Abstract:
The present invention is a directed to a non-pixelated scintillator array for a CT detector as well as an apparatus and method of manufacturing same. The scintillator array is comprised of a number of ceramic fibers or single crystal fibers that are aligned in parallel with respect to one another. As a result, the pack has very high dose efficiency. Furthermore, each fiber is designed to direct light out to a photodiode with very low scattering loss. The fiber size (cross-sectional diameter) may be controlled such that smaller fibers may be fabricated for higher resolution applications. Moreover, because the fiber size can be controlled to be consistent throughout the scintillator may and the fibers are aligned in parallel with one another, the scintillator array, as a whole, also is uniform. Therefore, precise alignment with the photodiode array or the collimator assembly is not necessary.
Abstract:
A two-dimensional ionising particle detector including a matrix of detecting fibers, each detecting fiber forming a pixel of the detector. Each detecting fiber is composed of a glass capillary filled with a liquid scintillator for which the chemical composition is chosen such that an average free path of primary scintillation photons is negligible compared with a diameter of the capillary. The detector is applicable, for example, to high resolution particle imagery.
Abstract:
An apparatus which is capable of detecting the incident direction of a radiation incident from afar and which is made to be small in size and light in weight is provided. The apparatus comprises a radiation detection system 12 having a scintillating optical fiber 10 converting an incident radiation into a light signal, light receiving elements 14a, 14b respectively connected to both ends of said scintillating optical fiber and converting the light signals propagating in two directions along said scintillating optical fiber into electric signals, and a radiation analysis system 16 deriving the incident position of the radiation on the basis of the difference between the arrival times of the electric signals from said light receiving elements. The scintillating optical fiber is arranged in a state of being curved in a circular arc shape, and a large number of flat collimators 18 are arranged on the outer periphery of the scintillating optical fiber in a radial pattern at nearly even intervals.
Abstract:
The invention related to a method for measuring a dose of radiation by a beam of high-power radiation, where in a scintillate (1) is disposed below said beam in order to emit scintillation light whose intensity is a function of the dose of said beam irradiating said scintillate (1); the scintillate (1) is coupled to a device (8) for measuring the light emitted by the scintillate (1) via an optical fiber (2); the amount of light transmitted by the optical fiber (2) is measured; the intensity of the light emitted by the scintillate (1) is determined on the basis of the light emitted by at least one other source, after said optical fiber (2) is used for transmission of the light emitted by the scintillate (1) and the light emitted by each other source. The invention also related to a device for measuring the dose of radiation for the implementation of said method.
Abstract:
A device (1) for collecting ionizing radiation comprises a scintillating optical fiber (4) received in an opaque sheath, having a first end (7) for receiving ionizing radiation and a second end (14), the fiber is arranged to convert the ionizing radiation received via its first end into light signals and to deliver the signals via its second end. The device further comprises filter means (9) placed at the first end (10) of the sheath (3) to prevent external photons (null) and gamma type (null) ionizing radiation from gaining access to the first end (7) of the scintillating fiber (4), and at the second end (14) of the scintillating fiber (4), first connection means (16) suitable for connection to light guide means (2) for enabling the second end (14) of the fiber to be coupled to the end (17) of a light guide (18) of the light guide means.
Abstract:
The present invention is an apparatus for detecting ionizing radiation, having: a waveguide having a first end and a second end, the waveguide formed of a scintillator material wherein the therapeutic ionizing radiation isotropically generates scintillation light signals within the waveguide. This apparatus provides a measure of radiation dose. The apparatus may be modified to permit making a measure of location of radiation dose. Specifically, the scintillation material is segmented into a plurality of segments; and a connecting cable for each of the plurality of segments is used for conducting scintillation signals to a scintillation detector.
Abstract:
A dosimeter for an x-ray brachytherapy system permits in situ monitoring and control of radiation treatment via a miniaturized energy transducer within a human body. The dosimeter comprises a scintillating optical fiber having a distal end which is placed at the treatment site and a proximal end which is coupled to a dosimeter measurement unit. Utilizing energy supplied by an energy source, the miniaturized transducer generates x-ray photons. The scintillating optical fiber absorbs x-ray photons, converts the x-ray photons into light photons, and conveys the light photons to a dosimeter measurement unit. The light photons are converted into an electrical current which is representative of the intensity of the x-ray photons. The dosimeter measurement unit utilizes the electrical current to calculate and display the instantaneous and accumulated radiation dose, and radiation dose parameters are utilized to adjust energy levels, which are sent to the miniature energy transducer. Use of the miniaturized energy transducer in combination with the dosimeter eliminates most of the problems related to the methods based on the use of radioactive sources and offers a method for efficient, accurate, and controllable radiation treatment.
Abstract:
The present invention is an apparatus for detecting ionizing radiation, having: a waveguide having a first end and a second end, the waveguide formed of a scintillator material wherein the therapeutic ionizing radiation isotropically generates scintillation light signals within the waveguide. This apparatus provides a measure of radiation dose. The apparatus may be modified to permit making a measure of location of radiation dose. Specifically, the scintillation material is segmented into a plurality of segments; and a connecting cable for each of the plurality of segments is used for conducting scintillation signals to a scintillation detector.
Abstract:
A radiation detecting section including scintillation fibers is arranged in a one-dimensional, two-dimensional or three-dimensional manner. A multichannel amplitude analyzer can obtain an incident position of radiation in the radiation detecting section, and a radiation dose rate at the incident position depending upon a signal having amplitude according to a difference in arrival time between two input signals. A microcomputer carries out inverse problem analysis to estimate a radiation source distribution or a spatial radiation intensity distribution.
Abstract:
A contraband detection system (18) using a single, cone shaped neutron beam determines substances concealed in a sample object by developing total neutron cross section spectra for a plurality of elements, including carbon, nitrogen, oxygen, hydrogen and other potential contraband-indicating elements. A processor (26) performs a contraband determination classification based on the neutron total cross section spectra for the plurality of elements, including hydrogen and elements which do not have peaks in the energy range of interest. The contraband detection system (18) includes a neutron source (20) for producing a pulsed, cone shaped beam of fast white neutrons; a spatial neutron detection array (40); a conveyor system (28) for situating a sample object (29) between the source (20) and the detection array (40); a spectra analysis system (24) for determining the neutron total cross section spectra of elements located in the sample object; and the processor (26). The neutron source (20) produces a pulsed beam (36) of fast white neutrons having sufficient energy range whereby removal of neutrons from the beam caused by the presence of a plurality of contraband-indicating elements can be determined. Various techniques of making contraband classification determinations are also disclosed.