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Journal articles on the topic 'Thermoluminescence'

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Published: 4 June 2021
Last updated: 28 July 2024

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1

Chandra, B. P., V. K. Chandra, and Piyush Jha. "Elastico-Mechanoluminescence of Thermoluminescent Crystals." Defect and Diffusion Forum 347 (December 2013): 139–77. http://dx.doi.org/10.4028/www.scientific.net/ddf.347.139.

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Elastico-mechanoluminescence (EML) is a type of luminescence induced by elastic deformation of solids. The present paper reports the elastic-ML of thermoluminescent crystals such as X-or γ-irradiated alkali halide crystals, ZnS:Mn, and ultraviolet irradiated persistent luminescent crystals. Generally, all the elastico-mechanoluminescent crystals are thermoluminescent, but all the thermoluminescent crystals are not the mechanoluminescent. The elastico-mechanoluminescence spectra of crystals are similar to their thermoluminescence spectra. Both the elastico-mechanoluminescence and thermoluminescence arise due to the de-trapping of charge carriers. As elastico-ML of persistent luminescent crystals depends on both the density of filled traps and piezoelectric field, the intense thermoluminescent crystals may not be the intense mechanoluminescent crystals. When a sample of X-or γ-irradiated alkali halide crystal, UV-irradiated persistent luminescent microcrystals mixed in epoxy resin, or a film of ZnS:Mn nanoparticles is deformed in the elastic region by the pressure rising at fixed pressing rate for a particular time, or by a pressure of triangular form, or by a pressure pulse, then after a threshold pressure, initially the EML intensity increases with time, attains a maximum value and later on it decreases with time. In the first case, the fast decay time of EML is related to the time-constant for stopping the moving crosshead of the testing machine; in the second case, generally the fast decay does not appear; and in the third case, the fast decay time is equal to the rise time of the pressure pulse. However, in all the cases, the slow decay time is related to the lifetime of re-trapped charge carriers in the shallow traps lying in the region where the piezoelectric field is negligible. When the sample is deformed by the pressure rising at fixed pressing rate for a particular time, or pressure of triangular form, then the ML appears after a threshold pressure and the transient EML intensity increases linearly with the applied pressure; however, the total EML intensity increases quadratically with the applied pressure. The EML intensity of persistent luminescent crystals decreases with increasing number of pressings. However, when these crystals are exposed to UV light, then the recovery of EML intensity takes place. The mechanical interaction between the bending segment of dislocations and filled electron traps is able to explain the elastico-ML of X-or γ-irradiated alkali halide crystals. However, the piezoelectrically-induced de-trapping model is suitable for explaining the ML of persistent luminescent crystals and ZnS:Mn. The investigation of elastico-ML may be helpful in understanding the thermoluminescence and the investigation of thermoluminescence may be helpful in understanding elastico-ML. Furthermore, similar to the thermoluminescence, the mechanoluminescence may also find application in radiation dosimetry. Expressions are derived for the elastico-ML of thermoluminescent crystals, in which a good agreement is found between the experimental and theoretical results. Finally, the application of the elasticoML of thermoluminescent crystals in light sources, displays, imaging devices, sensing devices, radiation dosimetry and in non-destructive testing of materials are discussed.Contents of Paper
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2

Gasiorowski, Andrzej, Piotr Szajerski, and Jose Francisco Benavente Cuevas. "Use of Terbium Doped Phosphate Glasses for High Dose Radiation Dosimetry—Thermoluminescence Characteristics, Dose Response and Optimization of Readout Method." Applied Sciences 11, no. 16 (August 5, 2021): 7221. http://dx.doi.org/10.3390/app11167221.

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The phosphate glass samples doped with Tb2O3 oxide (general formula: P2O5-Al2O3-Na2O-Tb2O3) were synthesized and studied for usage in high-dose radiation dosimetry (for example, in high-activity nuclear waste disposals). The influence of terbium concentration on thermoluminescent (TL) signals was analyzed. TL properties of glasses were investigated using various experimental techniques such as direct measurements of TL response vs. radiation dose, Tmax–Tstop and VHR (various heating rate) methods, and glow curve deconvolution analysis. The thermoluminescence dosimetry (TLD) technique was used as the main investigation tool to study detectors’ dose responses. It has been proved that increasing the concentration of terbium oxide in glass matrices significantly increases the thermoluminescence yield of examined material. For the highest dose range (up to 35 kGy), the dependence of the integrated thermoluminescent signals vs. dose can be considered as a saturation-type curve. Additional preheating of samples improves linearity of signal vs. dose dependencies and leads to a decrease of the signal loss over time. All obtained data suggest that investigated material can be used in high-dose radiation dosimetry. Additional advantages of the investigated dosimetric system are its potential ability to re-use the same dosimeters multiple times and the fact that reading dosimeters only requires usage of a basic TL reader without any modifications.
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3

Bhatt, B. C., and M. S. Kulkarni. "Thermoluminescent Phosphors for Radiation Dosimetry." Defect and Diffusion Forum 347 (December 2013): 179–227. http://dx.doi.org/10.4028/www.scientific.net/ddf.347.179.

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The use of thermoluminescence (TL) as a method for radiation dosimetry of ionizing radiation has been established for many decades and has found many useful applications in various fields, such as personnel and environmental monitoring, retrospective dosimetry, medical dosimetry, space dosimetry, high-dose dosimetry. Method of preparation, studies and applications of thermoluminescence (TL) dosimetric materials are reviewed. Several high sensitivity thermoluminescent dosimeters (TLDs) are now commercially available in different physical forms. These commercial TL dosimeters comply with a set of stringent requirements stipulated by the International Electrotechnical Commission (IEC). Specific features of TL phosphors for thermal neutron, fast neutron and high-energy charged particle (HCP) dosimetry are also considered. Some of the recent developments in the field of optically stimulated luminescence (OSL) and radiophotoluminescence (RPL) are also summarized. Comparative advantages of TL, OSL and RPL dosimeters are given. Results of recent studies of TL in nanosized materials are briefly presented. Future challenges in this field will also be discussed. Contents of Paper
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4

Taheri, Mohammad Ali, Amir Moslehi, Firooz Payervand, Farzad Ahmadkhanlou, and Farid Semsarha. "Experimental Test on the Effect of Taheri Consciousness Fields on Thermoluminescence Phenomenon." Scientific Journal of Cosmointel 2, no. 11 (October 11, 2023): 14–18. http://dx.doi.org/10.61450/joci.v2i11.156.

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In this paper, the combined effects of T-Consciousness Fields (TCFs) 1, 2, and 3 on the thermoluminescence phenomenon have been investigated. For this purpose, commercial thermoluminescent dosimeter chips GR-200 (LiF:Mg,Cu,P) were selected due to their high sensitivity to radiation. To assess the effects of TCFs on these chips, one GR-200 chip was discharged three consecutive times and radiated with beta radiation from a 90Sr source at an equivalent dose of 67.0 mSv (30 cycles in beta irradiator). Subsequently, its response (electric charge) and glow curve were measured. Then, the same chip was discharged three more consecutive times and irradiated under the same conditions, but in this case, TCFs were applied after discharge and simultaneously during irradiation. The results showed that the response of a single chip to TCFs decreased from 8.3% to 7.11% after the first to the third exposure. The observed results indicate a reduction in the response of GR-200 chip due to TCFs, thus experimentally confirming the effect of these fields on the thermoluminescence phenomenon.
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5

Sharmila, Kankanady, Nimitha S. Prabhu, Sudha D. Kamath, Vinayak A. Kamat, Kumaraswamy Swaroop, and Hiriyur M. Somashekarappa. "Thermoluminescence properties of copper-doped TiO2 nanoparticles synthesised using co-precipitation method for high-dose gamma dosimetry." Radiation Protection Dosimetry 199, no. 20 (December 2023): 2464–68. http://dx.doi.org/10.1093/rpd/ncad249.

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Abstract In this work, copper (Cu)-doped titanium dioxide (TiO2) nanoparticles were prepared by co-precipitation. For studying the morphological properties, the copper doped titanium dioxide (TiO2:Cu) nanocrystalline structures were characterised through powder X-ray diffraction and field emission scanning electron microscopy. The prepared TiO2:Cu nanoparticles were annealed at two temperatures, namely, copper doped titanium dioxide annealed at 723 K temperayure (TC1) and copper doped titanium dioxide annealed at 1073 K temperayure (TC2). The annealed samples were exposed to gamma radiation of 10-Gy-to-25-kGy doses. Thermoluminescence and dosimetric properties were evaluated using a thermoluminescent dosemeter reader. The glow curves of the TiO2:Cu nanoparticles were analysed. The thermoluminescence (TL) response of samples exhibited good linearity between 100 Gy and 10 kGy with high sensitivity of 1755.25 (TC1) and 5587.06 (TC2) counts g−1Gy−1 and a minimum detectable dose of 2.9666 Gy (TC1) and 0.4892 Gy (TC2). The fading of signals was observed by 12% for TC1 and 10% for TC2 samples after a week of storage.
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6

Oliveira Junot, Danilo, Marcos A. P. Chagas, and Divanízia Do Nascimento Souza. "ANÁLISE TERMOLUMINESCENTE DE COMPÓSITOS DE CaSO4 ATIVADO COM TERRAS RARAS." Eclética Química Journal 38, no. 1 (October 25, 2017): 90. http://dx.doi.org/10.26850/1678-4618eqj.v38.1.2013.p90-94.

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Since the thermoluminescence started to be applied to the dosimetry of ionizing radiation in 1940 different materials detectors have been proposed, and one of the most common is CaSO4. The motivation of this work was to produce crystals of CaSO4 doped with rare earth elements such as europium (Eu), neodymium (Nd) and thulium (Tm). It was also produced crystals of CaSO4:Ag. The interest in the production of these materials was to investigate other methods of production of thermoluminescent materials. The results show that the CaSO4:Tm is more suitable for use in the thermoluminescent dosimetry. Although not the most intense peak, the peak at 170 °C could be a dosimetric peak. Analyses showed that all samples have a TL response proportional to the dose absorbed.
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7

Furetta, C. "Thermoluminescence." La Rivista del Nuovo Cimento 21, no. 2 (February 1998): 1–62. http://dx.doi.org/10.1007/bf02900192.

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8

Wang, Xiao Ning, Jing Ning, Xiao Wei Fan, Chen Zhang, Xiao Sheng Huang, and Ying Huang. "Development of the Thermoluminescence Dosimetry Measure and Control System." Advanced Materials Research 663 (February 2013): 1023–28. http://dx.doi.org/10.4028/www.scientific.net/amr.663.1023.

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Briefly introduces the detection principle, characteristic and method of thermoluminescence dosimetry, and designs a set of data acquisition and processing system for thermoluminescence dosimeter reader. The device’s peripheral hardware circuit design is simple and scalable. This system can be applied to a variety of thermoluminescence dosimetry testing equipment.
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9

Xiong, Zheng Ye, Ping Ding, Qiang Tang, Jing Min Chen, and Wen Qing Shi. "Thermoluminescence Spectra of Lithium Tetraborate Single Crystal." Advanced Materials Research 160-162 (November 2010): 252–55. http://dx.doi.org/10.4028/www.scientific.net/amr.160-162.252.

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Lithium tetraborate (LBO or LTO) single crystal seems to be a promising new material for thermoluminescent dosimeter (TLD) and SAW resonators. In the present work, thermoluminescence (TL) characteristic and TL spectra of LTO single crystal grown by Bridgman method were measured, the kinetic parameters of TL traps were calculated, and TL spectra were analyzed. The result shows: The primary glow peaks are at about 186oC and 313oC. The activation energies of the traps corresponding to the two TL peaks are 0.96eV and 1.56eV, and the frequency factors are about 7.94×109s-1 and 6.31×1012s-1. The TL spectra of LTO crystal extends from 350nm to 460nm, and has its maximum at about 381nm. The intrinsic luminescent centers can send the energy from crystal lattice to Cu+ ions, because the activation energies of two are quite similar, and the Cu+ ions become new luminescent centers to increase TL sensitivity when Cu ions are doped into LTO crystals.
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10

Rivera Montalvo, T., C. Furetta, J. Azorín Nieto, C. Falcony Guajardo, M. García, and Eduardo Martínez. "Termoluminescent Properties of High Sensitive ZrO2+PTFE for UV Radiation Dosimetry." Materials Science Forum 480-481 (March 2005): 373–80. http://dx.doi.org/10.4028/www.scientific.net/msf.480-481.373.

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This paper presents the preparation method, luminescent characteristics and the results of studying the thermoluminescence (TL) properties of zirconium oxide (ZrO2) exposed to 260 nm ultraviolet radiation. The glow curve of ZrO2+PTFE pellets exhibited one peak centered at 180°C about 30°C lower than that the commercially available aluminum oxide peak (Al2O3:C). TL response as a function of spectral irradiance showed good linear in the range from 2.4 to 3000 µJ/cm2 of spectral irradiance. Experimental results of studying the thermoluminescent (TL) properties of ZrO2+PTFE exposed to ultraviolet radiation allow to propose zirconium oxide as an excellent candidate as ultraviolet radiation dosimeter.
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11

Kathren, R. L. "Unravelling thermoluminescence." Radiation Protection Dosimetry 163, no. 4 (October 24, 2014): 531–32. http://dx.doi.org/10.1093/rpd/ncu319.

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12

Mejdahl, Vagn. "Thermoluminescence dating." Norwegian Archaeological Review 23, no. 1-2 (January 1990): 21–29. http://dx.doi.org/10.1080/00293652.1990.9965503.

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13

Eremenko, A. N., I. I. Obraztsova, and N. K. Eremenko. "Nanodiamonds thermoluminescence." Russian Journal of Applied Chemistry 83, no. 1 (January 2010): 154–56. http://dx.doi.org/10.1134/s1070427210010295.

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14

Alexander, C. S., and S. W. S. McKeever. "Phototransferred thermoluminescence." Journal of Physics D: Applied Physics 31, no. 20 (October 21, 1998): 2908–20. http://dx.doi.org/10.1088/0022-3727/31/20/027.

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15

Sears, Derek W. G. "Thermoluminescence Dating." Geochimica et Cosmochimica Acta 50, no. 9 (September 1986): 2120–21. http://dx.doi.org/10.1016/0016-7037(86)90268-1.

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16

Bull, R. K. "Thermoluminescence dating." International Journal of Radiation Applications and Instrumentation. Part D. Nuclear Tracks and Radiation Measurements 11, no. 6 (January 1986): 339. http://dx.doi.org/10.1016/1359-0189(86)90064-6.

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17

Ducruet, Jean-Marc, and Imre Vass. "Thermoluminescence: experimental." Photosynthesis Research 101, no. 2-3 (June 24, 2009): 195–204. http://dx.doi.org/10.1007/s11120-009-9436-0.

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18

Rappaport, Fabrice, and Jérôme Lavergne. "Thermoluminescence: theory." Photosynthesis Research 101, no. 2-3 (June 17, 2009): 205–16. http://dx.doi.org/10.1007/s11120-009-9437-z.

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19

Rendell, Helen. "Thermoluminescence dating." Journal of Archaeological Science 13, no. 6 (November 1986): 603. http://dx.doi.org/10.1016/0305-4403(86)90047-6.

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20

Wintle, A. G. "Thermoluminescence dating." Quaternary Science Reviews 4, no. 4 (1985): iv—vi. http://dx.doi.org/10.1016/0277-3791(85)90007-1.

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21

Bhatt, BhuwanC. "Unraveling thermoluminescence." Radiation Protection and Environment 38, no. 4 (2015): 172. http://dx.doi.org/10.4103/0972-0464.176160.

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22

Huntley, D. J., D. I. Godfrey-Smith, M. L. W. Thewalt, J. R. Prescott, and J. T. Hutton. "Some quartz thermoluminescence spectra relevant to thermoluminescence dating." International Journal of Radiation Applications and Instrumentation. Part D. Nuclear Tracks and Radiation Measurements 14, no. 1-2 (January 1988): 27–33. http://dx.doi.org/10.1016/1359-0189(88)90038-6.

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23

Dhanalakshmi, K., A. Jagannatha Reddy, and V. Revathi. "Influence of Flux on the Structural and Thermoluminescence Properties of Y2SiO5:Dy3+ Nanophosphors for Dosimetric Applications." Asian Journal of Chemistry 34, no. 5 (2022): 1284–90. http://dx.doi.org/10.14233/ajchem.2022.23461.

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Potassium nitrate (KNO3) and ammonium chloride (NH4Cl) flux were added during the combustion synthesis of Y2SiO5:Dy3+ (9 mol %) nanophosphors, which influenced its structure, morphology and thermoluminescent properties. Reduction in the crystallite size to ~ 7 nm observed using XRD analysis. Surface morphology enhanced in terms of its texture. Thermoluminescence analysis of the prepared phosphors irradiated with gamma dose over a range of 500 Gy – 4 KGy at a constant heating rate 3 ºC s–1 have been carried out. Kinetic parameters were evaluated by Chens method and activation energy was found to be 1.01-1.3 eV. Flux addition resulted in creation of large number of charge carriers and hence the material become the potential for dosimetry applications.
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24

Rohul Rizki Mubaroq Hartman, Akhiruddin Maddu, Sitti Yani, and Nunung Nuraeni. "Synthesis and Thermoluminescence Properties of Undoped Calcium Fluoride (CaF2) Nanoparticles using Co-Precipitation Method." International Journal of Nanoelectronics and Materials (IJNeaM) 17, no. 1 (March 4, 2024): 131–35. http://dx.doi.org/10.58915/ijneam.v17i1.502.

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This study investigated the thermoluminescence properties of undoped CaF2 nanoparticles synthesized via co-precipitation with ethanol. X-ray diffraction revealed pure CaF2 nanoparticles with a complete cubic structure and an average crystallite size of 36.5 nm. Scanning electron microscopy confirmed the nanoscale size, averaging 51.23 nm. Electron dispersive spectroscopy analysis showed that the sample mainly consists of Ca and F, with oxygen potentially introducing defects in the crystal structure. Synthesized nanoparticles TL glow curves exposed to 7 mGy of 90Sr beta rays exhibited a prominent peak at 205 oC in thermoluminescence glow curves, likely due to oxygen-induced defects that act as thermoluminescence activators. The thermoluminescence activating energy and the frequency factor of the CaF2 nanoparticles were determined using initial rise methods of approximately 0.83 eV and 5.99 x 10-19, respectively.
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25

Amer, Hany, Mostafa Elashmawy, Huda Alazab, and El-Din Ezz. "Suitability of pure nano crystalline LiF as a TLD dosimeter for high dose gamma radiation." Nuclear Technology and Radiation Protection 33, no. 1 (2018): 93–99. http://dx.doi.org/10.2298/ntrp1801093a.

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LiF is an alkali halide that is commonly used in radiation dosimetry utilizing its well-known thermoluminescence property. Pure LiF has very limited use in radiation dosimetry since the density and types of the internal traps are limited. For that reason, LiF is usually doped with different elements such as Mg and Ti in (TLD-100) to enhance its thermoluminescence properties and to be suitable for dosimetry applications. In this work we used ball milling as an alternative to dopants (impurities) to induce structure defects (e.g. dislocation) that will play the major role in thermoluminescence process similar to defectsecaused by dopants. The dislocation density of 1 h ball milled pristine LiF was evaluated at the MCX beamline of the Italian Synchrotron ELETTRA. A ball milled LiF was then compressed in the form of chips, then annealed for 1 h at 600?C to get rid of low temperature dislocations. The annealed samples showed linear response in the range 50-300 Gy. Fading investigation showed that the integral thermoluminescence intensity almost stabilizes after 12 days from the first irradiation. Results indicate that ball milling is a new promising technique to produce thermoluminescence dosimeters without using any kind of dopants.
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26

Hideg, Éva, and Sándor Demeter. "Thermoluminescence and Delayed Luminescence Characterization of Photosystem IIα and Photosystem IIβ Reaction Centers." Zeitschrift für Naturforschung C 43, no. 7-8 (August 1, 1988): 596–600. http://dx.doi.org/10.1515/znc-1988-7-818.

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The thermoluminescence and delayed luminescence characteristics of PS IIα and PS IIβ centers were investigated in BBY particles and stroma thylakoids, respectively. The BBY particles exhibited a thermoluminescence band at 25 °C (B band) which was associated with the charge recombination of the S2Qв- redox couple and underwent period-2 oscillation in a sequence of flashes. In the flash-induced decay of delayed luminescence of BBY particles a component with a half-time of 34 s corresponded to the B thermoluminescence band and was also assigned to S2Oв- charge recombination. No corresponding thermoluminescence or delayed luminescence components associated with the secondary acceptor Qв could be observed in the glow curve or delayed luminescence decay of stroma thylakoids. These observations indicate that unlike PS IIα the PS IIβ centers are not associated with the two-electron gate, Qв.
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27

Dykeman, Douglas D., Ronald H. Towner, and James K. Feathers. "Correspondence in Tree-Ring and Thermoluminescence Dating: A Protohistoric Navajo Pilot Study." American Antiquity 67, no. 1 (January 2002): 145–64. http://dx.doi.org/10.2307/2694883.

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Dating of early Navajo residence and special use sites, ca. A.D. 1500-1775, has been hampered by a lack of datable materials and poor precision in radiocarbon results. Methods described in this paper use materials ubiquitous at early Navajo sites in northwestern New Mexico and employ a dual strategy involving tree-ring dating of nonarchitectural wood and thermoluminescence assay of ceramics and burned rock. Comparison of samples obtained from a number of sites near the Morris Site 1 pueblito indicates remarkable correspondence between tree-ring and thermoluminescence results. These techniques are argued to have considerable reliability for relatively recent cultural manifestations such as these early Navajo sites. Thermoluminescence in particular may be useful in protohistoric contexts where tree-ring dating is unavailable. The thermoluminescence technique has the added benefit of directly dating pottery sherds, which can be useful for developing ceramic cross-dating sequences.
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28

Sugakov, V. I. "Fine structure of thermoluminescence assisted by molecular vibrations in disordered organic semiconductors." Journal of Physics: Condensed Matter 34, no. 18 (March 2, 2022): 185703. http://dx.doi.org/10.1088/1361-648x/ac50d9.

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Abstract The article deals with the issue of the influence of a separate mode of molecular vibrations on the formation of the thermoluminescence from disordered systems with quasi-continuous spectra of localized carriers. The contribution of vibrations is noticeable if the energy of their quanta is close to the depth of some localized carriers and the transition of the carrier into the conductive region occurs via absorption of these quanta. At some value of a carrier–vibration interaction, the effect manifests itself in the appearance of a fine discrete structure on the generally smooth thermoluminescence curve. The thermoluminescence of polymers is calculated using the model of non-adiabatic transitions, in which the carrier–vibrational interaction is determined by the displacements of nuclei in the presence of the carrier. The dependence of the arising discrete structure of the thermoluminescence curve on a number of parameters of the system like the magnitude of the carrier–vibration interaction, the width of vibrational levels, the parameters of the conductive region is investigated. The processes with participation of multiple quanta of vibrations are investigated and the formation of repetitive structures on the thermoluminescence curve has been shown owing to the absorption of several vibrational quanta. Analysis of a number of experiments is presented using the suggested theory.
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29

Edilashvili, V., Yu Blagidze, O. Gogolin, and E. Tsitsishvili. "Thermoluminescence peculiarities of CdS1−xSex–doped borosilicate glasses." Chalcogenide Letters 20, no. 4 (April 2023): 235–41. http://dx.doi.org/10.15251/cl.2023.204.235.

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Thermally stimulated luminescence of the X-ray irradiated CdSSe-doped borosilicate glases have been studied. The two well defined temperarure maxima discovered for total thermoluminescence intensity, as well as the thermoluminescence dependence on the nanocrystal size and X-ray dose are discussed.
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30

Pathan, Suhana, Prachi Dubey, Prachi Tadge, and Sudeshna Ray. "A Comprehensive Review on Rare-Earth Based Thermoluminescence Phosphors for Radiation Dosimetry." ECS Transactions 107, no. 1 (April 24, 2022): 20073–84. http://dx.doi.org/10.1149/10701.20073ecst.

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When ionizing radiation is incident on an insulating crystal, some of the deposited energy is stored in the lattice at defect sites, colour centres, etc. Upon heating the crystal, this stored energy is released and a fraction of it may be emitted as visible light. This is called ‘Thermoluminescence.’ Within certain limitations, the amount of light emitted is proportional to the radiation dose previously absorbed by the TL material. The application of thermoluminescence (TL) as a methodology for radiation dosimetry of ionizing radiation has been well-established since several decades and has found number of practical applications in various fields, such as personnel and environmental monitoring, retrospective dosimetry, medical dosimetry, space dosimetry, high-dose dosimetry, etc. Especially, alkaline-earth silicates are appropriate compounds as radiation detectors due to their high chemical stability. Doping may either cause the formation of new defect centers or recovering of existing levels within the band-gap for a defective host which changes both the optical and electronic features of the materials. Therefore, it is of great importance by choosing both the dopant as well as the host for thermoluminescence application. It has already been reported that commercially available thermoluminescence phosphor suffers from fading, stability, etc., which justifies the ongoing need to identify factors that can be exploited to make a thermoluminescence phosphor with high efficiency and stability.
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Vass, Imre, Narendranath Mohanty, and Sándor Demeter. "Photoinhibition of Electron Transport Activity of Photosystem II in Isolated Thylakoids Studied by Thermoluminescence and Delayed Luminescence." Zeitschrift für Naturforschung C 43, no. 11-12 (December 1, 1988): 871–76. http://dx.doi.org/10.1515/znc-1988-11-1213.

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Abstract The effect of photoinhibition on the primary (QA) and secondary (QB) quinone acceptors of photosystem I I was investigated in isolated spinach thylakoids by the methods of thermoluminescence and delayed luminescence. The amplitudes of the Q (at about 2 °C) and B (at about 30 °C) thermoluminescence bands which are associated with the recombination of the S2QA- and S2QB charge pairs, respectively, exhibited parallel decay courses during photoinhibitory treatment. Similarly, the amplitudes of the flash-induced delayed luminescence components ascribed to the recombination of S20A and S2OB charge pairs and having half life-times of about 3 s and 30 s, respectively, declined in parallel with the amplitudes of the corresponding Q and B thermoluminescence bands. The course of inhibition of thermoluminescence and delayed luminescence intensity was parallel with that of the rate of oxygen evolution. The peak positions of the B and Q thermoluminescence bands as well as the half life-times of the corresponding delayed luminescence components were not affected by photoinhibition. These results indicate that in isolated thylakoids neither the amount nor the stability of the reduced OB acceptor is preferentially decreased by photoinhibition. We conclude that either the primary target of photodamage is located before the O b binding site in the reaction center of photosystem II or QA and OB undergo simultaneous damage.
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32

FUKUDA, Yasunori, and Nozomu TAKEUCHI. "Thermoluminescence in CaB4O7." Journal of the Society of Materials Science, Japan 34, no. 380 (1985): 533–35. http://dx.doi.org/10.2472/jsms.34.533.

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33

Demeter, S., and Govindjee. "Thermoluminescence in plants." Physiologia Plantarum 75, no. 1 (January 1989): 121–30. http://dx.doi.org/10.1111/j.1399-3054.1989.tb02073.x.

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Prescott, John R., Phillip J. Fox, R. A. Akber, and H. E. Jensen. "Thermoluminescence emission spectrometer." Applied Optics 27, no. 16 (August 15, 1988): 3496. http://dx.doi.org/10.1364/ao.27.003496.

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LAPRAZ, D., and P. IACCONI. "Dosimétrie par thermoluminescence." Radioprotection 25, no. 2 (April 1990): 117–33. http://dx.doi.org/10.1051/radiopro/1990020.

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Garcia Guinea, J., V. Correcher, and F. J. Valle-Fuentes. "Thermoluminescence of Kaolinite." Radiation Protection Dosimetry 84, no. 1 (August 1, 1999): 507–10. http://dx.doi.org/10.1093/oxfordjournals.rpd.a032787.

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Hamilton, Ian. "OPERATIONAL THERMOLUMINESCENCE DOSIMETRY." Health Physics 78, no. 5 (May 2000): 569. http://dx.doi.org/10.1097/00004032-200005000-00020.

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Sahare, P. D., and S. V. Moharil. "Thermoluminescence in LiNaSO4." Radiation Effects and Defects in Solids 114, no. 1-2 (May 1990): 167–72. http://dx.doi.org/10.1080/10420159008213093.

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McKeever, S. W. S., and Richard H. Bube. "Thermoluminescence of Solids." Physics Today 40, no. 4 (April 1987): 80–81. http://dx.doi.org/10.1063/1.2819986.

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Abtahi, A., P. Bräunlich, P. Kelly, and J. Gasiot. "Laser stimulated thermoluminescence." Journal of Applied Physics 58, no. 4 (August 15, 1985): 1626–39. http://dx.doi.org/10.1063/1.336052.

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Bos, A. J. J. "Theory of thermoluminescence." Radiation Measurements 41 (December 2006): S45—S56. http://dx.doi.org/10.1016/j.radmeas.2007.01.003.

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Drozdowski, W., D. Wisniewski, A. J. Wojtowicz, A. Lempicki, P. Dorenbos, J. T. M. de Haas, C. W. E. van Eijk, and A. J. J. Bos. "Thermoluminescence ofLuAlO3: Ce." Journal of Luminescence 72-74 (June 1997): 756–58. http://dx.doi.org/10.1016/s0022-2313(96)00212-8.

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H.K.H. "Thermoluminescence of solids." Materials Research Bulletin 22, no. 5 (May 1987): 711. http://dx.doi.org/10.1016/0025-5408(87)90121-8.

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H.K.H. "Thermoluminescence of solids." Materials Research Bulletin 24, no. 7 (July 1989): 916. http://dx.doi.org/10.1016/0025-5408(89)90058-5.

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Rendell, H. M. "Thermoluminescence of solids." Physics of the Earth and Planetary Interiors 59, no. 3 (1990): 225–26. http://dx.doi.org/10.1016/0031-9201(90)90229-q.

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Hornyak, William. "Thermoluminescence of solids." Journal of Luminescence 35, no. 4 (July 1986): 239–40. http://dx.doi.org/10.1016/0022-2313(86)90016-5.

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Furetta, C., and G. Kitis. "Models in thermoluminescence." Journal of Materials Science 39, no. 7 (April 2004): 2277–94. http://dx.doi.org/10.1023/b:jmsc.0000019989.60268.d7.

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Zeller, Edward J. "Thermoluminescence of solids." Geochimica et Cosmochimica Acta 54, no. 1 (January 1990): 255. http://dx.doi.org/10.1016/0016-7037(90)90218-a.

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Gartia, R. K., S. Ingotombi, and S. Dorendrajit Singh. "Thermoluminescence of cement." Bulletin of Materials Science 18, no. 2 (April 1995): 107–13. http://dx.doi.org/10.1007/bf02747529.

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Sears, Derek W. G. "Thermoluminescence of Solids." Geochimica et Cosmochimica Acta 50, no. 9 (September 1986): 2121. http://dx.doi.org/10.1016/0016-7037(86)90269-3.

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