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1 ntium-90 ((90)Sr) radionuclide and a plastic scintillator.
3 ponent level there have been improvements in scintillators and photon transducers as well as a greate
4 ight (lambda(max) = 435 nm) from the plastic scintillator, and the blue light excites the analyte-res
5 -5-phenyloxazole, (2) a mixed bed of organic scintillator (BC-400) and Tc-selective resin (TEVA), and
6 utron capture as state-of-the art commercial scintillators, but with the advantage of much lower cost
7 ng media investigated were (1) an extractive scintillator combining a porous polystyrene resin with t
12 ccessfully used to read out large numbers of scintillator crystals coupled through optical fibers wit
17 omparable or better resolution than standard scintillator detectors is collected under a small electr
18 sing a low-background, 14.6-kilogram CsI[Na] scintillator exposed to the neutrino emissions from the
19 nting mode and an indirect detection sensor (scintillator/fiber-optic/CCD) for electron energy-loss s
20 assive research effort, only a few different scintillators have been found that have a suitable combi
21 ray detector with a structured cesium iodide scintillator layer and an amorphous silicon thin-film tr
22 ss substrate with a structured cesium iodide scintillator layer and an amorphous silicon thin-film tr
23 This is the first PET scanner to use the new scintillator LSO and uses a novel detector design to ach
24 used a fully 3-dimensional scanner with the scintillator lutetium-yttrium oxyorthosilicate and a sys
27 ole-body imaging, 3-dimensional imaging, new scintillator materials, iterative reconstruction algorit
28 sin (TEVA), and (3) a mixed bed of inorganic scintillator particles (CaF2-Eu) with either TEVA resin
29 , live cells are cultured sparsely on a thin scintillator plate and incubated with a radiotracer.
31 of the favorable timing properties of newer scintillators; the integration of PET and MRI scanners i
33 MOF materials thus serve as efficient X-ray scintillators via synergistic X-ray absorption by the me
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