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Scintillation counter

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430: 476: 20: 164: 204:. This group of primary electrons is electrostatically accelerated and focused by an electrical potential so that they strike the first dynode of the tube. The impact of a single electron on the dynode releases a number of secondary electrons which are in turn accelerated to strike the second dynode. Each subsequent dynode impact releases further electrons, and so there is a current amplifying effect at each dynode stage. Each stage is at a higher potential than the previous to provide the accelerating field. 438: 176: 369: 219:
The scintillator must be shielded from all ambient light so that external photons do not swamp the ionization events caused by incident radiation. To achieve this a thin opaque foil, such as aluminized mylar, is often used, though it must have a low enough mass to minimize undue attenuation of the
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The chemistry of atomic de-excitation in the scintillator produces a multitude of low-energy photons, typically near the blue end of the visible spectrum. The quantity is proportional to the energy deposited by the ionizing particle. These can be directed to the photocathode of a photomultiplier
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monitors, for area or personal surveys require a large detection area to ensure efficient and rapid coverage of monitored surfaces. For this a thin scintillator with a large area window and an integrated photomultiplier tube is ideally suited. They find wide application in the field of radioactive
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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
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A scintillator 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, This technique is used in
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contamination monitoring of personnel and the environment. Detectors are designed to have one or two scintillation materials, depending on the application. "Single phosphor" detectors are used for either alpha or beta, and "Dual phosphor" detectors are used to detect both.
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The resultant output signal at the anode is a measurable pulse for each group of photons from an original ionizing event in the scintillator that arrived at the photocathode and carries information about the energy of the original incident radiation. When it is fed to a
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When an ionizing particle passes into the scintillator material, atoms are excited along a track. For charged particles the track is the path of the particle itself. For gamma rays (uncharged), their energy is converted to an energetic electron via either the
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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
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The number of such pulses per unit time also gives information about the intensity of the radiation. In some applications individual pulses are not counted, but rather only the average current at the anode is used as a measure of radiation intensity.
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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
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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
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Scintillation counters are widely used in radiation protection, assay of radioactive materials and physics research because they can be made inexpensively yet with good
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Measurement of gamma ray spectrum with a scintillation counter. A high voltage drives the counter which feeds signals to the Multichannel Analyser (MCA) and computer.
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Scintillation materials are used for ambient gamma dose measurement, though a different construction is used to detect contamination, as no thin window is required.
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which integrates the energy information, an output pulse is obtained which is proportional to the energy of the particle exciting the scintillator.
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both hand-held and fixed monitoring equipment, and such instruments are relatively inexpensive compared with the gas proportional detector.
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Scintillation probe being used to measure surface radioactive contamination. The probe is held as close to the object as practicable
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of input energy is fairly constant. By measuring the intensity of the flash (the number of the photons produced by the
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Hand-held scintillation counter reading ambient gamma dose. The position of the internal detector is shown by the cross
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Schematic showing incident high energy photon hitting a scintillating crystal, triggering the release of low-energy
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Hand-held large area alpha scintillation probe under calibration with a plate source in a bench calibration jig.
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peak. Higher energies can be measured when two or more photons strike the detector almost simultaneously (
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of uranium salts in 1896. Previously, scintillation events had to be laboriously detected by eye, using a
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Scintillation counters are used to measure radiation in a variety of applications including hand held
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Glenn F Knoll. Radiation Detection and Measurement, third edition 2000. John Wiley and sons,
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chain), appearing as sum peaks with energies up to the value of two or more photopeaks added
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Instrumentation Between Science, State and Industry (Sociology of the Sciences Yearbook, 22)
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detectors, high efficiency is gained through the use of scintillating materials rich in
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to accurately count the flashes of light from a scintillator subjected to radiation.
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or gamma photon) it is therefore possible to discern the original photon's energy.
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into high number of lower-energy photons, where the number of photons per
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tube which emits at most one electron for each arriving photon due to the
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animation of radiation scintillation counter using a photomultiplier tube.
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which generates photons in response to incident radiation, a sensitive
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The first electronic scintillation counter was invented in 1944 by
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is used as a scintillator for the detection of gamma waves and
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in the detector, and certain scintillating materials, such as
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of some of the elements of which they are composed. However,
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tube carries a detailed description of the tube's operation.
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This built upon the work of earlier researchers such as
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are an efficient and practical means of quantifying
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material, and detecting the resultant light pulses.
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Hand-held units are also commonly used. 797: 672:"Automatic Radiation Detection Vehicles" 502:The spectrometer consists of a suitable 474: 436: 428: 367: 280: 174: 167:Apparatus with a scintillating crystal, 162: 18: 750: 748: 746: 630: 620:Oxford Dictionary of National Biography 598:Counting tubes, theory and applications 419: 1176: 594: 230: 1114:Radiation Protection Convention, 1960 771: 483:Scintillators often convert a single 143:which were used in metabolic studies 743: 700: 527:, within the time resolution of the 464: 277:(LiI) is used in neutron detectors. 106:University of California at Berkeley 265:(NaI) containing a small amount of 220:incident radiation being measured. 13: 171:, and data acquisition components. 50:effect of incident radiation on a 14: 1210: 322:detectors based on semiconductors 251:) that fluoresces when struck by 363: 881:Computed tomography dose index 682: 664: 646: 624: 613: 588: 27:which are then converted into 1: 715:Health & Safety Executive 689:Portable MicroR Survey Meters 581: 576:Total absorption spectroscopy 551:Liquid scintillation counting 354:Liquid scintillation counters 249:liquid scintillation counting 100:whilst he was working on the 1194:Ionising radiation detectors 425:Alpha and beta contamination 296:The quantum efficiency of a 158: 114:Radio Corporation of America 7: 534: 414:Health and Safety Executive 10: 1215: 1145: 631:Joerges, Bernward (2001). 595:Curran, Samuel C. (1949). 468: 456: 335: 284: 91: 1143: 1122: 1091: 1040: 1004: 939: 856: 838:Radioactive contamination 805: 446:Radioactive contamination 386:radioactive contamination 1146:See also the categories 1135:Radiation-induced cancer 1130:Acute radiation syndrome 382:environmental monitoring 291: 404:Diffusion cloud chamber 378:radiation survey meters 121:Antoine Henri Becquerel 88:of incident radiation. 986:Semiconductor detector 942:measurement techniques 480: 442: 434: 373: 352:neutrons efficiently. 330:gamma-ray spectrometry 180: 172: 127:whilst working on the 35: 31:and multiplied in the 1005:Protection techniques 969:Scintillation counter 478: 440: 432: 371: 281:Detector efficiencies 178: 166: 71:charge-coupled device 40:scintillation counter 22: 1199:Radiation protection 1164:Radiation protection 981:Radiation monitoring 974:Proportional counter 859:quantities and units 813:Background radiation 799:Radiation protection 420:Radiation protection 324:, notably hyperpure 202:photoelectric effect 186:photoelectric effect 996:Whole-body counting 906:Mean glandular dose 843:Radioactive sources 287:Counting efficiency 231:Detection materials 223:The article on the 73:(CCD) camera, or a 1184:Particle detectors 833:Internal dosimetry 828:Ionizing radiation 694:2009-12-07 at the 561:Pandemonium effect 541:Gamma spectroscopy 517:Compton scattering 481: 471:Gamma spectroscopy 443: 435: 374: 253:ionizing radiation 190:Compton scattering 181: 173: 123:, who discovered 112:tubes made by the 82:quantum efficiency 44:ionizing radiation 36: 1171: 1170: 1152:Radiation effects 1123:Radiation effects 886:Counts per minute 465:As a spectrometer 398:radioactive waste 314:bismuth germanate 102:Manhattan Project 98:Sir Samuel Curran 57:It consists of a 1206: 1027:Radon mitigation 1022:Potassium iodide 940:Instruments and 792: 785: 778: 769: 768: 762: 752: 741: 740: 734: 726: 724: 722: 712: 704: 698: 686: 680: 679: 674:. 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Index


photons
photoelectrons
photomultiplier
ionizing radiation
excitation
scintillating
scintillator
photodetector
photomultiplier
charge-coupled device
photodiode
quantum efficiency
energy
Sir Samuel Curran
Manhattan Project
University of California at Berkeley
photomultiplier
Radio Corporation of America
Antoine Henri Becquerel
radioactivity
phosphorescence
spinthariscope
tritium
carbon-14
in vivo
in vitro

photomultiplier

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