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Journal articles on the topic 'Radioluminescenza'

Author: Grafiati

Published: 9 March 2023

Last updated: 10 March 2023

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1

Cooper, Daniel R., John A. Capobianco, and Jan Seuntjens. "Radioluminescence studies of colloidal oleate-capped β-Na(Gd,Lu)F4:Ln3+ nanoparticles (Ln = Ce, Eu, Tb)." Nanoscale 10, no. 16 (2018): 7821–32. http://dx.doi.org/10.1039/c8nr01262h.

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2

Shvindin, Mikhail A., and Vadim V. Bakhmetyev. "SYNTHESIS OF ZINC SULFIDE RADIOLUMINESCENT PHOSPHORS WITH USE OF ELECTRONIC BEAM MODIFICATION AND INVESTIGATION OF THEIR PROPERTIES." Bulletin of the Saint Petersburg State Institute of Technology (Technical University) 58 (2021): 46–50. http://dx.doi.org/10.36807/1998-9849-2021-58-84-46-50.

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Synthesized recombination-type zinc sulfide phosphors used in solid-state radioluminescent light sources (SSRLS) are the object of the research. In the course of the study, experimental data were obtained for the first time on the effect of the amount of the incorporated activator on the brightness-spectral characteristics of radioluminescence upon excitation by β-radiation of tritium. Data were obtained on the changes in the radioluminescence parameters under various synthesis conditions, phase composition and electron-beam modification of the crystal structure of the initial phosphors. The results of the work make it possible to find the best light compositions for the use in solid-state radioluminescent light sources

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3

Bai, Tingting, Fei Kang, Shouping Zhu, Xueli Chen, Yihan Wang, and Xu Cao. "Painted radioluminescence imaging with radioluminescent nanophosphors." Applied Physics Letters 121, no. 23 (December 5, 2022): 233701. http://dx.doi.org/10.1063/5.0130428.

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Optical strategies like Cerenkov luminescence imaging (CLI) or radioluminescence imaging (RLI) to image clinically available positron emission tomography and single photon emission computed tomography probes still suffer from low sensitivity or resolution. This study investigated a painted radioluminescence imaging (PRLI) approach that employed a painted scintillator to improve signal and resolution for imaging clinical used 18F-fluorinated deoxyribose (18F-FDG). Results of phantom and in vivo experiments revealed that PRLI could achieve ∼100 times higher signal intensity than CLI and higher resolution compared to Flexible radioluminescence imaging (FRLI), a flexible scintillation-based RLI. PRLI increased signal-to-background ratio in the pseudotumor model by 81.8% (compared to CLI) and 73.9% (compared to FRLI) as well as in the tumor model by 60.0% (compared to CLI) and 33.3% (compared to FRLI). As a conclusion, PRLI is a more effective optical approach for detecting tumors using 18F-FDG.

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Zelenina, Elena V., Vadim V. Bakhmetyev, Maxim М. Sychov, and Mikhail A. Shvindin. "Synthesis and Electron-Beam Modification of Zinc-Sulphide Phosphors for Solid-State Radioluminescent Light Sources (SRLS)." Materials Science Forum 1040 (July 27, 2021): 35–40. http://dx.doi.org/10.4028/www.scientific.net/msf.1040.35.

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Radioluminescence technologies are at the front line of the optic and electronic studies. Effective, self-contained and safe radioluminescent light sources can find their application in space industry, in medicine and in military technologies. The question of the performance improvement of the solid-state radioluminescent light sources (SRLS) without raising the included activity of working radionuclide can be solved by upgrading the phosphor crystalline structure. The electron-beam treatment for zinc-sulphide phosphors initial batch has been studied in a wide range of concentrations of the activating agent (Cu) for improving the radioluminescent performances of the phosphors, for creating the structural defects that form centers of luminescence. The changes of the phase composition were investigated under different synthesis conditions. It is revealed that electron-beam treatment of the initial batch leads to the growth of the wurtzite phase content in zinc-sulphide phosphors synthesized below the phase transition temperature. The changes of the phase content promote the spectral redistribution under the tritium beta-excitation. It is obviously the reflection of the fact of «green» luminescence centers rearrangement between the volume of the crystal and its surface. The correlations between structural configuration and performances of ionizing luminescence were found. Electron beam treatment gave the 20% increase of brightness of the radioluminescence. The achieved enhancement of luminescence performances allows the development of advanced tight-packed SRLS with minimal radioactivity and high energy-light conversion.

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Bakhmetyev, V. V., E. V. Zelenina, and M. A. Shvindin. "Synthesis of ZnS:Cu,Br radioluminescent phosphors using the electron-beam treatment and studying their characteristics." Journal of Physics: Conference Series 2056, no. 1 (October 1, 2021): 012047. http://dx.doi.org/10.1088/1742-6596/2056/1/012047.

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Abstract ZnS:Cu radioluminescent phosphors find their applications in medicine nondestructive testing, safety control and can be used as a part of the solid-state radioluminescent light sources (SRLS). This devices are very promising technology due to their independence longevity and safety compared to the gas-filled RLS. Because of the fact that tritium (the most popular radioisotope for RLS) has a very short range in substances, the improving the operating performances of radiophosphors is a crucial task for SRLS. In our study we used the electron-beam treatment to increase the brightness of radioluminescence of ZnS:Cu phosphors. It was found that bombardment of the phosphors initial charge with electrons of 900 kEv energy improves the brightness of radioluminescence by 15 – 20%. Double modifying of the initial charge and ready phosphor cause the 80% increase of brightness. The effect of electron-beam treatment on the phase content and the surface properties was studied at varying the content of activator (Cu) in the range of 0 – 0.6 % mass. As a result the model describing structure of the acid-base sites on the ZnS:Cu phosphor surface was suggested.

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6

Purbandari, Dessy, Ferdiansjah Ferdiansjah, and Tjipto Sujitno. "Optimization of the Alpha Energy Deposited in Radioluminescence Thin Film for Alphaphotovoltaic Application." Proceeding International Conference on Science and Engineering 2 (March 1, 2019): 41–44. http://dx.doi.org/10.14421/icse.v2.52.

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Activated zinc sulfide (ZnS) is a semiconductor material which able to emit photon in the form of visible light when expose to external energy. The capability of activated ZnS, mainly doped with silver (Ag) and copper (Cu), to convert radiation become light to make it potentially applicable as the radioluminescent thin film for alphaphotovoltaic-type nuclear battery. One of the important specifications of the radioluminescence layer that influences the fluorescence efficiency is the thickness. This work presents a study on the thickness optimization for ZnS:Ag:Cu as the radioluminescent film for alpha particles using Monte Carlo model. Simulation to study alpha particles’ energy deposited by using Stopping and Range of Ions in Matter/TRansport of Ions in Matter (SRIM/TRIM) code. The model examined the transport of 5.485 MeV alpha particles emitted by to determine the best thickness based on energy deposition depth. Based on TRIM module simulation, the optimal thickness for radioluminescence film is approximately 19-22 µm. Most energy from 5.485 MeV alpha particles is deposited in 18.92 µm depth activated zinc sulfide. The results from SRIM/TRIM model then compare with analytical calculation using Bragg-Kleman rule. The alpha particles stop at 22 µm from the SRIM/TRIM simulation while using Bragg-Kleman formula the alpha particles stop at 23.51 µm.

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7

Yamaji, Akihiro, Shunsuke Kurosawa, Akira Suzuki, Jan Pejchal, Kei Kamada, Yuui Yokota, and Akira Yoshikawa. "Optical and Scintillation Properties of Cr Doped Y₃Ga₅O₁₂ Crystal for Infra-Red Scintillators." Key Engineering Materials 616 (June 2014): 92–95. http://dx.doi.org/10.4028/www.scientific.net/kem.616.92.

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We evaluated optical and scintillation properties of a Cr 0.5%:Y3Ga5O12 (YGG) and Cr 0.5%:Y3Al5O12 (YAG) crystals grown by the micro-pulling down method for infrared emission scintillators. In the photoluminescence and X-ray induced radioluminescence measurements, the emissions peaks of Cr:YGG were located in the longer wavelength than those of Cr:YAG. Radioluminescene spectrum of Cr:YGG had a broad peak at 716 nm related to Cr3+2E→4A2 and 4T→4A2 transitions.

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8

Chiodini, N., A. Vedda, and I. Veronese. "Rare Earth Doped Silica Optical Fibre Sensors for Dosimetry in Medical and Technical Applications." Advances in Optics 2014 (October 14, 2014): 1–9. http://dx.doi.org/10.1155/2014/974584.

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Radioluminescence optical fibre sensors are gaining importance since these devices are promising in several applications like high energy physics, particle tracking, real-time monitoring of radiation beams, and radioactive waste. Silica optical fibres play an important role thanks to their high radiation hardness. Moreover, rare earths may be incorporated to optimise the scintillation properties (emission spectrum, decay time) according to the particular application. This makes doped silica optical fibres a very versatile tool for the detection of ionizing radiation in many contexts. Among the fields of application of optical fibre sensors, radiation therapy represents a driving force for the research and development of new devices. In this review the recent progresses in the development of rare earth doped silica fibres for dosimetry in the medical field are described. After a general description of advantages and challenges for the use of optical fibre based dosimeter during radiation therapy treatment and diagnostic irradiations, the features of the incorporation of rare earths in the silica matrix in order to prepare radioluminescent optical fibre sensors are presented and discussed. In the last part of this paper, recent results obtained by using cerium, europium, and ytterbium doped silica optical fibres in radiation therapy applications are reviewed.

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9

Kerst, Thomas, Rikard Malmbeck, Nidhu Banik, and Juha Toivonen. "Alpha Radiation-Induced Luminescence by Am-241 in Aqueous Nitric Acid Solution." Sensors 19, no. 7 (April 2, 2019): 1602. http://dx.doi.org/10.3390/s19071602.

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When exposed to air, alpha particles cause the production of light by exciting the molecules surrounding them. This light, the radioluminescence, is indicative of the presence of alpha radiation, thus allowing for the optical sensing of alpha radiation from distances larger than the few centimeters an alpha particle can travel in air. While the mechanics of radioluminescence in air and other gas compositions is relatively well understood, the same cannot be said about the radioluminescence properties of liquids. Better understanding of the radioluminescence properties of liquids is essential to design methods for the detection of radioactively contaminated liquids by optical means. In this article, we provide radioluminescence images of Am-241 dissolved in aqueous nitric acid ( HNO 3 ) solution and present the recorded radioluminescence spectrum with a maximum between 350 nm and 400 nm , and a steep decrease at the short wavelength side of the maximum. The shape of the spectrum resembles a luminescence process rather than Cerenkov light, bremsstrahlung, or other mechanisms with broadband emission. We show that the amount of light produced is about 150 times smaller compared to that of the same amount of Am-241 in air. The light production in the liquid is evenly distributed throughout the sample volume with a slight increase on the surface of the liquid. The radioluminescence intensity is shown to scale linearly with the Am-241 concentration and not be affected by the HNO 3 concentration.

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10

Mysiura, I. "Photo- and radioluminescence of poleskiy amber." Functional Materials 23, no. 4 (December 20, 2016): 582–86. http://dx.doi.org/10.15407/fm23.04.404.

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11

Santos, D. A. A., E. A. S. Junior, and M. A. Macêdo. "Radioluminescence in ZnO." Radiation Physics and Chemistry 79, no. 5 (May 2010): 612–14. http://dx.doi.org/10.1016/j.radphyschem.2009.12.008.

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12

Прудченко, К. К., И. А. Толкачев, Е. В. Контрош, Е. А. Силантьева, and В. С. Калиновский. "Источник электрической энергии на основе Al-=SUB=-0.8-=/SUB=-Ga-=SUB=-0.2-=/SUB=-As/GaAs фотоэлектрического преобразователя и YPO-=SUB=-4-=/SUB=- : Eu/(-=SUP=-238-=/SUP=-Pu) радиолюминесцентного излучателя." Журнал технической физики 92, no. 12 (2022): 1875. http://dx.doi.org/10.21883/jtf.2022.12.53754.199-22.

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An AlGaAs/GaAs photovoltaic converter for a mock-up of an environmentally friendly radioisotope energy source of ultra-long use with a YPO4:Eu/(238Pu) radioluminescent emitter with an extremely low content of the 238Pu isotope < 0.1 wt.% was studied. The modeling of the Al0.8Ga0.2As/GaAs heterostructure for the conversion of nanowatt power levels of an optical signal has been carried out. The calculated and experimental efficiency of the mock-up with a photovoltaic converter at a radioluminescent source power of 1nW was ~ 1.4%.

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13

Mathis II, Stephan R., Saki T. Golafale, John Bacsa, Alexander Steiner, Conrad W. Ingram, F. Patrick Doty, Elizabeth Auden, and Khalid Hattar. "Mesoporous stilbene-based lanthanide metal organic frameworks: synthesis, photoluminescence and radioluminescence characteristics." Dalton Transactions 46, no. 2 (2017): 491–500. http://dx.doi.org/10.1039/c6dt03755k.

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14

Chiquita, S., R. Pirraco, and C. C. Rosa. "PO-358 BRACHYTHERAPY RADIOLUMINESCENT FIBER SENSOR: SEARCH FOR INFRARED RADIOLUMINESCENT MATERIALS." Radiotherapy and Oncology 103 (May 2012): S144. http://dx.doi.org/10.1016/s0167-8140(12)72324-1.

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15

Chanthima, Natthakridta, Thanapong Sareein, Yaowaluk Tariwong, Jakrapong Kaewkhao, and Narong Sangwaranatee. "Investigations on Luminescence Properties of Ce³⁺ Ion Doped Bismuth Borophosphate Glasses." Applied Mechanics and Materials 879 (March 2018): 22–26. http://dx.doi.org/10.4028/www.scientific.net/amm.879.22.

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Bismuth borophosphate glasses containing different doping cerium oxide have been synthesized at 1200 °C by melt-quenching technique. The doping concentration of the Ce3+ was varied from 0.05 mol% to 2.0 mol%. The glass samples were characterized through optical absorption and luminescence spectral measurements. UV-visible and near infrared absorption spectra of glass samples were not observed nevertheless the absorption edge was shift to the longer wavelength. The photoluminescence and radioluminescence spectra show emission bands around 367 nm under 317 nm excitation wavelength. Also, the highest emission intensity was found at 0.5 mol% CeF3 dopant for both of photoluminescence and radioluminescence.

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16

Zhao, Chen, Jiwei Ren, Lin lei, Feiyi Liao, Kezhao Liu, and Yiying Zhao. "X-ray radioluminescent battery with near milliwatt output power using CsI:Tl single crystal scintillator." Applied Physics Letters 121, no. 12 (September 19, 2022): 123906. http://dx.doi.org/10.1063/5.0109011.

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Low output power has long been the bottleneck of micro-radioisotope batteries as power supplies for the wireless sensor network, implantable medical equipment, and outer space exploration. Recently, x-ray radioluminescent batteries demonstrated the great potential to break the deadlock. In this work, we fabricated an x-ray radioluminescent battery with near milliwatt output power and demonstrated various potential applications. A 100% improvement on the conversion efficiency of 2.46% and the highest output power of 136.1 μW/cm2 were achieved when adopting a thallium doped cesium iodide (CsI:Tl) single-crystal scintillator in the battery. Subsequently, a 2 × 2 battery array was fabricated with a maximum output power of 466.9 μW and was used to power devices including micro-LEDs and a wireless sensor system with temperature monitoring. This demo system shows the feasibility of x-ray radioluminescent batteries as a long-lifetime micropower. The tremendous progress will draw broad attention on micro-nuclear batteries and inspire further exploration on the applications in the field of medical devices, space explorations, and Internet of Things.

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17

Sengupta, Debanti, Tae Jin Kim, Sepideh Almasi, Stuart Miller, Zsolt Marton, Vivek Nagarkar, and Guillem Pratx. "Development and characterization of a scintillating cell imaging dish for radioluminescence microscopy." Analyst 143, no. 8 (2018): 1862–69. http://dx.doi.org/10.1039/c8an00106e.

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18

Venevtsev, Ivan D., Andrey P. Tarasov, Arsen E. Muslimov, Elena I. Gorokhova, Ludmila A. Zadorozhnaya, Piotr A. Rodnyi, and Vladimir M. Kanevsky. "Ultraviolet Luminescence of ZnO Whiskers, Nanowalls, Multipods, and Ceramics as Potential Materials for Fast Scintillators." Materials 14, no. 8 (April 16, 2021): 2001. http://dx.doi.org/10.3390/ma14082001.

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The presented work is dedicated to the study and comparison of scintillating properties of zinc oxide samples prepared in different morphologies: whiskers, nanowalls, multipods, and ceramics. It was shown that total transmittance, photo- and radioluminescence spectra, and radioluminescence kinetics can vary significantly depending on sample structure and preparation conditions. The highest total transmittance was registered for ZnO ceramics (>50% at 0.5 mm thickness). Differences in the transmittance of whiskers, nanowalls, and multipods can be attributed to their shape and thickness which affects the amount of light refraction and scattering. The study of radioluminescence demonstrated that all samples, except undoped ceramics and air annealed whiskers, have predominantly fast luminescence with a decay time <1 ns. High transmittance of ceramics opens the way for their use in the registration of high energy X-ray and gamma radiation, where a large volume of scintillators is required. In cases, where large scintillator thickness is not a necessity, one may prefer to use other ZnO structures, such as ensembles of whiskers and nanowalls. Studies of near-band-edge luminescence components at low temperatures showed that the structure is quite similar in all samples except Ga doped ceramics.

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19

Kherani, N. P., and W. T. Shmayda. "Radioluminescence Using Metal Tritides*." Zeitschrift für Physikalische Chemie 183, Part_1_2 (January 1994): 453–63. http://dx.doi.org/10.1524/zpch.1994.183.part_1_2.453.

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20

Matos, Ivus L. O., Adriano B. Andrade, Zélia S. Macedo, and Mário E. G. Valerio. "Influence of the Uniaxial Hot-Pressing Sintering Condition on Bi4Ge3O12 Ceramic Scintillators." Journal of Spectroscopy 2018 (June 14, 2018): 1–6. http://dx.doi.org/10.1155/2018/5732561.

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The production of high-density bismuth germanate (Bi3Ge4O12) ceramic scintillators by uniaxial hot pressing was investigated as a function of different applied pressure conditions. The X-ray diffraction showed that the sintering process was able to eliminate the undesirable secondary phase present in the nonsintered samples. The height changes from samples with higher applied pressure rate and applied pressure duration lead to a better relative density value, >95% for samples sintered under a pressure of 0.14 and 0.18 MPa. The radioluminescence results showed that all samples have the characteristic emission spectra of Bi3Ge4O12 and that the hot-pressed samples have higher radioluminescence emission efficiency.

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21

Renschler, C. L., J. T. Gill, R. J. Walko, C. S. Ashley, T. J. Shepodd, S. T. Reed, G. M. Malone, L. E. Leonard, R. E. Ellefson, and R. L. Clough. "Solid state radioluminescent lighting." Radiation Physics and Chemistry 44, no. 6 (December 1994): 629–44. http://dx.doi.org/10.1016/0969-806x(94)90223-2.

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22

Děcká, Kateřina, Adéla Suchá, Jan Král, Ivo Jakubec, Martin Nikl, Vítězslav Jarý, Vladimir Babin, Eva Mihóková, and Václav Čuba. "On the Role of Cs4PbBr6 Phase in the Luminescence Performance of Bright CsPbBr3 Nanocrystals." Nanomaterials 11, no. 8 (July 27, 2021): 1935. http://dx.doi.org/10.3390/nano11081935.

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CsPbBr3 nanocrystals have been identified as a highly promising material for various optoelectronic applications. However, they tend to coexist with Cs4PbBr6 phase when the reaction conditions are not controlled carefully. It is therefore imperative to understand how the presence of this phase affects the luminescence performance of CsPbBr3 nanocrystals. We synthesized a mixed CsPbBr3-Cs4PbBr6 sample, and compared its photo- and radioluminescence properties, including timing characteristics, to the performance of pure CsPbBr3 nanocrystals. The possibility of energy transfer between the two phases was also explored. We demonstrated that the presence of Cs4PbBr6 causes significant drop in radioluminescence intensity of CsPbBr3 nanocrystals, which can limit possible future applications of Cs4PbBr6-CsPbBr3 mixtures or composites as scintillation detectors.

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23

Metzner, E., C. Bäumer, C. Behrends, A. Dammene Debbih, D. D. Döhler, M. J. van Goethem, E. R. van der Graaf, et al. "Spectral fiber dosimetry with beryllium oxide for quality assurance in hadron radiation therapy." Journal of Instrumentation 17, no. 02 (February 1, 2022): P02009. http://dx.doi.org/10.1088/1748-0221/17/02/p02009.

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Abstract Using the radioluminescence light of solid state probes coupled to long and flexible fibers for dosimetry in radiotherapy offers many advantages in terms of probe size, robustness and cost efficiency. However, especially in hadron fields, radioluminophores exhibit quenching effects dependent on the linear energy transfer. This work describes the discovery of a spectral shift in the radioluminescence light of beryllium oxide in dependence on the residual range at therapeutic proton energies. A spectrally resolving measurement setup has been developed and tested in scanned proton fields. It is shown that such a system can not only quantitatively reconstruct the dose, but might also give information on the residual proton range at the point of measurement.

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24

Lu, Hao, Xieming Xu, Guiqing Feng, Baoping Sun, Shuaihua Wang, and Shaofan Wu. "Terbium doped LiLuF₄ nanocrystal scintillator-based flexible composite film for high resolution X-ray imaging." RSC Advances 12, no. 8 (2022): 4615–23. http://dx.doi.org/10.1039/d1ra08989g.

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25

Pagliazzi, Marco, Federico Boschi, and Antonello E. Spinelli. "Imaging of luminescence induced by beta and gamma emitters in conventional non-scintillating materials." RSC Adv. 4, no. 26 (2014): 13687–92. http://dx.doi.org/10.1039/c3ra47102k.

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26

Du, Ying, Lu Deng, and Danping Chen. "Ag Nanocluster-Enhanced Scintillation Properties of Borophosphate Glasses Doped with CsPbBr3 Quantum Dots." Materials 15, no. 15 (July 26, 2022): 5187. http://dx.doi.org/10.3390/ma15155187.

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A novel and effective method to improve scintillation properties of glass-ceramics, such as intensity enhancement and decay-time shortening, is reported in this work. Compared with crystal scintillators, glass scintillators always have the problems of low efficiency and long decay; how to solve them has always been a scientific puzzle in the field of scintillation glass-ceramics. The plasma enhancement effect can be predicted to solve the above problems. Ag+ ions were diffused into glasses by ion exchange, and then Ag nanoparticles and CsPbBr3 quantum dots were formed by heat treatment. The structure of the CsPbBr3 perovskite consists of a series of shared corner PbBr6 octahedra with Cs ions occupying the cuboctahedral cavities. By using Ag and the plasma resonance effect, the photoluminescence intensity of CsPbBr3 quantum dot glasses was enhanced by 3 times, its radioluminescence intensity increased by 6.25 times, and its decay time was reduced by a factor of more than one. Moreover, the mechanism of photoluminescence and radioluminescence enhanced by Ag and plasma was discussed based on the experimental results and finite-difference time-domain method. We concluded that the increase in radioluminescence intensity was related to plasma enhancements and the energy exchange between Ag nanoclusters and CsPbBr3 quantum dots. Doping Ag is a valid means to improve the scintillation luminescence of CsPbBr3 quantum dot glasses, which can be applied in the field of scintillation.

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27

Li, Xiaolong, Zhenluan Xue, Mingyang Jiang, Youbin Li, Songjun Zeng, and Hongrong Liu. "Soft X-ray activated NaYF4:Gd/Tb scintillating nanorods for in vivo dual-modal X-ray/X-ray-induced optical bioimaging." Nanoscale 10, no. 1 (2018): 342–50. http://dx.doi.org/10.1039/c7nr02926h.

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Soft X-ray-activated NaYF₄:Gd/Tb nanoprobes with efficient green radioluminescence and good biocompatibility were developed for simultaneous X-ray imaging and X-ray-induced optical bioimaging.

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28

Frangville, Camille, Matthieu Hamel, Guillaume H. V. Bertrand, Eva Montbarbon, Amélie Grabowski, and Clément Lynde. "Large solubility of lithium carboxylates reaching high rates of 6Li incorporation in polystyrene-based plastic scintillators for fast/thermal neutron and gamma ray detection." Materials Chemistry Frontiers 3, no. 8 (2019): 1626–31. http://dx.doi.org/10.1039/c9qm00153k.

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29

Belmont-Moreno, E., A. Menchaca-Rocha, M. E. Brandan, J. Hernandez A, M. Gonin, K. Hagel, R. Wada, and J. B. Natowitz. "Radioluminescence study in KI(Eu)." Radiation Effects and Defects in Solids 118, no. 2 (November 1991): 185–89. http://dx.doi.org/10.1080/10420159108220634.

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30

Tirskiĭ, V. V., and E. F. Martynovich. "Intraband radioluminescence of LiF crystals." Optics and Spectroscopy 88, no. 4 (April 2000): 533–37. http://dx.doi.org/10.1134/1.626833.

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31

Chithambo, M. L., and P. Niyonzima. "Radioluminescence of annealed synthetic quartz." Radiation Measurements 106 (November 2017): 35–39. http://dx.doi.org/10.1016/j.radmeas.2017.02.005.

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32

Moreira, Mário L., Diogo P. Volanti, Juan Andrés, Paulo J. R. Montes, Mário E. G. Valerio, José A. Varela, and Elson Longo. "Radioluminescence properties of decaoctahedral BaZrO3." Scripta Materialia 64, no. 2 (January 2011): 118–21. http://dx.doi.org/10.1016/j.scriptamat.2010.09.017.

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33

Brovetto, P., V. Maxia, F. Quarati, and M. Salis. "Radioluminescence investigation of Nasicon materials." Materials Research Bulletin 35, no. 11 (August 2000): 1797–803. http://dx.doi.org/10.1016/s0025-5408(00)00389-5.

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34

Moroño, A., and E. R. Hodgson. "Radioluminescence problems for diagnostic windows." Journal of Nuclear Materials 224, no. 3 (September 1995): 216–21. http://dx.doi.org/10.1016/0022-3115(95)00082-8.

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35

Coy-Yll, R., T. Calderon, and M. Aguilar. "Thermoluminescence and radioluminescence in aragonite." Mineralogy and Petrology 39, no. 1 (September 1988): 39–53. http://dx.doi.org/10.1007/bf01226261.

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36

Nowotny, R. "Radioluminescence of some optical fibres." Physics in Medicine and Biology 52, no. 4 (January 30, 2007): N67—N73. http://dx.doi.org/10.1088/0031-9155/52/4/n01.

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37

Appleton, W. R. Simon, and Brian Brocklehurst. "Radioluminescence of cyclohexane-benzene mixtures." International Journal of Radiation Applications and Instrumentation. Part C. Radiation Physics and Chemistry 32, no. 2 (January 1988): 245–49. http://dx.doi.org/10.1016/1359-0197(88)90193-2.

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38

Yang, Dandan, Zhiheng Xu, Chunhui Gong, Lin Su, Xiaoming Li, Xiaobin Tang, Dongling Geng, Cuifang Meng, Feng Xu, and Haibo Zeng. "Armor-like passivated CsPbBr3 quantum dots: boosted stability with hand-in-hand ligands and enhanced performance of nuclear batteries." Journal of Materials Chemistry A 9, no. 13 (2021): 8772–81. http://dx.doi.org/10.1039/d0ta12365j.

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An armor-like passivation strategy is developed to improve luminous efficiency, storage stability, water resistance and irradiation stability of PQDs. Moreover, PQDs as the transducer component are used in radioluminescent nuclear battery.

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39

Marazuev, Yu A., A. B. Brik, and V. Ya Degoda. "Radioluminescent dosimetry of α-quartz." Radiation Measurements 24, no. 4 (October 1995): 565–69. http://dx.doi.org/10.1016/1350-4487(95)00278-m.

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40

Zhou, Quan, Jiwei Ren, Jiawen Xiao, Lin Lei, Feiyi Liao, Haipeng Di, Chao Wang, et al. "Highly efficient copper halide scintillators for high-performance and dynamic X-ray imaging." Nanoscale 13, no. 47 (2021): 19894–902. http://dx.doi.org/10.1039/d1nr03996b.

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The β-Cs3Cu2Cl5 nanocrystals were developed as high-performance scintillators, which showed a PLQY of 94.6% and a radioluminescence light yield of ∼34000 photons per MeV. A high spatial resolution in the X-ray imaging results was demonstrated.

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41

Zelenina, E. V., E. A. Pechertseva, V. V. Bakhmetyev, and M. M. Sychov. "ADVANCED TECHNOLOGY OF LUMINOPHOR SCREENS FOR SOLID RADIOLUMINESCENT LIGHT SOURCES." Doklady BGUIR, no. 7 (125) (December 7, 2019): 59–66. http://dx.doi.org/10.35596/1729-7648-2019-125-7-59-66.

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The article observes different methods of coating the phosphor screens on the tritiated titanium matrices for creating the solid-state radioluminescent light sources (SRLS). Technology of SRLS is alternative to the existing technology of the gas-filled radioluminescent light sources. The main idea of SRLS is in bonding the working isotope (tritium) in the solid matrix and combining it with the phosphor. The key problem of SRLS is to provide the closest contact between the tritiated carrier matrix and phosphor screen. The basic requirements for the phosphor screens for SRLS would be the strength of fixation on the plate, uniformity and radiological and thermal stability. There have been made a comparison of various techniques of coating and fixing the phosphor screens by their effect on spectral and brightness characteristics of SRLS. The improved sol-gel technique of suspended sedimentation of phosphor screen from the potassium water glass binder solution was developed. The composition of the solution was established experimentally and we get the strong and uniform experimental prototypes of the glass coated phosphor screens of various thickness. The developed technology allows to deposit the strong and uniform phosphor coatings without using any additional dispersing agents. Screen thickness regulates by the amount of phosphor in the suspension. Also the optimal thickness of the phosphor screen, giving the maximum luminescence intensity was determined. The two laboratory prototypes of solid-state radioluminescent light sources were manufactured by coating the phosphor directly on the tritium β-source.

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42

Ouyang, Xiao, Richeng Lin, Ying Ding, Yali Liang, Wei Zheng, Liang Chen, Xiaojing Song, Feng Huang, and Xiaoping Ouyang. "Efficient sky-blue radioluminescence of microcrystalline Cs3Cu2I5 based large-scale eco-friendly composite scintillators for high-sensitive ionizing radiation detection." Materials Chemistry Frontiers 5, no. 12 (2021): 4739–45. http://dx.doi.org/10.1039/d1qm00356a.

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A high-efficiency sky-blue radioluminescence, large-size, eco-friendly hybrid scintillator made of CsI:Na and Cs₃Cu₂I₅ single crystals is expected to become a potential ionizing radiation detection scintillator.

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43

Volkova, L. V., E. A. Borisova, and R. N. Nurmukhametov. "Determination of Optical Centers of Emission in a Plastic Scintillator Irradiated by UV-laser." Izvestiya MGTU MAMI 3, no. 1 (January 10, 2009): 114–18. http://dx.doi.org/10.17816/2074-0530-69947.

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Photoprocesses in a plastic scintillator irradiated by UV-laser were studied. The spectral properties and structure of photoproducts in irradiated plastic scintillator were found. The mechanism of photochemical processes leading to radioluminescence signal decrease in the scintillator during its usage has been suggested

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44

Mikhal’chenko, A. G. "Properties of radioluminescence sources for photometry." Journal of Optical Technology 78, no. 7 (July 30, 2011): 452. http://dx.doi.org/10.1364/jot.78.000452.

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45

Khanlary, M. R., P. D. Townsend, and J. E. Townsend. "Radioluminescence response of germanosilicate optical fibres." Radiation Effects and Defects in Solids 127, no. 1 (July 1993): 47–59. http://dx.doi.org/10.1080/10420159308219897.

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46

Martini, M., M. Fasoli, I. Villa, and P. Guibert. "Radioluminescence of synthetic and natural quartz." Radiation Measurements 47, no. 9 (September 2012): 846–50. http://dx.doi.org/10.1016/j.radmeas.2012.01.008.

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47

Kirsh, Y., I. Schnitzer, and P. Townsend. "Radioluminescence of silver halide optical fibers." Journal of the Optical Society of America B 6, no. 2 (February 1, 1989): 146. http://dx.doi.org/10.1364/josab.6.000146.

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Krbetschek, M. R., T. Trautmann, A. Dietrich, and W. Stolz. "Radioluminescence dating of sediments: methodological aspects." Radiation Measurements 32, no. 5-6 (December 2000): 493–98. http://dx.doi.org/10.1016/s1350-4487(00)00122-0.

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49

Wu, Z., B. Yang, and P. D. Townsend. "Low temperature radioluminescence spectra of CsI:Tl." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 266, no. 21 (November 2008): 4757–61. http://dx.doi.org/10.1016/j.nimb.2008.07.015.

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50

Petö, Á., A. Kelemen, and N. Ötvös. "Radioluminescence characteristics of CaSO4:Dy,Cu." Journal of Luminescence 72-74 (June 1997): 778–80. http://dx.doi.org/10.1016/s0022-2313(96)00356-0.

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