Relevant bibliographies by topics / Thermoluminescence glow curve

Academic literature on the topic 'Thermoluminescence glow curve'

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Published: 10 December 2022
Last updated: 28 January 2023

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Journal articles on the topic "Thermoluminescence glow curve"

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Vejnovic, Zdravko, Milos Pavlovic, Marina Kutin, and Milorad Davidovic. "Glow curve analysis by Gauss-Lorentz function." Nuclear Technology and Radiation Protection 28, no. 1 (2013): 45–51. http://dx.doi.org/10.2298/ntrp1301045v.

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A new method for fitting glow curves, described in a mixed order kinetics model, with Gauss-Lorentz function is shown. Theoretical expressions of the mixed order kinetics model are shown in a new way, so that the values of kinetic parameters can be obtained through the geometric parameters. When the model is described in this way it is possible to calculate precisely the kinetic parameters such as activation energy, pre-exponential factor and the factor a= n0/(h + n0). At the same time, obtained values of geometric parameters of the experimental curve, which is described with the Gauss-Lorentz function, can be used to estimate the kinetic model, in which thermoluminescence relaxation occurs. This gives a possibility of a new application of Gauss-Lorentz function to be used as a criterion for assessing model of relaxation, when it is not known in advance. The accuracy of fitting is studied, for the specific cases of computer simulated thermoluminescent curves with one peak.
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Perks, C. A., and M. Marshall. "Techniques for Thermoluminescence Glow Curve Analysis." Radiation Protection Dosimetry 38, no. 4 (September 1, 1991): 261–69. http://dx.doi.org/10.1093/oxfordjournals.rpd.a081100.

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Singh, L. Robindro, and S. Dorendrajit Singh. "Particle Size Effect on TL Emission of ZnS Nanoparticles and Determination of Its Kinetic Parameters." Journal of Nanomaterials 2012 (2012): 1–8. http://dx.doi.org/10.1155/2012/239182.

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Nanoparticles have large surface area, and most of the ions are lying on its surface. Could these surface ions be contributed in thermoluminescence emission or enhanced nonradiative transition? In view of this, we have prepared small sizes of ZnS nanoparticles at low temperature and made two samples, one as-prepared (size ~3 nm) and the other heat-treated at 1073 K (size ~32 nm). Characterization of the samples shows that the prepared phosphors are pure. Thermoluminescence (TL) glow curves could not be recorded in both samples without irradiation. Even for higher dose ofγ-radiation the as-prepared samples could not show TL signal, but 1073 K heat-treated sample shows the TL signal. This may be due to the fact that smaller particles have large surface area compared to bigger particles, the surface ions may produce the nonradiative transitions. The kinetic parameters of the TL glow curves are evaluated by the conventional methods and compared with curve fitting computerised glow curve deconvolution (CGCD) technique. The variations in both techniques are found only ±0.02. The shape factor of all the glow curves ~0.48, and these TL glow curves could be fitted with order of kinetics 1.5.
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Salama, Elsayed, Dalal A. Aloraini, Sara A. El-Khateeb, and Mohamed Moustafa. "Rhyolite as a Naturally Sustainable Thermoluminescence Material for Dose Assessment Applications." Sustainability 14, no. 11 (June 6, 2022): 6918. http://dx.doi.org/10.3390/su14116918.

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Thermoluminescence characteristics of natural rhyolite have been studied. Dose response at a wide dose range of 0.5–2000 Gy has been determined. Minimum detectable dose and thermal fading rate are evaluated. Glow curve deconvolution is conducted after determining the best read-out conditions. The repeated initial rise (RIR) method is used to detect the overlapping peaks, and a glow curve deconvolution procedure is used to extract the thermoluminescence parameters of rhyolite. According to the findings, rhyolite glow curves show five interfering peaks corresponding to five electron trap levels at 142, 176, 221, 298, and 355 °C, respectively, at a heating rate of 3 °C/s. The obtained kinetic order for the deconvoluted peaks showed mixed-order kinetic. The reported results might be useful to introduce rhyolite as a natural sustainable material for radiation dosimetry applications.
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Verma, Durga, R. P. Patel, and Mohan L. Verma. "Optical properties of Sr2SiO4:Eu2+, Dy3+ phosphors prepared by combustion method." Materials Science-Poland 36, no. 3 (September 1, 2018): 387–96. http://dx.doi.org/10.1515/msp-2018-0029.

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AbstractIn the present paper, TL and PL study of Dy3+ doped Sr2SiO4:Eu2+ phosphor is reported. A polycrystalline sample of Sr2SiO4:Eu2+, Dy3+ was prepared by combustion method. The obtained phosphor was characterized by powder X-ray diffraction, scanning electron microscopy, UV-Vis spectroscopy, PL and thermoluminescence. The results of the XRD studies obtained for Sr2SiO4:Eu2+, Dy3+ phosphor revealed its monoclinic structure. The average crystallite size was calculated as 12.77 nm. Thermoluminescence study was carried out for the phosphor using UV irradiation and a single glow peak was found. The thermoluminescence glow curves of the samples were measured at various concentrations of co-dopant. The kinetic parameter has been calculated using Chen’s glow curve method. In this paper, the photoluminescence and afterglow behavior of these phosphors are reported.
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Singh, S. Dorendrajit, and S. Ingotombi. "Thermoluminescence glow curve of gamma -irradiated calcite." Journal of Physics D: Applied Physics 28, no. 7 (July 14, 1995): 1509–16. http://dx.doi.org/10.1088/0022-3727/28/7/032.

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Prakash, Jai. "Thermoluminescence glow curve with second order kinetics." Solid State Communications 85, no. 7 (February 1993): 647–50. http://dx.doi.org/10.1016/0038-1098(93)90326-i.

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AHN, J., B. GAN, Q. ZHANG, S. F. YOON, V. LIGATCHEV, S. G. WANG, Q. F. HUANG, K. CHEW, R. MELÉNDREZ, and M. BARBOZA-FLORES. "APPLICATION OF CVD DIAMOND FILMS FOR UV THERMOLUMINESCENCE DOSIMETER." International Journal of Modern Physics B 16, no. 06n07 (March 20, 2002): 1003–7. http://dx.doi.org/10.1142/s0217979202010762.

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This study presents the investigation of CVD diamond for the application of an UV TL dosimeter. A 9-μm-thick film used in this study presents a TL glow curve with a well-defined first-order kinetic peak (at about 273 K), which norm ally presents in the glow curve from ionizing radiations, is not observed. By fitting the glow curve to a first-order kinetic model, the trap activation energy E t = 0.95 eV and frequency factor s = 5.6 x 106 s -1 have been resolved.
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Kitis, G., R. Chen, V. Pagonis, E. Carinou, P. Ascounis, and V. Kamenopoulou. "Thermoluminescence under an exponential heating function: II. Glow-curve deconvolution of experimental glow-curves." Journal of Physics D: Applied Physics 39, no. 8 (March 30, 2006): 1508–14. http://dx.doi.org/10.1088/0022-3727/39/8/009.

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Vejnović, Z., M. Pavlović, P. Hadžić, and M. Davidović. "Glow curve analysis and calculation of thermoluminescence parameters." Scientific Publications of the State University of Novi Pazar Series A: Applied Mathematics, Informatics and mechanics 9, no. 2 (2017): 167–86. http://dx.doi.org/10.5937/spsunp1702167v.

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Dissertations / Theses on the topic "Thermoluminescence glow curve"

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Ferreira, Marcela Felix Chaves. "Implementação de uma análise computadorizada da curva de emissão termoluminescente e aplicação em dosimetria clínica." Universidade de São Paulo, 2018. http://www.teses.usp.br/teses/disponiveis/59/59135/tde-04062018-101047/.

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Nas décadas de 1960 e 1970, as primeiras investigações de dosímetros termoluminescentes (TLD), especificamente, os picos dosimétricos, rapidamente revelaram um número surpreendente de fenômenos que poderiam estar diretamente relacionados à densidade de ionização. Um pouco mais tarde, nos anos 80 e no início dos anos 90, a radiação aparentemente desconectada induziu fenômenos que foram descobertos em outros sistemas baseados em fluoreto de lítio (LiF). A última década, no entanto, testemunhou o surgimento de vários modelos, encabeçado através de uma compreensão mais profunda dos mecanismos TL subjacentes, bem como na modelagem micro dosimétrica e especificamente desenvolvida para explicar fenômenos de densidade de ionização. Muitas aplicações em radioterapia fornecem níveis de dose de radiação superiores a 1 Gy, porém em radiodiagnóstico estão na faixa de alguns mGy, e níveis muito altos de precisão são necessárias para promover o tratamento ideal. Isto exige uma atenção muito cuidadosa aos protocolos de medição altamente detalhados, bem como à calibração demorada de todos os TLDs para corrigir a não-linearidade da resposta à dose. Essas propriedades podem variar de lote para lote e também podem ser uma função da exposição à radiação, do aquecimento e histórico de manuseio. Deste modo, mesmo com excelentes avanços nos estudos do TLD com relação aos tratamentos térmicos e às formas de análise da curva de emissão TL, é necessário continuar os estudos a fim de possibilitar uma melhor utilização desta técnica na clínica. Uma análise computadorizada da curva de emissão (CGCA do inglês, computadorized glow curve analisys) foi implementada utilizando dados provenientes do software WinREMS de dosímetros TL que absorvem e armazenam a energia da radiação ionizante, reemitida na forma de fóton na região do ultravioleta visível. A luz emitida é, então, detectada por uma fotomultiplicadora e correlacionada à dose absorvida recebida pelo material. Os picos de emissão foram ajustados por meio de um algoritmo no programa MATLAB adotando-se o modelo de cinética de primeira ordem. O material testado foi o LiF:Mg,Ti (fluoreto de lítio dopado com magnésio e titânio) da marca Harshaw e a qualidade do ajuste foi determinada por um parâmetro chamado figura de mérito (FOM - do inglês, figure of merit). O menor FOM obtido para o grupo de dosímetros foi de 1,04 % e o maior foi de 9,79 %. Também foi avaliada a dose mínima detectável, utilizando o parâmetro que apresentou melhor desempenho, segundo a homogeneidade do grupo de dosímetros. O valor médio de dose mínima apresentado foi 28 µGy. Os resultados de reprodutibilidade, índice de variabilidade do detector (DVI - do inglês, device variability index) foi 14,01 %, que pode ser explicado pelo alto número de dosímetros no lote. Então, com a diminuição do tempo de preparo do dosímetro e com a análise computadorizada da curva de emissão, a utilização clínica do TLD torna-se mais viável, visto que não houve interferência na sensibilidade do dosímetro. Apesar de a reprodutibilidade ter sido a cima do esperado, é indicado uma correção individual para cada dosímetro e o descarte daqueles que apresentarem valores mais discrepantes comparado ao lote.
In the decades of 1960 and 1970, the first investigations of termoluminescentes dosimeters (TLD), specifically, the dosimetric peaks quickly revealed a surprising number of phenomena that could be directly related to the density of ionization. A little later, in the years 80 and 90 at the beginning of the year, seemingly disconnected radiation induced phenomena were discovered on other systems based on lithium fluoride (LiF). The last decade, however, has witnessed the emergence of several models, spearheaded through a deeper understanding of the underlying TL mechanisms as well as in modeling specifically developed for microdosimetric and explain phenomena of ionization density. Many applications in radiation oncology provide levels of radiation dose in excess of 1 Gy, however in diagnostic radiology are in the range of a few mGy, and very high levels of precision are necessary to promote the ideal treatment. This requires careful attention to the highly detailed measurement protocols, as well as the time-consuming calibration of all TLDs to correct the non-linearity of dose-response. These properties can vary from batch to batch, and can also be a function of exposure to radiation, heating and handling history. In this way, even with excellent advances in the studies of the TLD for the heat treatment and the ways of issuing TL curve analysis, it is necessary to continue studies in order to enable a better use of this technique in the clinic. A computerized analysis of the emission curve (CGCA computadorized glow curve analysis) was implemented using data from the WinREMS software of TL dosimeters that absorb and store energy from ionizing radiation, reissued in the form of photon in the visible ultraviolet. The light emitted is then detected by a photomultiplier and correlated to the absorbed dose received by the material. The emission peaks were adjusted by means of an algorithm in MATLAB program by adopting the model of first-order kinetics. The material tested was the LiF: Mg, Ti (lithium fluoride doped with magnesium and titanium) brand Harshaw and the quality of the fit was determined by a parameter called figure of merit (FOM- figure of merit). The smallest FOM obtained for the group of dosimeters was 1.04% and the highest was 9.79%. Also minimum detectable dose was evaluated, using the parameter that showed better performance, according to the homogeneity of the Group of dosimeters. The average value of minimum dose presented was 28 µGy. The results of reproducibility, index of variability of the detector (DVI-English, device variability index) was 14.01%, which can be explained by the high number of dosimeters in the batch. Then, with the decrease in the time of preparation of the dosimeter and the computerized analysis of the emission curve, the clinical use of the TLD becomes more viable, since there was no interference on sensitivity of the dosimeter. Although the reproducibility have been above expectations, indicated a single correction for each badge and the disposal of those who submit more discrepant values compared to the batch.
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Al-Maghrabi, Mufied Mahmoud. "Thermoluminescence spectra from sulphates, fluorides and garnets doped with rare earth ions." Thesis, University of Sussex, 2001. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.366054.

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Luminescence measurements have been applied to three different structures namely, sulphate, fluorides and YAG. In all cases the RE doping suppresses the intrinsic emission and results in intense luminescence characteristic of the RE dopant. Additionally, in double doped samples, or contaminated ones, the TL data show that each dopant defines a glow peak, which is displaced in temperature relative to the others. Examples of this were discussed for CaS04:Ce,Mn; YAG:Nd,Tb,Cr,Mn; BaF2:Ho,Ce and BaF2:Tm,Ce. The data are discussed in terms of an energy transfer model between different parts of extended defect complexes which encompass the RE ion and the lattice defects. Calcium sulphate doped with Dy define a TL peak near 200°C suitable for radiation measurements, but when co-doped with Ag the TL peak move to higher temperatures with minor effects on the peak sensitivity. In Ce,Mn double doped samples, the peak temperatures differ by -7°C between the Ce and Mn sites. The TL glow curves from alkaline earth fluorides are complex and contain several overlapping peaks. Curve fitting show that the peak maxima below room temperature are insensitive to the RE dopant. Additionally the host material has a modest effect on the peak positions. Above room temperature each dopant provides a TL curve specific to the added RE ion and do not show common peaks. Concentration has many effects on the resultant glow curve, and even at the lowest concentration used here (0.01%) there is evidence of cluster formation. Samples with high RE content show low values of the frequency factor consistent with the energy transfer model in that the emission from RE-RE cluster dominates over the emission from direct charge recombination within the defect complex. The effect of concentration and the TL mechanism operating below room temperature are also discussed. Luminescence signals from the near surface of YAG:Nd (via CL) were contrasted with those from the bulk material via RL. Results indicate that the outer few micron layers differ significantly in luminescence response from the bulk crystal. The differences were ascribed to result from solvents that enter the YAG lattice during the growth stage or subsequently from cleaning treatments via the dislocations caused by cutting and polishing. Additionally, the growth stage may include gases from the residual air in the growth furnace trapped into the YAG lattice. In each case there is a discontinuity in luminescence intensity and/or emission wavelengths at temperatures which mach the phase transitions of the contaminants. At the transition temperature there will be a sudden pressure change and this will induce surface expansion or bulk compression. The differences between the two cases were detected by the alternatives of CL and RL excitation, where the Nd or Er lines have moved in opposite directions. The detection of such low concentrations of solvents/trapped gases by luminescence is extremely difficult due to experimental limitations. Hence their role in luminescence generation is normally ignored.
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Perks, Christopher A. "Techniques for thermoluminescent glow-curve analysis and the dose response of individual glow peaks in '7LiF." Thesis, University of Sussex, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.334934.

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Kayhan, Mehmet. "Effects Of Synthesis And Doping Methods On Thermoluminescence Glow Curves Of Manganese Doped Lithium Tetraborate." Master's thesis, METU, 2009. http://etd.lib.metu.edu.tr/upload/3/12610667/index.pdf.

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In this study, differences in glow curves of Mn doped LTB powder samples synthesized with solid and wet synthesis methods and doped by using solid and wet doping techniques were investigated. Firstly, LTB was synthesized by using wet synthesis method which mainly comprises dissolution of reactants in water as solvent. Second way to produce LTB which was used in this study was solid synthesis method. In solid synthesis method, reactants were mixed in powder form. In the second part of the study, LTB produced by two different methods were doped with Mn and additionally Ag, Mg or P by using two different doping techniques. In order to see structural differences between differently synthesized and differently doped LTB samples which contained different amount of dopant powder X-Ray Diffraction (XRD) method was employed. Besides, FTIR (Fourier Transform Infrared) spectroscopy analyses were performed in order to detect differences in the bond structure caused by doping. Additionally, Inductively Coupled Plasma Optical Emission Spectrometer (ICP-OES) was used to determine the actual amount of dopant in LTB. Also morphological structures of samples were compared by using Scanning Electron Microscopy (SEM). Thermoluminescence measurements were performed with (TLD) Thermoluminescence Dosimeter equipment. XRD and FTIR analysis showed that syntheses of products were done in well success. Addition of dopants did not cause any changes in structural or bonding properties of LTB. It was possible to observe that, synthesis and doping methods and dopant concentration effect the thermoluminescence glow curves of doped LTB.
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PAIVA, FABIO de. "Estudo das respostas de TLD tipo LiF para caracterização de campos mistos." reponame:Repositório Institucional do IPEN, 2016. http://repositorio.ipen.br:8080/xmlui/handle/123456789/26930.

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Submitted by Marco Antonio Oliveira da Silva (maosilva@ipen.br) on 2016-12-21T15:11:54Z No. of bitstreams: 0
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A Terapia por Captura de Nêutrons, NCT (Neutron Capture Therapy) é uma técnica radioterápica em que a energia útil do tratamento vem da energia liberada em uma reação nuclear e não do feixe primário, como comumente utilizado em outros procedimentos radioterápicos. O Boro, por constituir-se em um elemento de baixa toxicidade e por apresentar um isótopo (10B) com alta seção de choque para a reação 10B(n,α)7Li tem sido o elemento mais utilizado nas pesquisas que visam o aprimoramento e a promoção desta técnica, derivando daí o termo BNCT (Boron Neutron Capture Therapy). Para fins de pesquisa em BNCT foi construída ao longo de um dos extratores de feixes (BH - Beam Hole) do reator IEA-R1 uma instalação, onde filtros e moderadores são posicionados entre o núcleo do reator e a posição de irradiação com o objetivo de modular o feixe de irradiação, otimizando a componente útil do feixe, os nêutrons térmicos, e reduzindo os contaminantes, raios gama e nêutrons em outras faixas energéticas. Tem-se realizado estudos visando a implementação de melhorias na caracterização e otimização do feixe obtido nesse arranjo instalado no BH-3. Atualmente a monitoração dos nêutrons é feita através de folhas de ativação, e a componente gama pelo TLD-400. Uma nova metodologia de monitoração tem sido estudada pelo grupo. A referida técnica consiste em usar TLDs de tipos diferentes, ou seja, que possuam sensibilidades distintas aos nêutrons térmicos, em virtude de diferenças na concentração dos isótopos de Lítio. No estudo dessa nova metodologia têm sido usados os TLD-600 e TLD-700. Este trabalho propõe uma metodologia usando o par TLD-100 e TLD-700. Inicialmente foi verificada a reprodutibilidade das respostas dos TLDs 700, 400 e 100 frente a campos gama puro e campos mistos, gama e nêutron. Campos estes obtidos em arranjos usando fontes de 60Co e 241AmBe. A partir de simulações usando o VI MCNP5 foi projetado e construído um Irradiador de campos mistos, que permitiu expor os dosímetros em campos mistos com diferentes espectros energéticos. As condições criadas no irradiador permitiram verificar, como a resposta do TLD é modificada pelas mudanças no espectro energético de um campo misto gama e nêutrons de baixo fluxo. O irradiador de campo misto permitiu condições para estabelecer uma relação entre o formato da curva termoluminescente e a composição do campo misto. A relação estabelecida relaciona o fluxo relativo e a razão entre a resposta das duas regiões de interesse dos TLDs 700 e 100. A partir de campos mistos com condições controladas, esse trabalho permitiu verificar a viabilidade do uso do par de TLD-100 e TLD-700 para monitoração de nêutrons térmicos na instalação de BNCT.
Dissertação (Mestrado em Tecnologia Nuclear)
IPEN/D
Instituto de Pesquisas Energéticas e Nucleares - IPEN-CNEN/SP
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Al-Hameed, Hiba Musadaq Salim. "Study on the application of phototransferred thermoluminescence to reassessment of radiation dose using MCP-N and MTS-N detectors." Phd diss., 2019. http://hdl.handle.net/11089/31816.

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The topic of a dissertation is to examine the impact of UV and thermal stimulation on the emission of thermoluminescence light using the PTTL (PhotoTransferred ThermoLuminescence) phenomenon, and consequently – the search for optimal stimulation conditions determining the accuracy of dose re-evaluation. Measurements were performed with the MTS-N (LiF:Mg,Ti) and MCP-N (LiF:Mg,Cu,P) dosimeters exposed to electromagnetic radiation with dose up to 1000 mGy for MTS-N and up to 25 mGy for MCP-N detectors. Using the TLD Reader-Analyser RA’04 the dependence of PTTL data reading performance on UV wavelength, irradiation time and temperature of detectors during UV irradiation was examined. Among all available UV wavelengths (254, 302 and 365 nm) the highest efficiency occurred at λ = 254 nm. Further measurements were carried out with this wavelength. The light emission efficiency of the detectors using the PTTL phenomenon was tested with the following stimulation parameters: – UV irradiation time: from 30 minutes to 8 hours for MTS-N and from10 minutes to 4 hours for MCP-N detectors, and – a heating temperature during UV irradiation: from 33 to 140 °C for MTS-N and from 30 to 120 °C for MCP-N detectors. The most important results relate to the usefulness of the PTTL method for the dose re-evaluation: PTTL reading performance, detector linearity, and an indication of optimal conditions for UV irradiation and thermal treatment of detectors. Studies have shown that the high sensitivity of MCP-N detectors in routine measurements of TL dosimetry is lost at repeated readings in PTTL mode.
Tematem rozprawy jest badanie wpływu parametrów stymulacji UV i termicznej na emisję światła z detektorów termoluminescencyjnych promieniowania jonizującego, z wykorzystaniem zjawiska termoluminescencji stymulowanej światłem (PTTL: PhotoTransferred ThermoLuminescence), a w konsekwencji – poszukiwanie warunków stymulacji optymalnych ze względu na dokładność ponownego (tzn. wykonywanego po pierwszym odczycie) wyznaczenia dawki. Pomiary były wykonywane z dozymetrami MTS-N (LiF:Mg,Ti) i MCP-N (LiF:Mg,Cu,P) napromieniowanymi promieniowaniem elektromagnetycznym o dawce do 1000 mGy dla MTS-N oraz do 25 mGy dla MCP-N. Za pomocą czytnika TLD Reader-Analyser RA’04 została zbadana zależność wydajności odczytu danych PTTL od długości fali promieniowania UV, czasu ekspozycji i temperatury detektorów w trakcie naświetlania UV. Spośród wszystkich dostępnych długości fal promieniowania UV (254, 302 i 365 nm) najwyższa wydajność detekcji wystąpiła przy λ = 254 nm. Dalsze pomiary były prowadzone ze stymulacją promieniowaniem UV o tej długości fali. Wydajność detekcji z wykorzystaniem zjawiska PTTL była badana przy następujących parametrach stymulacji: – czas ekspozycji na promieniowanie UV połączonej z nagrzewaniem detektorów: od 30 min. do 8 godz. dla detektorów MTS-N i od 10 min. do 4 godz. dla MCP-N, – temperatura ogrzewania w trakcie ekspozycji UV: od 33°C do 140°C dla detektorów MTS-N i od 30°C do 120°C dla MCP-N. Najważniejsze wyniki dotyczą przydatności metody PTTL do powtórnej oceny dawki: wyznaczenie wydajności odczytu PTTL, analiza liniowości wskazań detektorów, oraz wskazanie optymalnych warunków ekspozycji UV i obróbki termicznej detektorów TL. Badania wykazały, że wysoka czułość detektorów MCP-N w rutynowych pomiarach dozymetrycznych nie znajduje odzwierciedlenia w powtórnym odczycie, z wykorzystaniem zjawiska PTTL.
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Books on the topic "Thermoluminescence glow curve"

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Horowitz, Y. S. Computerised glow curve deconvolution: Application to thermoluminescence dosimetry. Ashford: Nuclear Technology Publishing, 1995.

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Book chapters on the topic "Thermoluminescence glow curve"

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Tripathi, Shubha, Vikarm Awate, K. K. Kushwah, Ratnesh Tiwari, and Nigama Prasan Sahoo. "Novel Tool to Determine Kinetic Parameters of Thermoluminescence (TL) Glow Curve—CGCD: CaZrO3: Eu3+, Tb3+." In International Conference on Intelligent Computing and Smart Communication 2019, 795–803. Singapore: Springer Singapore, 2019. http://dx.doi.org/10.1007/978-981-15-0633-8_82.

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Sunta, C. M. "Kinetics Analysis of TL Glow Curves." In Unraveling Thermoluminescence, 77–102. New Delhi: Springer India, 2014. http://dx.doi.org/10.1007/978-81-322-1940-8_4.

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Sunta, C. M. "Thermal Stimulation of Luminescence and Theory of the Glow Curves." In Unraveling Thermoluminescence, 29–75. New Delhi: Springer India, 2014. http://dx.doi.org/10.1007/978-81-322-1940-8_3.

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Awate, Vikram, Lokeshwar Patel, Rashmi Sharma, A. K. Beliya, Ratnesh Tiwari, Vikas Dubey, and Neha Dubey. "Thermoluminescence Glow Curve Analysis of Mn4+-Doped Barium Yttrium Oxide Phosphor." In Luminescence, 211–14. De Gruyter, 2021. http://dx.doi.org/10.1515/9783110676457-008.

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Dubey, Vikas, Neha Dubey, Jagjeet Kaur, Jyoti Singh, T. Ramarao, Manoj Pandey, and Sanjay J. Dhoble. "Thermoluminescence glow curve analysis and proposed model for rare-earth activated some oxide-based phosphors for dosimetric application." In Radiation Dosimetry Phosphors, 299–327. Elsevier, 2022. http://dx.doi.org/10.1016/b978-0-323-85471-9.00003-8.

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"ANALYSIS OF TL GLOW CURVES." In Theory of Thermoluminescence and Related Phenomena, 85–150. WORLD SCIENTIFIC, 1997. http://dx.doi.org/10.1142/9789812830890_0003.

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Conference papers on the topic "Thermoluminescence glow curve"

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Ghomeishi, Mostafa, Peyman Jahanshahi, Elian Dermosesian, and Faisal Rafiq M. Adikan. "Analysis of optical fibre defects using thermoluminescence glow curve method." In 2014 IEEE 5th International Conference on Photonics (ICP). IEEE, 2014. http://dx.doi.org/10.1109/icp.2014.7002336.

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Yerpude, M. M., and S. J. Dhoble. "Thermoluminescence glow curve analysis of RE doped LiMgBO3 phosphor using GCCD function." In INTERNATIONAL CONFERENCE ON “MULTIDIMENSIONAL ROLE OF BASIC SCIENCE IN ADVANCED TECHNOLOGY” ICMBAT 2018. Author(s), 2019. http://dx.doi.org/10.1063/1.5100470.

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Tiwari, Ratnesh, and Seema Chopra. "Thermoluminescence glow curve analysis and CGCD method for erbium doped CaZrO3 phosphor." In INTERNATIONAL CONFERENCE ON CONDENSED MATTER AND APPLIED PHYSICS (ICC 2015): Proceeding of International Conference on Condensed Matter and Applied Physics. Author(s), 2016. http://dx.doi.org/10.1063/1.4946722.

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Shivaramu, N. J., B. N. Lakshminarasappa, K. R. Nagabhushana, E. Coetsee, and H. C. Swart. "Correlation between thermoluminescence glow curve and emission spectra of gamma ray irradiated LaAlO3." In DAE SOLID STATE PHYSICS SYMPOSIUM 2017. Author(s), 2018. http://dx.doi.org/10.1063/1.5028766.

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Fadzil, Muhammad S. A., Ung N. Min, Alawiah Ariffin, David A. Bradley, and Noramaliza M. Noor. "Evaluation on Thermoluminescence Kinetic Parameters of Ge-Doped Cylindrical Fibre Dosimeter by Computerised Glow Curve Deconvolution Technique." In Proceedings of the Second International Symposium on Radiation Detectors and Their Uses (ISRD2018). Journal of the Physical Society of Japan, 2019. http://dx.doi.org/10.7566/jpscp.24.011036.

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Ionescu, C., E. Pajuste, J. Prikulis, M. Dima, S. Sokovnin, and P. Krug. "Modelling glow curves of thermoluminescent radiometric devices." In 2017 IEEE 23rd International Symposium for Design and Technology in Electronic Packaging (SIITME). IEEE, 2017. http://dx.doi.org/10.1109/siitme.2017.8259893.

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Armstrong, Philip R., Merlin L. Mah, Lucas Taylor, and Joseph J. Talghader. "Reduced blackbody microheaters for measuring high temperature thermoluminescent glow curve peaks." In 2014 International Conference on Optical MEMS and Nanophotonics (OMN). IEEE, 2014. http://dx.doi.org/10.1109/omn.2014.6924512.

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Hassan, M. F., W. N. W. A. Rahman, A. B. A. Kadir, N. M. Isa, T. Tominaga, M. Geso, H. Akasaka, D. A. Bradley, and N. M. Noor. "Fabricated Ge-doped flat optical fibres: Assessing the thermoluminescence glow curves for proton beam irradiation." In 4TH ELECTRONIC AND GREEN MATERIALS INTERNATIONAL CONFERENCE 2018 (EGM 2018). Author(s), 2018. http://dx.doi.org/10.1063/1.5080897.

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