ライフサイエンスコーパス: scintillator

1 ntium-90 ((90)Sr) radionuclide and a plastic scintillator.

2 n ABS plastic probe that retains the LYSO:Ce scintillator.

3 tions of individual photons emitted from the scintillator.

4 d detection system based on an organic glass scintillator.

5 Center-of-Mass of the interaction within the scintillator.

6 ement in light yield compared to unpatterned scintillators.

7 scalable, low-cost, and fast-response X-ray scintillators.

8 ly polarized light-emitting diodes and X-ray scintillators.

9 of a new generation of nanophotonic-enhanced scintillators.

10 as-filled proportional counters(6) and light scintillators(7) for thermalized neutrons.

11 of registering spots of light emitted by the scintillator after a particle interaction, allowing to r

12 rall, the proposed event-based evaluation of scintillators allows for quantifying and optimizing vari

13 erformance liquid chromatography with a flow scintillator analyzer and liquid scintillation counting

14 of gamma-rays by changing the combination of scintillator and beam filter used at the NECTAR instrume

15 ns close to the decay origin through a CdWO4 scintillator and does not use any optical elements.

16 While different types of scintillator and sensor configurations exist, it can be

17 posed of 200 bismuth germanium oxide crystal scintillators and 393 channel silicon photomultipliers h

18 ponent level there have been improvements in scintillators and photon transducers as well as a greate

19 ight (lambda(max) = 435 nm) from the plastic scintillator, and the blue light excites the analyte-res

20 rection, imaging of gamma rays using organic scintillators, and imaging of multiple sources in the sa

21 Intrinsic GaN-based neutron scintillators are demonstrated via the intrinsic (14)N(n

22 Scintillators are used in combination with a camera syst

23 Organic scintillators are used within radiation portal monitors

24 hosilicate crystals and full coverage of the scintillator area.

25 Each scintillator array was coupled at the nonreadout side to

26 les of a 26 x 26 pixelated bismuth germanate scintillator array with individual crystals measuring 1.

27 multicrystal lutetium yttrium orthosilicate scintillator arrays directly coupled 4-to-1 and 9-to-1 t

28 They are scintillator based detectors that detect the scintillati

29 tector compared to more established types of scintillator based neutron detectors.

30 X-ray imaging tests show that scintillators based on (C(38)H(34)P(2))MnBr(4) powders p

31 rt for the first time high-performance X-ray scintillators based on facile, solution-processed amorph

32 brication method for large-area nanophotonic scintillators based on the self-assembly of chalcogenide

33 , marking a step-change in opportunities for scintillator-based applications.

34 first is a position sensitive ZnS:Ag/(6)LiF scintillator-based detector coupled with wavelength shif

35 n fast neutron resonance radiography using a scintillator-based event-mode imaging detector at a shor

36 mponents that sets it apart from established scintillator-based imaging detectors.

37 the detection efficiency and resolution of a scintillator-based system strongly depend on the scintil

38 -5-phenyloxazole, (2) a mixed bed of organic scintillator (BC-400) and Tc-selective resin (TEVA), and

39 utron capture as state-of-the art commercial scintillators, but with the advantage of much lower cost

40 ay radiography, and high resolution flexible scintillators can be fabricated by blending (C(38)H(34)P

41 ng media investigated were (1) an extractive scintillator combining a porous polystyrene resin with t

42 shell heterostructures as X-ray and electron scintillators, combining efficiency, speed, and durabili

43 Scintillators convert X-ray energy into visible light an

44 In this imaging technique, a scintillator crystal (e.g., CdWO4) is placed in close pr

45 Scintillator crystal arrays are made from 22 x 10 and 21

46 A recently developed scintillator crystal, cerium-doped lutetium oxyorthosili

47 comparing two common high-resolution neutron scintillators, crystalline Gadolinium Gallium Garnet (GG

48 In PET, inorganic scintillator crystals are used to record gamma-rays prod

49 ccessfully used to read out large numbers of scintillator crystals coupled through optical fibers wit

50 rchers have investigated virtually all known scintillator crystals for possible use in PET.

51 Epitaxial quantum dot (QD) scintillator crystals with picosecond-scale timing and h

52 to arrays of lutetium oxyorthosilicate (LSO) scintillator crystals.

53 of 2 square (10 x 10 cm) arrays of discrete scintillator crystals.

54 We design a thin multilayer nanophotonic scintillator, demonstrating Purcell-enhanced scintillati

55 potential for utilising a WLSF ZnS:Ag/(6)LiF scintillator detector and a pixelated GS20 detector for

56 ion and detection using a flow-through solid scintillator detector.

57 lutetium-yttrium oxyorthosilicate inorganic scintillators detector elements with light collection vi

58 omparable or better resolution than standard scintillator detectors is collected under a small electr

59 A detector prototype using GS20 glass scintillator directly coupled to a multi-anode photomult

60 ission, which usually governs and limits the scintillator emission rate and light yield.

61 ed photodetectors, solar cells, transistors, scintillators, etc.

62 sing a low-background, 14.6-kilogram CsI[Na] scintillator exposed to the neutrino emissions from the

63 Nanophotonic scintillators, featuring wavelength-scale nanostructures

64 nting mode and an indirect detection sensor (scintillator/fiber-optic/CCD) for electron energy-loss s

65 trate the feasibility of an ultrafast PbI(2) scintillator for temperature determination, using the ti

66 er for evaluation of materials to be used as scintillators for high quality X-ray detection and imagi

67 Efficient, fast, and robust scintillators for ionizing radiation detection are cruci

68 dimensional hybrid perovskite single-crystal scintillators grown inside microcapillary channels as sm

69 The Cherenkov emission in inorganic crystal scintillators has been shown to dramatically improve tim

70 While numerous 0D OMHH scintillators have been developed to date, most of them

71 assive research effort, only a few different scintillators have been found that have a suitable combi

72 The sensor tips consist of inorganic scintillators, i.e. Gd(2)O(2)S:Tb for LDR-BT, and Y(2)O(

73 These results indicate GaN scintillator is a suitable candidate neutron detector in

74 coupled with a [Formula: see text]LiF-ZnS:Ag scintillator is applied for neutron resonance imaging (N

75 Imaging using scintillators is a widespread and cost-effective approac

76 sed devices, including photodetectors, X-ray scintillators, lasers, and high-brightness light-emittin

77 ray detector with a structured cesium iodide scintillator layer and an amorphous silicon thin-film tr

78 ss substrate with a structured cesium iodide scintillator layer and an amorphous silicon thin-film tr

79 This is the first PET scanner to use the new scintillator LSO and uses a novel detector design to ach

80 used a fully 3-dimensional scanner with the scintillator lutetium-yttrium oxyorthosilicate and a sys

81 Prototype catheters, using a plastic scintillator mated to an optical fiber, have been tested

82 tillator-based system strongly depend on the scintillator material and its thickness.

83 trinsic radioactivity within the LSO crystal scintillator material.

84 ole-body imaging, 3-dimensional imaging, new scintillator materials, iterative reconstruction algorit

85 te with that of a commercial inorganic X-ray scintillator (NaI:Tl).

86 nique enables the production of nanophotonic scintillators over wafer-scale areas, achieving a six-fo

87 ion of FAR CLI is challenging because of the scintillator overlay.

88 sin (TEVA), and (3) a mixed bed of inorganic scintillator particles (CaF2-Eu) with either TEVA resin

89 veguiding crystal and allows a wide range of scintillator-photodetector coupling geometries.

90 uclide imaging by incorporating an inorganic scintillator plate (CdWO(4)) into a microfluidic chip.

91 , live cells are cultured sparsely on a thin scintillator plate and incubated with a radiotracer.

92 emitted during radioactive decay, traverse a scintillator plate placed below the cells.

93 Both scintillators reach similar resolution (4-5 mu m) in eve

94 s been realized by using a neutron sensitive scintillator read out by a single-photon sensitive camer

95 For decades, scintillator research focused on developing faster-emitt

96 how prospects for bridging nanophotonics and scintillator science toward reduced radiation dosage and

97 At the same time, the use of a thick scintillator screen and lenses to focus the produced lig

98 ble to utilize them by using gamma sensitive scintillator screens in place of the neutron sensitive s

99 g results of a camera constructed using this scintillator show Modulation Transfer Function values si

100 this identification capability using organic scintillators (stilbene crystals and EJ-309 liquid scint

101 on from the hydrogen atom, using the plastic scintillator target of the MINERvA(11) experiment, extra

102 However, traditional scintillator technologies face challenges in simultaneou

103 e developed a unified theory of nanophotonic scintillators that accounts for the key aspects of scint

104 of the favorable timing properties of newer scintillators; the integration of PET and MRI scanners i

105 therefore provides a pathway to overcome the scintillator thickness limitation and increase the effec

106 practical applicability of our nanophotonic scintillators through X-ray imaging of biological and in

107 used to load neutrons into the trap and as a scintillator to detect their decay.

108 on integrating nanophotonic structures into scintillators to enhance their emission, obtaining nearl

109 MOF materials thus serve as efficient X-ray scintillators via synergistic X-ray absorption by the me

110 or screens in place of the neutron sensitive scintillators, viewed by the same camera based detector

111 Nanostructured ZnO scintillators were rearranged to form a vertically well-

112 llators (stilbene crystals and EJ-309 liquid scintillators), which do not provide direct, high-resolu

113 elatively slow [Formula: see text]LiF-ZnS:Ag scintillator, which may not be optimal for absorption re

114 oupled to the ends of eight stilbene organic scintillators, which have an overall volume of 5.74 x 5.

115 The device couples a LYSO:Ce scintillator with a photodetector via a polymer optical

116 on emission tomography (TOF-PET) for in slow scintillators with a high refractive index such as bismu

117 The introduction of fast scintillators with good stopping power for 511-keV photo

118 s (176)Lu background radiation from detector scintillators with low-count PET data.

119 Here, we report highly efficient X-ray scintillators with state-of-the-art performance based on

120 s of brighter, faster, and higher-resolution scintillators with tailored and optimized performance.