Made available in DSpace on 2014-10-09T12:29:45Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:00:04Z (GMT). No. of bitstreams: 1 00456.pdf: 1075435 bytes, checksum: 5890a1018150d05979ee39919f44ca34 (MD5) / Dissertacao (Mestrado) / IEA/D / Instituto de Energia Atomica - IEA

Made available in DSpace on 2014-10-09T12:29:50Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:00:27Z (GMT). No. of bitstreams: 1 00968.pdf: 911616 bytes, checksum: e0c8f486a6db58c7bd4da508c15517cf (MD5) / Dissertacao (Mestrado) / IEA/D / Instituto de Energia Atomica - IEA

Made available in DSpace on 2014-10-09T12:24:18Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:04:26Z (GMT). No. of bitstreams: 1 00508.pdf: 1394827 bytes, checksum: 4841c122d3cfa0b91639516519105971 (MD5) / Dissertacao (Mestrado) / IEA/D / Instituto de Fisica, Universidade de Sao Paulo - IF/USP

Made available in DSpace on 2014-10-09T12:23:47Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:06:36Z (GMT). No. of bitstreams: 1 01265.pdf: 3555927 bytes, checksum: 1f15fc90d6320240cb55282e4d484224 (MD5) / Tese (Doutoramento) / IEA/T / Instituto de Fisica, Universidade de Sao Paulo - IF/USP

Made available in DSpace on 2014-10-09T12:25:56Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:06:38Z (GMT). No. of bitstreams: 1 00993.pdf: 5816029 bytes, checksum: 8d66be3f85d993bc132e70054181033d (MD5) / Thesis (Doctorate) / IPEN/T / University of Washington - Wash

Made available in DSpace on 2014-10-09T12:41:02Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:09:42Z (GMT). No. of bitstreams: 1 04028.pdf: 4334494 bytes, checksum: 3b9778498dc6bdac0e8a5c8f8ad038da (MD5) / Tese (Doutoramento) / IPEN/T / Instituto de Pesquisas Energeticas e Nucleares - IPEN/CNEN-SP

No presente trabalho, foi montado um sistema de eletrodifusão para o estudo dos efeitos da substituição de íons alcalinos, presentes no canal estrutural, por íons de hidrogênio (H POT. +), nas propriedades termoluminescentes e ópticas do quartzo. A corrente elétrica de eletrólise apresenta, na parte inicial de aquecimento, um ombro ou pico de corrente. Através da análise do comportamento deste pico e informações obtidas de dados de absorção óptica na região espectral do infravermelho, concluiu-se que o pico presente na curva inicial de eletrólise se deve ao complexo [AL POT. 3+/M POT. +]. As medidas de termoluminescência e absorção óptica na região espectral do visível e ultra-violeta foram feitas em amostras de quartzo eletrodifundidos e não eletrodifundidos e chegou-se à proposição de uma reação envolvendo os alcalinos presentes no canal. Nesta reação, os íons alcalinos fazem o papel de centros armadilhadores de íons de oxigênio O POT. produzidos pela radiação ionizante, e estabilizadores de vacâncias de oxigênio. O aquecimento, em tomo de 300 GRAUS C, provoca a desestabilização desses centros armadilhadores, liberando os íons alcalinos que reagem com os defeitos [ALO IND. 4] POT. 0 emitindo luz TL. Aproveitando a existência de canais estruturais, semelhantes ao quartzo, tentou-se eletrodifundir H POT + no berilo. Através de medidas de termoluminescência e corrente inicial de eletrólise, discute-se a possibilidade da existência do defeito [FE POT. 3+/M POT. +] no berilo. / A system of electrodiffusion was made in the laboratory to investigate effects of exchanging alkali ions, usually present in the structural channels by protons, in the optical and thermoluminescent properties of quartz. In the initial part of heating, the sweeping current presents a peak at about 350 GRAUS C. The analysis of the behaviour of this peak with additional data of optical absorption in the region of infrared, it was concluded that the peak at 350 GRAUS C of the current is due to [AL POT. 3+/M POT. +] system. Thermoluminescence and optical absorption spectra in the visible and ultraviolet light region for swept and unswept quartz were compared. Based on this comparison it was shown that, once irradiated to gama- or X-rays, alkali ions are removed from [AL POT. 3+/ M POT. +] and either couple to o ions or capture electron and become interstitial alkali atom, leaving, further, [ALO IND. 4] POT. 0 hole center. Heating at about 300 GRAUS C electrons from M POT 0 or M POT +O POT recombine with holes in [ALO IND. 4] POT. 0, emitting TL light, besides regrouping Al POT. 3+ and M POT. + to reform [Al POT. 3+/M POT. +] system by coulomb attraction. The electrodiffusion experiment was extended to beryl crystal, because beryl has also structural channels. To explain initial sweeping current behaviour as well as thermoluminescent property a mechanism involving [FE POT. 3+/M POT. +] system is proposed.

Carbon-doped aluminium oxide, α-Al₂O₃:C, is a ultra-sensitive dosimeter of topical research interest. The aim of this project was to investigate the dynamics of luminesce in this material. The methods of investigation consisted of thermoluminescence and time-resolved optical stimulation. Thermoluminescence measurements provide information on trap distribution and kinetic parameters of the traps involved in luminescence whereas time-resolved optical stimulation is a handy technique in investigation of luminescence lifetimes and provides an insight into the charge transitions between traps and recombination centres. Measurements were made on samples annealed at a nominal temperature of 900⁰C for 15 minutes. The material shows the presence of five thermoluminescence peaks at 37⁰C, 160⁰C, 300⁰C 410⁰C, and 480⁰C at a heating rate of 0.03k/s when irradiated to 6.0 Gy of beta. The main peak at 160⁰C, shows a linear dose response for doses between 0.1 Gy and 10 Gy and then goes sublinear above 10 Gy, the peak at 37⁰C shows a sublinear dose response for doses between 0.1 Gy and 10 Gy and appears to saturate thereafter, whereas the dose response of the peak at 300⁰C goes from linear to supralinear then apparently quadratic behaviour in the dose range of 0.1 Gy to 16.0 Gy. The trap depth of the main peak, that is, its activation energy as determined below the conduction band, has been approximated at 1.3 eV with a kinetic order of approximately 1.2. Time-resolved optical stimulation has been used to investigate luminescence lifetimes. The mean luminescence lifetime obtained for the sample at ambient temperatures is 35.0±1.0 ms. The investigations of the dependence of luminescence lifetimes on measurement temperature show that the material suffers from thermal quenching effects at measurement temperatures above 140⁰C with the activation energy of thermal quenching estimated at 1.045±0.002 eV. Shallow traps i.e. traps lying close to the conduction band, seem to elongate the lifetimes of optically stimulated luminescence in the material at temperatures between 30⁰C - 80⁰C due to charge retrapping. The material exhibits both fading and recuperation of the optically stimulated luminescence signal with storage time.

L'intérêt des matériaux scintillateurs est la conversion de rayonnements de hautes énergies (particule γ, particules α, électrons,...) en photons de basse énergie détectables par les photo-détecteurs habituels. Ils sont utilisés dans de nombreuses applications : recherche en physique des hautes énergies, spectrométrie gamma pour la recherche ou la radio-protection, imagerie médicale ou technique, ainsi que pour la sécurité intérieure. Les propriétés de scintillation de ce type de matériau sont dépendantes de l'historique d'irradiation. Ce comportement, appelé effets mémoire, influe directement sur les performances des instruments utilisant ces matériaux. Trois effets mémoire différents peuvent être distingués : le vieillissement qui est une diminution du rendement de scintillation après une absorption de rayonnements ionisants, la rémanence qui est la persistance de l'émission lumineuse après la fin de l'excitation, et enfin la radio-sensibilisation qui est une augmentation, temporaire ou non, du rendement de scintillation en fonction de la dose absorbée par le scintillateur. Ce travail s'attache principalement à la compréhension du phénomène de radio-sensibilisation et à la rémanence dans les scintillateurs. Un matériau modèle, YP O4 : Ce, N d, a été utilisé afin de mettre en évidence la corrélation entre les pièges électroniques présents dans le matériau et les effets mémoire. Une fois ce lien mis en évidence, une étude sur un matériau commercial largement utilisé dans de nombreuses applications, l'iodure de césium dopé thallium, a été menéee. Sur la base de mesures de thermoluminescence, un modèle numérique a été développé afin de simuler les effets mémoire dans ces matériaux, puis de prédire leurs comportements en cas de modification des pièges électroniques. Par ailleurs, des méthodes de réduction des effets mémoire ont été étudiées via l'introduction de nouveaux pièges aux caractéristiques précises ou via la stimulation optique du matériau en parallèle de son irradiation / The interest of scintillating materials is the conversion of high energy radiations (γ or α particles, electrons, ...) in low energy photons detectable by usual photo-detectors. They are used in many applications : research in high energy physics, gamma spectrometry for research or radiation protection, medical and technical X-ray imaging, as well as for homeland security. The scintillation properties of this materials is dependent on the history of irradiation. This behavior, called memory effect, directly affects the performance of instruments using these materials. Three different memory effects can be distinguished : aging is a decrease in the scintillation yield after an absorption of ionizing radiation, the afterglow is the persistence of light emission after excitation, and finally radio-sensitization which is an increase of scintillation yield depending on the dose absorbed by the scintillator. This work mainly focus on the understanding of radio-sensitization phenomenon and afterglow in the scintillators. A model material, Y PO4 : Ce,Nd, was used to highlight the correlation between charges carrier traps present in the material and memory effects. Once this link is highlighted, a study of a commercial material widely used in many applications, thallium doped cesium iodide, was lead. Based on thermoluminescence measures, a numerical model was developed to simulate the memory effects in these materials and to predict their behavior in case of modification of charge carrier traps. Furthermore, several methods to reduce memory effects were investigated through the introduction of new traps with specific characteristics or through optical stimulation of the material in parallel to its irradiation. Finally, the role of radiosensitization in the scintillation efficiency under gamma excitation was highlighted on BaAl4O7 : Eu2+ ceramics. These results suggest a way to improve performance of some scintillating performance by the exaltation via prior irradiation

Les structures de combustion constituent un témoin de la fréquentation humaine et leur étude permet d’appréhender un aspect du mode d’occupation d’un lieu donné. Ainsi, pour compléter les approches classiques qui s’intéressent à la typologie des foyers, à la fréquence des feux, à la nature des combustibles, etc., une caractérisation thermique de ces structures a été proposée. Elle s’appuie sur les impacts thermiques enregistrés par les sédiments soumis aux feux et plus précisément sur les modifications des propriétés de thermoluminescence (TL) et de magnétisme avec la chauffe.Le site-laboratoire est celui de la grotte de Fraux (Dordogne), occupée à l’Âge du bronze, dont le statut et le mode d’occupation pose question puisqu’elle présente tant des vestiges domestiques (sols de circulation, foyers, mobiliers) que des vestiges symboliques (manifestations pariétales, dépôts de mobilier). La place importante des foyers parmi ces vestiges a induit une étude spécifique de ces structures. En effet, ce site recèle plus d’une soixantaine de structures de combustion et, aspect important pour notre approche archéométrique, présente un état de conservation exceptionnel puisque la grotte est restée fermée depuis l’occupation de l’Âge du bronze.L’étude de certains foyers de la grotte des Fraux a permis de tester le potentiel de paléothermomètres fondés sur ces deux propriétés indépendantes à savoir la TL des grains de quartz et le magnétisme des oxydes de fer contenus dans les sédiments. Le paléothermomètre TL a été élaboré en comparant les signaux TL d’échantillons provenant de foyers archéologiques à ceux de références thermiques chauffées en laboratoire. Pour le magnétisme deux pistes ont été exploitées : les températures de déblocage de l’aimantation rémanente et l’évolution de la signature magnétique -minéralogie et taille de grain) avec la chauffe. La détermination des paléotempératures atteintes par les sédiments substrats des structures de combustion apporte une première indication sur leur intensité de chauffe. Afin d’étalonner ces informations paléothermométriques en termes d’énergie mise en jeu, des feux expérimentaux ont été réalisés. Ils ont permis de comparer les impacts thermiques entre feux archéologiques et feux expérimentaux, de construire un échantillonnage d’histoire thermique connue, mais aussi d’estimer les températures atteintes, les épaisseurs de sédiments affectés, les quantités de combustibles consommés pendant un temps donné, la quantité d’énergie dégagée par la combustion… Ces expérimentations ont aussi servi de base à une modélisation de la propagation de la chaleur dans les sédiments. Les simulations effectuées dans ce modèle numérique permettent alors d’estimer un temps minimal de fonctionnement des structures de combustion.Nous disposons ainsi d’un nouvel outil pour la caractérisation thermique de foyers archéologiques. / The study of the combustion structures, which are a remaining evidence of the human occupation, can give information about the way of occupation of a site. In this research we decided to complete the classical approaches of combustion structures generally based on typological description of hearths, frequency of fires, nature of fuel, etc. by a a thermal characterisation. This study deals with the thermal impacts recorded by the fired sediment. More precisely, the modifications of both thermoluminescence (TL) and magnetism properties with heating were investigated.The laboratory-site is the cave of Les Fraux (Dordogne, France) which was occupied in the Bronze Age. The archaeologists were wandering about the function and the way of occupation of this cave because of the existence of both domestic vestiges (archaeological occupation grounds, hearths, and ceramics) and symbolic evidences (rock art and votive ceramic deposition). A specific study of the combustion structures had started considering the significant number of hearths, more than sixty, and their importance in the human occupation. In addition, as the cave remained closed since the Bronze Age, the hearths are in an excellent state of conservation and that is an important point for our archaeometric study. The thermal characterisation of some hearths from the cave of Les Fraux firstly consisted in studying the paleothermometer potential of two properties: the thermoluminescence of quartz grains and the magnetism of iron oxides taken from the sediments. The TL paleothermometer was established by comparing TL signals of samples from archaeological hearths and those of thermal references heated in laboratory. Two properties were explored for the magnetic paleothermometer: the unblocking temperatures of the remanent magnetization and the evolution of magnetic signature (mineralogy and grain size) with heating. The paleotemperatures determined for the sediment of the hearths give a first information about the heating intensity of fires.Then experimental fires were carried out to calibrate paleothermometric data in quantity of energy and wood consumption, to check the suitability of laboratory thermal references, and to characterise the process of heat transfer inside the sediment. Finally, a numerical modeling of heat propagation within the sediment was implemented from temperatures recorded during fire experimentations. Numerical simulations performed in this model allowed us to estimate a minimal duration of functioning of the combustion structures.A novel tool for the thermal characterisation of combustion structures is then available.