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1 ntium-90 ((90)Sr) radionuclide and a plastic scintillator.
2 ns close to the decay origin through a CdWO4 scintillator and does not use any optical elements.
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
8                 In this imaging technique, a scintillator crystal (e.g., CdWO4) is placed in close pr
9                                              Scintillator crystal arrays are made from 22 x 10 and 21
10                         A recently developed scintillator crystal, cerium-doped lutetium oxyorthosili
11                            In PET, inorganic scintillator crystals are used to record gamma-rays prod
12 ccessfully used to read out large numbers of scintillator crystals coupled through optical fibers wit
13 rchers have investigated virtually all known scintillator crystals for possible use in PET.
14 to arrays of lutetium oxyorthosilicate (LSO) scintillator crystals.
15  of 2 square (10 x 10 cm) arrays of discrete scintillator crystals.
16 ion and detection using a flow-through solid scintillator detector.
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
25         Prototype catheters, using a plastic scintillator mated to an optical fiber, have been tested
26 trinsic radioactivity within the LSO crystal scintillator material.
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.
30 emitted during radioactive decay, traverse a scintillator plate placed below the cells.
31  of the favorable timing properties of newer scintillators; the integration of PET and MRI scanners i
32 used to load neutrons into the trap and as a scintillator to detect their decay.
33  MOF materials thus serve as efficient X-ray scintillators via synergistic X-ray absorption by the me
34                     The introduction of fast scintillators with good stopping power for 511-keV photo

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