出典(authority):フリー百科事典『ウィキペディア(Wikipedia)』「2012/09/20 00:23:10」(JST)
A scintillation counter measures ionizing radiation. The sensor, called a scintillator, consists of a transparent crystal, usually phosphor, plastic (usually containing anthracene) or organic liquid (see liquid scintillation counting) that fluoresces when struck by ionizing radiation.
A sensitive photomultiplier tube (PMT) measures the light from the crystal, and the output signal is fed to an electronic amplifier and other electronic equipment to count and possibly quantify the amplitude of the signals produced by the photomultiplier.
Scintillation counters are widely used because they can be made inexpensively yet with good quantum efficiency.
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When a charged particle strikes the scintillator, the phosphor's atoms are excited and emit photons, which are directed at the photomultiplier tube's photocathode which is connected to the negative of a high voltage source. Each incident photon releases an electron. A number of accelerating electrodes called dynodes are arranged in the tube at increasing positive potentials and the electron is accelerated by this electric field towards the first dynode. The incident electron causes multiple secondary electrons to be emitted, which accelerate towards and hit the second dynode. More electrons are emitted and the electron multiplication chain continues through the increasing potentials of the dynodes, with increasing numbers of electrons generated each time. By the time the electrons reach the anode, enough have been released to generate a measurable voltage pulse across external resistors. This voltage pulse is amplified and recorded by the processing electronics.
The scintillator must be in complete darkness so that visible light photons do not swamp the individual photon events caused by incident ionising radiation. A thin opaque foil, such as aluminised mylar, is used to achieve this, though it must have a low enough mass to prevent attenuation of the incident radiation that is being measured.
Cesium iodide (CsI) in crystalline form is used as the scintillator for the detection of protons and alpha particles. sodium iodide (NaI) containing a small amount of thallium is used as a scintillator for the detection of gamma waves and Zinc Sulphide is widely used as a detector of alpha particles.
The quantum efficiency of a gamma-ray detector (per unit volume) depends upon the density of electrons in the detector, and certain scintillating materials, such as sodium iodide and bismuth germanate, achieve high electron densities as a result of the high atomic numbers of some of the elements of which they are composed. However, detectors based on semiconductors, notably hyperpure germanium, have better intrinsic energy resolution than scintillators, and are preferred where feasible for gamma-ray spectrometry. In the case of neutron detectors, high efficiency is gained through the use of scintillating materials rich in hydrogen that scatter neutrons efficiently. Liquid scintillation counters are an efficient and practical means of quantifying beta radiation.
Scintillation counters are used to measure radiation in a variety of applications.
Several products have been introduced in the market utilising scintillation counters for detection of potentially dangerous gamma-emitting materials during transport. These include scintillation counters designed for freight terminals, border security, ports, weigh bridge applications, scrap metal yards and contamination monitoring of nuclear waste. There are variants of scintillation counters mounted on pick-up trucks and helicopters for rapid response in case of a security situation due to dirty bombs or radioactive waste.[1][2] Hand-held units are also commonly used.[3]
The industrial contamination monitoring detector, consisting of a scintillator and photomultiplier tube, finds wide application in the field of radioactive contamination monitoring of personnel and the environment. Detectors are designed to have one or two scintillation materials, depending on the application. Such as zinc sulphide is used for alpha particle detection, whilst plastic scintillators are used for beta detection. The resultant scintillation energies can be discriminated so that alpha and beta counts can be measured separately with the same detector. "Single phosphor" detectors are used for either alpha or beta, and "Dual phosphor" detectors are used to detect both. These detectors are used in both hand-held and fixed monitoring equipment. Such instruments are relatively inexpensive compared with the gas proportional detector. They are also able to discriminate between alpha and beta, which the Geiger tube cannot.
Scintillators often convert a single photon of high energy radiation into high number of lower-energy photons, where the number of photons per megaelectronvolt of input energy is fairly constant. By measuring the intensity of the flash (the number of the photons produced by the x-ray or gamma photon) it is therefore possible to discern the original photon's energy.
The spectrometer consists of a suitable scintillator crystal, a photomultiplier tube, and a circuit for measuring the height of the pulses produced by the photomultiplier. The pulses are counted and sorted by their height, producing a x-y plot of scintillator flash brightness vs number of the flashes, which approximates the energy spectrum of the incident radiation, with some additional artifacts. A monochromatic gamma radiation produces a photopeak at its energy. The detector also shows response at the lower energies, caused by Compton scattering, two smaller escape peaks at energies 0.511 and 1.022 MeV below the photopeak for the creation of electron-positron pairs when one or both annihilation photons escape, and a backscatter peak. Higher energies can be measured when two or more photons strike the detector almost simultaneously (pile-up, within the time resolution of the data acquisition chain), appearing as sum peaks with energies up to the value of two or more photopeaks added.[4]
The modern electronic scintillation counter was invented in 1944 by Sir Samuel Curran[5][6] whilst he was working on the Manhattan Project at the University of California at Berkeley, and it is based on the work of earlier researchers reaching back to Antoine Henri Becquerel, who is generally credited with discovering radioactivity, whilst working on the phosphorescence of certain uranium salts (in 1896). The Spinthariscope was a early method of detecting the scintillation events by eye.
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リンク元 | 「scintillation counting」 |
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