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1

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 o
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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
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3

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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4

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.
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5

Omanwar, S. K., K. A. Koparkar, and Hardev Singh Virk. "Recent Advances and Opportunities in TLD Materials: A Review." Defect and Diffusion Forum 347 (December 2013): 75–110. http://dx.doi.org/10.4028/www.scientific.net/ddf.347.75.

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Thermoluminescence (TL) is the thermally stimulated emission of light from an insulator or a semiconductor following the previous absorption of energy from ionizing radiation. TL dosimetry is used in many scientific and applied fields such as radiation protection, radiotherapy, industry, and environmental and space research, using many different materials. The basic demands of a thermoluminescent dosimeter (TLD) are good reproducibility, low hygroscopicity, and high sensitivity for very low dose measurements and good response at high doses in radiotherapy and in mixed radiation fields. In this
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6

Murthy, K. V. R. "Thermoluminescence and its Applications: A Review." Defect and Diffusion Forum 347 (December 2013): 35–73. http://dx.doi.org/10.4028/www.scientific.net/ddf.347.35.

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The present review article contains various applications of Thermoluminescence. The phenomena of thermoluminescence (TL) or thermally stimulated luminescence (TSL) and optically stimulated luminescence (OSL) are widely used for measurement of radiation doses from ionizing radiations, viz. x-rays, γ rays and β particles. The applications of TL are initiated in the field of Geology followed by Archaeology, personal dosimetry, material characterization and many more to name. The TL technique has been found to be useful in dating specimens of geologically recent origin where all other conventional
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7

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 p
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8

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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9

Abraheem, Abeer Z., F. Khamis, and Y. A. Abdulla. "TL Characteristics and Dosimetric Aspects of Mg-Doped ZnO." European Journal of Applied Physics 3, no. 1 (January 29, 2021): 43–47. http://dx.doi.org/10.24018/ejphysics.2021.3.1.37.

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Dosimetry characterization and the evaluation of kinetics parameters of trapping states of Mg-doped ZnO phosphors synthesized by Sol-Gel technique. The thermoluminescence response of Mg-doped ZnO samples showed a linear response when exposed to X-ray radiation and the optimum annealing condition was 400oC/4h for the three concentrations. A broad-shaped TL glow curve with an upper bound of 270 °C, which shifts to lower temperatures with increasing dose, indicating that general order (GO) kinetics thermoluminescence processes are involved. We conclude that the ZnO doped Mg phosphors under study
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10

Paprocki, K., J. Winiecki, R. Kabacińska, K. Przegietka, M. Szybowicz, and K. Fabisiak. "Thermoluminescence properties of undoped diamond films deposited using HF CVD technique." Materials Science-Poland 35, no. 4 (March 21, 2018): 785–90. http://dx.doi.org/10.1515/msp-2017-0103.

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Abstract Natural diamond has been considered as a perspective material for clinical radiation dosimetry due to its tissuebiocompatibility and chemical inertness. However, the use of natural diamond in radiation dosimetry has been halted by the high market price. The recent progress in the development of CVD techniques for diamond synthesis, offering the capability of growing high quality diamond layers, has renewed the interest in using this material in radiation dosimeters having small geometricalsizes. Polycrystalline CVD diamond films have been proposed as detectors and dosimeters of β and
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11

Julius (INVITED), H. W. "Instrumentation in Thermoluminescence Dosimetry." Radiation Protection Dosimetry 17, no. 1-4 (December 1, 1986): 267–73. http://dx.doi.org/10.1093/rpd/17.1-4.267.

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12

Bos, A. J. J. "High sensitivity thermoluminescence dosimetry." Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms 184, no. 1-2 (September 2001): 3–28. http://dx.doi.org/10.1016/s0168-583x(01)00717-0.

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13

Julius (INVITED), H. W. "Instrumentation in Thermoluminescence Dosimetry." Radiation Protection Dosimetry 17, no. 1-4 (December 1, 1986): 267–73. http://dx.doi.org/10.1093/oxfordjournals.rpd.a079821.

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14

Rivera, T. "Thermoluminescence in medical dosimetry." Applied Radiation and Isotopes 71 (December 2012): 30–34. http://dx.doi.org/10.1016/j.apradiso.2012.04.018.

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15

Burruel-Ibarra, S. E., C. Cruz-Vázquez, R. Bernal, J. R. Martínez-Castelo, A. R. García Haro, and V. R. Orante-Barrón. "Synthesis and Thermoluminescent Properties of New ZnO Phosphors." Materials Science Forum 755 (April 2013): 139–44. http://dx.doi.org/10.4028/www.scientific.net/msf.755.139.

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In this work, results on the thermoluminescence dosimetry properties of beta particle irradiated ZnO obtained by thermal annealing of chemically synthesized ZnS are reported. ZnS powder was sintered at 950 °C during 24 h in air, in order to obtain pellet-shaped ZnO samples. The thermoluminiescence (TL) intensity of ZnO previously exposed to beta radiation increased as the dose increased in the 0.025-6.4 kGy interval studied. Characteristic glow curves exhibited two emission maxima at ~ 94 and ~ 341 °C. The dosimetric peak located at ~ 341 °C shifted towards lower temperatures as the dose incre
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16

García-Haro, A. R., R. Bernal, C. Cruz-Vázquez, S. E. Burruel-Ibarra, V. R. Orante-Barrón, and F. Brown. "Study of the Thermoluminescent Characteristics of Ceramic Roof Tiles Exposed to Beta Radiation." MRS Proceedings 1481 (2012): 89–95. http://dx.doi.org/10.1557/opl.2012.1636.

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ABSTRACTIn this work, thermoluminescence (TL) characteristics of roof tile ceramic samples previously exposed to beta radiation are reported for the very first time. TL measurements were carried out using powdered samples obtained by the the fine-grained method, with grain size ranged from 300 nm to 5 μm. Characteristic thermoluminescence glow curves showed a complex structure with a dosimetric maximum located at ~ 200 °C. TL response of roof tile samples increases as the radiation dose increases in the 25 Gy to 1.6 kGy range. One response showed a linear behaviour, with no evidence of saturat
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17

Cipa, J., L. Trinkler, and B. Berzina. "Thermoluminescence Response of AlN+Y2O3 Ceramics to Sunlight and X-Ray Irradiation." Latvian Journal of Physics and Technical Sciences 58, no. 1 (January 29, 2021): 3–14. http://dx.doi.org/10.2478/lpts-2021-0001.

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Abstract AlN is a wide band gap material with promising properties for dosimetric applications, especially in UV dosimetry. In the present research, the thermoluminescence method is used in order to better understand sunlight and X-ray irradiation effects on yttria doped AlN ceramics. In general, the TL response is characterised by a broad TL peak with maxima around 400–450 K and a TL emission spectrum with UV (400 nm), Blue (480 nm) and Red (600 nm) bands. Compared to the X-ray irradiation, sunlight irradiation creates a wider TL glow curve peak with a maximum shifted to higher temperatures b
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18

Abdel-Razek, Yassin A. "Thermoluminescence dosimetry using natural calcite." Journal of Taibah University for Science 10, no. 2 (April 2016): 286–95. http://dx.doi.org/10.1016/j.jtusci.2015.08.002.

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19

McKeever, S. W. S. "Editorial - Thermoluminescence Dosimetry: Deterministic Unpredictability." Radiation Protection Dosimetry 49, no. 4 (October 1, 1993): 405–6. http://dx.doi.org/10.1093/oxfordjournals.rpd.a081979.

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20

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 thermoluminesc
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21

Orante-Barrón, V. R., F. M. Escobar-Ochoa, C. Cruz-Vázquez, and R. Bernal. "Thermoluminescence of Novel Zinc Oxide Nanophosphors Obtained by Glycine-Based Solution Combustion Synthesis." Journal of Nanomaterials 2015 (2015): 1–5. http://dx.doi.org/10.1155/2015/273571.

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High-dose thermoluminescence dosimetry properties of novel zinc oxide nanophosphors synthesized by a solution combustion method in a glycine-nitrate process are presented for the very first time in this work. Sintered particles with sizes ranging between ~500 nm and ~2 μm were obtained by annealing the synthesized ZnO at 900°C during 2 h in air. X-ray diffraction patterns indicate the presence of the ZnO hexagonal phase, without any remaining nitrate peaks observed. Thermoluminescence glow curves of ZnO obtained after being exposed to beta radiation consists of two maxima: one located at ~149°
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22

Freire de Souza, Luiza, and Divanízia N. Souza. "PRODUÇÃO DE DOSÍMETROS TERMOLUMINESCENTES À BASE DE MgB4O7: Dy e MgB4O7:Tm." Eclética Química Journal 38, no. 1 (October 25, 2017): 101. http://dx.doi.org/10.26850/1678-4618eqj.v38.1.2013.p101-108.

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The thermoluminescent dosimetry (TL) is a well-established technique for the detection of ionizing radiation in hospitals, clinics, and industrial establishments where there is the need to quantify the radiation. For this practice is require the use phosphors which are sensitive to radiation. Some phosphors are already commonly used in this practice, for example, TLD-100 (LiF: Mg, Ti), CaSO4:Tm and CaSO4:Dy. A compound that was most recently introduced in dosimetry and has many advantageous features to detect neutrons, electrons and gamma is the magnesium tetraborate (MgB4O7), but the undoped
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23

Journal, Baghdad Science. "Using LiF Disc in Thermoluminescence Dosimetry." Baghdad Science Journal 5, no. 1 (March 2, 2008): 51–54. http://dx.doi.org/10.21123/bsj.5.1.51-54.

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A LiF (TLD-700) PTFED disc has adiameter of (13mm) and thickness of (0.4mm) for study the response and sensetivity of this material for gamma and beta rays by using (TOLEDO) system from pitman company. In order to calibrate the system and studying the calibration factor. Discs were irradiated for Gamma and Beta rays and comparing with the theoretical doses. The exposure range is between 15×10-2 mGy to 1000×10-2 mGy. These doses are within the range of normal radiation field for workers.
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24

Cameron, John. "Thermoluminescence dosimetry materials: Properties and uses." Applied Radiation and Isotopes 49, no. 4 (April 1998): 405–6. http://dx.doi.org/10.1016/s0969-8043(96)00317-x.

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25

Olko, P. "Thermoluminescence dosimetry materials: Properties and uses." Radiation Physics and Chemistry 50, no. 3 (September 1997): 313–14. http://dx.doi.org/10.1016/s0969-806x(95)00177-y.

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26

Gilvin, P. J., S. T. Baker, D. C. Rose, and N. J. Garratt. "The UK HPA thermoluminescence dosimetry system." Radiation Measurements 43, no. 2-6 (February 2008): 611–15. http://dx.doi.org/10.1016/j.radmeas.2007.12.048.

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27

Moscovitch (INVITED), M. "Dose Algorithms for Personal Thermoluminescence Dosimetry." Radiation Protection Dosimetry 47, no. 1-4 (May 1, 1993): 373–80. http://dx.doi.org/10.1093/rpd/47.1-4.373.

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28

Furetta, C., V. Mendozzi, C. Sanipoli, A. Scacco, C. Leroy, F. Marullo, and P. Roy. "Thermoluminescence of LiF:Cu2+in radiation dosimetry." Journal of Physics D: Applied Physics 28, no. 7 (July 14, 1995): 1488–94. http://dx.doi.org/10.1088/0022-3727/28/7/030.

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29

Gfirtner, H. "A management system for thermoluminescence dosimetry." IFAC Proceedings Volumes 36, no. 15 (August 2003): 517–20. http://dx.doi.org/10.1016/s1474-6670(17)33557-7.

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30

Somaiah, K., and B. Sathyanarayana. "A New Phospnor for Thermoluminescence Dosimetry." Crystal Research and Technology 26, no. 2 (1991): K34—K38. http://dx.doi.org/10.1002/crat.2170260223.

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31

Moscovitch (INVITED), M. "Dose Algorithms for Personal Thermoluminescence Dosimetry." Radiation Protection Dosimetry 47, no. 1-4 (May 1, 1993): 373–80. http://dx.doi.org/10.1093/oxfordjournals.rpd.a081770.

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32

Ranogajec-Komor, M^ ^aacute;ria. "Thermoluminescence Dosimetry-Application in Environmental Monitoring." Radiation Safety Management 2, no. 1 (2003): 2–16. http://dx.doi.org/10.12950/rsm2002.2.2.

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33

Kron, T. "Applications of Thermoluminescence Dosimetry in Medicine." Radiation Protection Dosimetry 85, no. 1 (September 1, 1999): 333–40. http://dx.doi.org/10.1093/oxfordjournals.rpd.a032865.

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34

Sweet, M. A. S., and J. Rennie. "Thermoluminescence dosimetry using doped calcium sulphide." Journal of Crystal Growth 86, no. 1-4 (January 1988): 942–47. http://dx.doi.org/10.1016/0022-0248(90)90829-a.

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35

Einbergs, Ernests, Aleksejs Zolotarjovs, Ivita Bite, Katrina Laganovska, Krisjanis Auzins, Krisjanis Smits, and Laima Trinkler. "Usability of Cr-Doped Alumina in Dosimetry." Ceramics 2, no. 3 (September 2, 2019): 525–35. http://dx.doi.org/10.3390/ceramics2030040.

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Dosimetry is a widespread material science field dealing with detection and quantification of ionizing radiation using electronic processes in materials. One of the main aspects that determines the performance of dosimeters is the type of defects the material contains. Crystalline lattice imperfections are formed around impurity ions, which may have a smaller or larger size, or different oxidation states compared to host ions. In this study, we show what effects Cr impurities have on the luminescent properties of alumina. Porous Al 2 O 3 : Cr microceramics synthesized using the sol-gel method
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36

Chandler, J. R., S. Sholom, S. W. S. McKeever, and H. L. Hall. "Thermoluminescence and phototransferred thermoluminescence dosimetry on mobile phone protective touchscreen glass." Journal of Applied Physics 126, no. 7 (August 21, 2019): 074901. http://dx.doi.org/10.1063/1.5108971.

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37

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
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38

Matsumoto, Tetsuo. "Thermal neutron response of thermoluminescence dosimeters for application to biomedical dosimetry." Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment 301, no. 3 (March 1991): 552–57. http://dx.doi.org/10.1016/0168-9002(91)90022-i.

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39

Rahman, M. Obaidur, Md Ashraful Hoque, Md Shakilur Rahman, and Afia Begum. "Responses of LiF Thermoluminescence Dosimeters to Diagnostic 60Co Teletherapy Beams." Bangladesh Journal of Medical Physics 8, no. 1 (September 10, 2017): 14–21. http://dx.doi.org/10.3329/bjmp.v8i1.33930.

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Thermoluminescence Dosimeter (TLD) is used as an ionizing radiation detector in the field of clinical radiotherapy, diagnostic radiology, personal radiation monitoring as well as in environmental radiation dosimetry. The sensitivity of all the TLDs is not the same even though the manufacturer produced them in the same batch. The response of TLD at various doses is also not always linear. In the present study fifty-seven rod shaped LiF TLDs had been irradiated by doses of 50cGy, 100cGy, 150cGy and 200cGy using 60Co teletherapy unit of Dhaka Medical College (Alcyon II, CGR, McV, France). The TLD
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40

Journal, Baghdad Science. "Thermoluminescence dosimetry of mixed neutron – gamma fields." Baghdad Science Journal 9, no. 3 (December 11, 2018): 446–49. http://dx.doi.org/10.21123/bsj.9.3.446-449.

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The method of measurement dosimetry in neutron – gamma field by using CaSo4 : Dy (PTFE) disc which has a diameter of 1.3mm and thickness of 0.2mm and using hydrogenated material as a converters of neutron to recoil protons (n-p) reaction, the discs were irradiated by neutron source (241Am-Be) with flux of 4.5?105 n/cm2s for different time to obtain different dose. The TL signals, which we have been obtained by using the converters, are increases to 71%. So we can resolve the neutron and gamma in mixed field.
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41

Braunlich, P. F., and W. Tetzlaff. "An Automated Laser Heated Thermoluminescence Dosimetry System." Radiation Protection Dosimetry 17, no. 1-4 (December 1, 1986): 321–24. http://dx.doi.org/10.1093/rpd/17.1-4.321.

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42

Shaver, I. Kh, and V. G. Krongauz. "Compositional Principle in Fast Neutron Thermoluminescence Dosimetry." Radiation Protection Dosimetry 33, no. 1-4 (October 1, 1990): 67–70. http://dx.doi.org/10.1093/rpd/33.1-4.67.

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43

Puppalwar, S. P., S. J. Dhoble, and Animesh Kumar. "Cu+emission in Li2BPO5material for thermoluminescence dosimetry." Radiation Effects and Defects in Solids 167, no. 5 (May 2012): 333–41. http://dx.doi.org/10.1080/10420150.2011.653663.

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44

Braunlich, P. F., and W. Tetzlaff. "An Automated Laser Heated Thermoluminescence Dosimetry System." Radiation Protection Dosimetry 17, no. 1-4 (December 1, 1986): 321–24. http://dx.doi.org/10.1093/oxfordjournals.rpd.a079832.

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45

Shaver, I. Kh, and V. G. Krongauz. "Compositional Principle in Fast Neutron Thermoluminescence Dosimetry." Radiation Protection Dosimetry 33, no. 1-4 (October 1, 1990): 67–70. http://dx.doi.org/10.1093/oxfordjournals.rpd.a080760.

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46

Hirning, C. Ross. "Detection and Determination Limits For Thermoluminescence Dosimetry." Health Physics 62, no. 3 (March 1992): 223–27. http://dx.doi.org/10.1097/00004032-199203000-00002.

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47

A. Sono, D., and S. W. S. McKeever. "Phototransferred Thermoluminescence for Use in UVB Dosimetry." Radiation Protection Dosimetry 100, no. 1 (July 1, 2002): 309–12. http://dx.doi.org/10.1093/oxfordjournals.rpd.a005875.

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48

Ginzburg, D., L. Oster, I. Eliyahu, G. Reshes, S. Biderman, and Y. S. Horowitz. "MANIPULATION OF THE DOSE–RESPONSE OF COMPOSITE GLOW PEAK 5 IN THE THERMOLUMINESCENCE OF LiF:Mg,Ti (TLD-100) VIA OPTICAL EXCITATION POST-IRRADIATION: POTENTIAL FOR IMPROVED DOSE–RESPONSE LINEARITY BEYOND 1 Gy." Radiation Protection Dosimetry 184, no. 2 (December 1, 2018): 248–55. http://dx.doi.org/10.1093/rpd/ncy206.

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Abstract Many dosimetric applications and especially those involved in clinical dosimetry are hampered by the supralinearity of TLD-100 which begins at a level of dose of 1 Gy. This research investigates the effect of optical excitation following irradiation on the dose–response. It is expected that this will lead to a more linear dose–response, however, irrespective of the hoped-for linearity, the theoretical/kinetic simulations of the effect of optical excitation will further enhance our understanding of the thermoluminescence mechanisms, especially the role of spatially correlated trapping
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49

Mat Nawi, Siti Nurasiah, Norfadira Wahib, Nurul Najua Zulkepely, Yusoff Mohd Amin, Ung Ngie Min, David Andrew Bradley, Siti Fairus Abdul Sani, and Mohd Jamil Maah. "Thermoluminescence Characteristics of Cylindrical Optical Fibers with Different Diameters in Radiation Dosimetry Subjected to Electron Irradiation." Advanced Materials Research 1133 (January 2016): 409–13. http://dx.doi.org/10.4028/www.scientific.net/amr.1133.409.

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Thermoluminescence (TL) characteristics for various cross-sections of 6 mole% of tailor-made Ge-doped cylindrical optical fibers were determined. The general TL characteristic i.e., dose rate dependence, energy dependence, dose response and reproducibility of the samples have been investigated. The samples were irradiated using electron beam (Linac) and been exposed to dose ranging from 1 to 4 Gy. The cylindrical optical fibers provide highly linear dose response within the clinical relevant dose range, independence of radiation energy over the range of energies investigated, independence of d
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50

Patel, Nimesh P., Vishwnath Verma, Dhaval Modi, K. V. R. Murhty, and M. Srinivas. "Thermoluminescence kinetic features of Eu3+ doped strontium pyrophosphate after beta irradiation." RSC Advances 6, no. 81 (2016): 77622–28. http://dx.doi.org/10.1039/c6ra15672j.

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Strontium pyrophosphate (Sr<sub>2</sub>P<sub>2</sub>O<sub>7</sub>) doped with various concentrations of Eu<sup>3+</sup> as a doping agent is synthesized using a combustion method and to study the thermoluminescence dosimetry [TLD] and applications.
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