging multiplier, preferably a gaseous electron multiplier in which the secondary electron multiplication starts at their emission location from the convertor, preferably a low-pressure multistage electron multiplier.
Abstract:
Apparatus for digital imaging including at least one electron multiplier (16) arranged to receive beta radiation from a sample (12), apparatus for collimating the beta radiation without totally blocking all radiation from any location within a given region of interest on the sample (12), and readout electrodes operative in response to electrons from the electron multiplier (16) to provide a first output indication of the incidence and location of beta radiation from the sample (12).