De nos jours, les dosimètres existants sont insuffisants pour la surveillance et le contrôle des rayonnements ionisants dans toutes les configurations et surtout en environnement sévère. En dosimétrie optique, les systèmes fibrés permettent de répondre en temps réel à des débits de dose relativement faibles, de réaliser des mesures dans des endroits difficiles d’accès, avec une résolution spatiale intéressante. Ce travail a consisté en l’étude de verres de silice élaborés par voie sol-gel et dopés par du cuivre ou du cérium ionique, en vue de les utiliser dans un dispositif dosimétrique. Ces verres ont été caractérisés par différentes techniques spectroscopiques avant et après irradiations. Dans le cas des verres dopés Cu, après irradiation X ou γ (1 MGy), les défauts HC1, HC2 et E’ ont été identifiés. Quant aux verres dopés Ce, ils sont plus résistants et restent incolores, même après une dose de 8,8 MGy sous X. Des mesures de la réponse optique des échantillons sous rayons X ont été réalisées grâce à un dispositif fibré. Concernant les verres dopés Cu, la sensibilité en radioluminescence (RL) couvre la gamme de débits de doses allant de 0,25 à au moins 800 mGy/s et la linéarité de la luminescence optiquement stimulée (OSL) a été démontrée entre 40 mGy et 200 Gy. Les verres dopés Ce sont plus performants en termes de linéarité. En effet, les signaux de RL et d’OSL sont linéaires jusqu’à 1,2 Gy/s et 500 Gy respectivement pour ce dopant. Un fading de l’OSL à court-terme a été mis en évidence avant stabilisation du signal. Les résultats obtenus montrent que ces verres dopés présentent un grand intérêt pour la dosimétrie fibrée de radiations ionisantes. / Nowadays, existing dosimeters are insufficient for monitoring and control of ionizing radiation in all configurations and especially in severe environments. In optical dosimetry, fiber systems allow to provide a real-time response to relatively low dose rates, making possible some measurements in hard-to-reach places with interesting spatial resolution. This work consisted in the study of sol-gel silica glasses doped with ionic copper or cerium, with the aim of using them in a dosimetry device. These glasses have been characterized by different spectroscopic techniques before and after irradiations. In the case of Cu-doped glasses, after X or γ irradiation (1 MGy), the defects HC1, HC2 and E' have been identified. As for Ce-doped glasses, they are more resistant and remain colorless, even after a dose of 8.8 MGy under X. Measurements of the optical response from the samples under X-rays were carried out using a fibered device. For Cu-doped glasses, radioluminescence (RL) sensitivity covers dose rates ranging from 0.25 to at least 800 mGy/s and the linearity of optically stimulated luminescence (OSL) has been demonstrated in the range 40 mGy-200 Gy. Ce-doped glasses are more efficient in terms of linearity. Indeed, for this dopant, RL and OSL signals are linear up to 1.2 Gy/s and 500 Gy, respectively. Short-term OSL fading was observed before stabilization of the signal. The obtained results show that these doped glasses are of great interest for fibered dosimetry of ionizing radiations.

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Ce travail porte sur l'étude de nanoparticules scintillatrices qui sont capables, par définition, de convertir un rayonnement ionisant en lumière visible ou proche UV. Si le processus de scintillation est actuellement bien connu dans le cas des matériaux macroscopiques, les perturbations susceptibles d'apparaître pour des nanomatériaux le sont moins. En effet, des modifications peuvent être induites par le confinement spatial et les spécificités de structure propres aux nanomatériaux. L'étude de ces perturbations constitue l'objet de cette thèse. Le manuscrit se divise en trois parties. La première vise à quantifier la fraction d'énergie qui se dépose dans une assemblée de nanoparticules après interaction avec un photon haute énergie (X ) ou en réalisant des simulations Monte Carlo basées sur le code de calcul Geant4. La deuxième partie présente un travail expérimental exploratoire qui consiste à comparer des mesures de spectroscopie résolue en temps pour des nanoparticules et un monocristal afin d'extraire des informations sur les étapes de thermalisation et de recombinaison radiative spécifiques aux nanoparticules. La dernière partie de ce manuscrit présente l'étude d'une application novatrice des nanoscintillateurs comme agents thérapeutiques. Ils sont alors utilisés pour activer sous excitation X l'effet photodynamique, base d'une thérapie anti-cancéreuse actuellement limitée au traitement de lésions superficielles / This work deals with scintillating nanoparticles, material able to convert ionizing radiations into visible or Ultra-Violet light. The scintillation process is currently well-known for bulk materials. However, for nanomaterials, several steps of the scintillation process are likely to be slightly modified mainly because of the spatial confinement of charges and the structure specificities in nanomaterials. The study of such perturbations is the aim of this thesis. The manuscript is divided into three parts. The first one aims to quantify the amount of deposited energy within a set of nanoparticles after the interaction with a high energy photon (X or –rays). We thus developed Monte Carlo simulations with the Geant4 toolkit to quantify this energy. The second part presents an exploratory experimental study that consists in comparing time resolved spectroscopy measurements for nanoparticles and a single crystal. The aim is to extract a few tendencies on the thermalization and on the radiative recombination processes specific to nanoscintillators. The last part of this thesis presents an application of nanoscintillators as therapeutic agents. In that case, they are used to activate the photodynamic effect under X-ray irradiation. This last effect is the basis of the photodynamic therapy, an anticancer treatment currently limited to superficial tumors

This research explores the synthesis of anthracene and stilbene-based metal-organic framework (MOF) structures as potential scintillating (radioluminescent) materials for use in the detection of gamma radiation. The organic molecules 9,10-anthracenedicarboxylic acid (ADCH2) and trans-4,4’-stilbenedicarboxylic acid (SDCH2), were each used as a linker, in combination with a range of lanthanide metal ions, to synthesize novel three dimensional MOF structures under hydrothermal conditions. With ADCH2, the early period lanthanides yield isostructures with the metal ion in higher coordination (nine) than for those with late period metals (seven). The ADC-MOFs show linker-based photoluminescence properties with well defined vibronic peaks in their emission profile and their emission (λmax~435 nm) blue shifting from that of the ADCH2 powder (~500 nm) and closer to the organic molecule in monomer arrangement (λmax ~ 420 nm). The structures also show photoluminescence lifetimes between 1 and 2 ns, which is similar to the reported value for monomeric anthracene units. The blue-shift and reduction in lifetime, compared to ADCH2, are indicative of minimal π-π interactions amongst the aromatic moieties, thereby limiting the non-radiative relaxation pathways. On exposure to ionizing radiation (protons and g- rays), the ADC-MOFs demonstrated scintillation properties, with a radioluminescence lifetime of ~ 6 ns which is similar to that of the ADCH2 powder. A combination of SDCH2 and lanthanide metal ions produced two isostructured MOFs containing Tm3+ and Er3+, under the hydrothermal synthesis conditions explored. The 3-D structure contained ultra large diamond-shaped pores with dimensions of 16 Å x 30 Å. A blue-shift of fluorescence spectra was observed for the SDC-MOF structures (λmax ~ 425 nm) compared to that of bulk SDCH2 powder (λmax ~475 nm), and closely resembling that of monomeric isolated SDC units (λmax~475 nm). Their photoluminescence lifetime is ~0.76 ns, about half of that observed for SDCH2 powder. The blue shift and reduction in lifetime (compared to SDCH2) is attributed to minimal π-π interactions between SDC units in the MOF structure, thus minimizing associated non-radiative relaxation pathways. The isolation of anthracene and stilbene in MOF structures therefore has the potential to improve their performance as scintillators.

Les données chronologiques disponibles pour les gisements du Paléolithique moyen du Sud-Ouest de la France font état d’un manque de jalons chronologiques fiables. Pour ces périodes anciennes, l’établissement d’un cadre chronologique nécessite un investissement méthodologique important dans le domaine de la datation numérique. Les résultats obtenus dans cette étude reposent essentiellement sur la datation par luminescence optique de grains de feldspaths et de quartz contenus dans les sédiments. En particulier, l’étude des signaux de luminescence classiquement exploités (IRSL, pIR-IRSL), nous permet de mieux évaluer la fiabilité des datations à partir des feldspaths potassiques. Un protocole de datation fondé sur l’exploitation du signal de radioluminescence (IR-RF) de ces minéraux a aussi été développé. Ainsi, la luminescence optique a été appliquée à des échantillons provenant de six gisements de référence : Les Pradelles (Marillac, Charente), Combe Brune 2 (Creysse, Dordogne), Roc de Marsal (Campagne, Dordogne), Artenac (Saint-Mary, Charente), La Quina (Gardes-le-Pontaroux, Charente) et La Ferrassie (Savignac-de-Miremont, Dordogne). La combinaison des résultats obtenus nous a permis, au sein de chaque niveau archéologique, d’évaluer la pertinence des datations et de proposer pour chaque gisement un scénario chronologique qui nous semble fiable. À l’issue de cette étude, les occupations humaines, caractérisées selon leurs industries, ont pu être replacées sur une échelle des temps en regard des variations paléoclimatiques et paléoenvironnementales régionales. Plusieurs constats ont été dressés enrichissant le registre de nos connaissances sur les cultures néandertaliennes. / Currently available chronological information for Middle Palaeolithic sites in southwestern France precludes the establishment of a robust chronological framework. For these early periods, developing such a framework relies upon important methodological advancements in numerical dating techniques. The results of this study are essentially based on the optical luminescence dating of sedimentary feldspars and quartz. Focusing on the most commonly employed luminescence signals (IRSL, pIR-IRSL), it was possible to more clearly evaluate the reliability of dates obtained on K-feldspars. A dating protocol for these materials based on their radioluminescence signal (IR-RF) was also developed. Optical luminescence dates were produced for six major archaeological sites: (Marillac, Charente), Combe Brune 2 (Creysse, Dordogne), Roc de Marsal (Campagne, Dordogne), Artenac (Saint-Mary, Charente), La Quina (Gardes-le-Pontaroux, Charente) et La Ferrassie (Savignac-de-Miremont, Dordogne). Collating the results for each archaeological level allowed the coherence of the dates to be tested and a reliable chronological sequence to be proposed for each site. The different human occupations, characterised by their industrial attribution, could be placed within a chronological framework that incorporates regional palaeoenvironmental and palaeoclimatic variations. Finally, several observations provide new insights for our understanding of Neandertal cultures.

In this work, initially the radioluminescence (RL) and thermoluminescence (TL) techniques are presented. The radioluminescence is the prompt luminescence emitted by a material under ionizing radiation exposure. The thermoluminescence is the luminescence emitted by a material previously exposed to ionizing radiation when excited by heat. Enegy bands concepts, defects in crystals and the different processes of ionization that take place in matter when exposed to ionizing radiation are briefly discussed in order to present the mechanisms involved in RL and TL processes. The usage of the techniques in characterization of materials and dosimetry is reported, legitimating the importance of the instrument developed. Mechanical and structural parts as well as a description of each component of the instrument are fairly described. The implemented algorithm for controlling the instrument and acquiring data is also discussed. The development of the instrument enabled us to generate temperature ramps with a quite good performance, reaching temperatures up to 500 °C with deviations up to 2 °C, having used heating rates between 0.5 °C/s and 5 °C/s. Calibrations of optical spectrometer used in light collection and irradiation system were carried out. Lastly, TL and RL spectra tests were performed. The RL tests were carried out using several materials which emission spectra are well known by literature, namely, carbon-doped aluminium oxide Al2O3:C, terbium-doped gadolinium oxysulphide Gd2O2S:Tb, europium-doped yttrium oxide Y2O3:Eu and dysprosium-doped calcium borate CaB6O10:Dy. For the TL spectra test, the aluminium oxide doped with carbon Al2O3:C was used. The results of RL and TL spectra tests showed a good agreement with the literature, pointing out that the instrument developed in this work is comparable to others instruments in operation from others research groups, making our results reliable. / Nesse trabalho, inicialmente as técnicas de radioluminescência (RL) e termolumi- nescência (TL) são apresentadas. A radioluminescência é a luminescência imediata emitida por um material quando exposto à radiaçao ionizante. A termoluminescência é a luminescência emitida por um material previamente exposto à radiação quando este é aquecido. Conceitos de bandas de energia, defeitos em cristais e os diferentes processos de ionização que ocorrem na matéria quando exposta à radiação ionizante são brevemente discutidos a fim de apresentar os mecanismos envolvidos na RL e TL. A utilização das técnicas na caracterização de materiais e na dosimetria é reportada, justificando a importância do instrumento desenvolvido. As partes mecânicas/estruturais e uma descrição de cada componente do instrumento são descritos. O algoritmo implementado para controle do instrumento e aquisição de dados é também descrito. O desenvolvimento do instrumento possibilitou a geração de rampas de temperatura com uma boa performance, atingindo até 500 °C com variações de até 2 °C ao utilizar taxas de aquecimento entre 0.5 °C/s e 5 °C/s. Calibrações do espectrômetro óptico utilizado na aquisição da luminescência e do sistema de irradiação foram executadas. Por fim, testes de aquisição de espectros de RL e TL foram realizados. Os testes de RL foram realizados utilizando vários materiais cujos espectros de emissão são bem conhecidos pela literatura, a saber, óxido de alumínio dopado com carbono Al2O3:C , oxisulfeto de gadolínio dopado com térbio Gd2O2S:Tb , óxido de ítrio dopado com európio Y2O3:Eu e borato de cálcio dopado com disprósio CaB6O10:Dy. Para o teste dos espectros de TL, o Al2O3:C foi utilizado. Os resultados dos espectros de RL e TL mostraram concordância com a literatura, indicando que o instrumento desenvolvido é comparável a outros instrumentos em operação de outros grupos, tornando os nossos resultados confiáveis.

Os objetivos deste trabalho foram a implantação e a otimização da técnica de sinterização a laser de corpos cerâmicos, o estudo da cinética do processo e a avaliação de propriedades físicas dos compostos Bi4Ti3O12 e Bi4Ge3O12 sinterizadas a laser, em comparação com as cerâmicas processadas em forno convencional. A escolha dos materiais baseou-se em seu potencial de aplicação: o Bi4Ge3O12 como dispositivo cintilador e o Bi4Ti3O12 como cerâmica eletrônica. A sinterização a laser mostrou-se eficiente para estes materiais, produzindo cerâmicas com densidade superior a 98 % e pequeno tamanho de grão. A combinação de pré-aquecimento e subida gradual da potência do laser evitou gradientes de temperatura e taxas de aquecimento excessivos, e reduziu consideravelmente a incidência de trincas e a porosidade nas cerâmicas. No estudo cinético da sinterização a laser, registraram-se energias de ativação inferiores às observadas no processamento convencional, exceto para o BIT no estágio final de sinterização, e os resultados sugerem um adiantamento no processo de sinterização, provocado por efeito da irradiação a laser. A caracterização física do BIT foi feita por espectroscopia de impedância e medidas de histerese ferroelétrica. Comparado à cerâmica convencional, o corpo cerâmico sinterizado a laser apresentou condutividade elétrica 3 vezes menor na região de bulk, maior permissividade dielétrica acima de 300 °C, com igual perda dielétrica, mesmo campo coercitivo e polarização remanescente 35 % superior. A caracterização física do BGO foi feita por medidas de absorção óptica, radioluminescência e termoluminescência. Os resultados mostraram que a cerâmica de BGO sinterizada a laser possui grau de transparência 50 % maior, densidade de defeitos estruturais 2 vezes menor, eficiência levemente superior e mesmo dano por radiação, se comparada à cerâmica sinterizada em forno elétrico. Os resultados obtidos foram interpretados com base na escala de tempo característica da sinterização a laser, que afeta a formação e distribuição dos defeitos durante o processo, e resulta em cerâmicas com microestrutura diferenciada. / The goals of this work were the implantation and optimization of the laser sintering technique for ceramic bodies, the kinetic study of the process and the evaluation of the physical properties of the laser sintered compounds Bi4Ti3O12 and Bi4Ge3O12, compared to ceramics sintered in conventional furnace. The choice of the materials was based on their potential applications: Bi4Ge3O12 as scintillator device and Bi4Ti3O12 as an electronic ceramic. Laser sintering showed to be efficient for these materials, producing ceramics with density higher than 98 % and small grain sizes. The combination of pre-heating with a gradual rising of the laser power prevented excessive temperature gradient and heating rate, and reduced considerably the incidence of cracks and pores in the ceramics. The kinetic study of the laser sintering revealed lower activation energies than that observed in the conventional processing, except for BIT ceramics during the final stage of sintering. The results suggest that the laser irradiation anticipates the stages of the sintering process. The physical characterization of BIT was done through impedance spectroscopy and ferroelectric hysteresis measurements. Compared to the conventional sample, this material presented bulk electrical conductivity 3 times smaller, higher dielectric permittivity above 300 °C, comparable dielectric loss, the same coercive field and 35 % higher remanent polarization. The physical characterization of BGO was done through optical absorption, radioluminescence and thermoluminescence measurements. The results showed that the transparency of the laser sintered BGO ceramic was 50 % higher than the transparency of the conventional BGO ceramic, the density of structural defects is 2 times lower, the radiation damage levels are comparable and the overall scintillating efficiency is slightly higher. The obtained results were interpreted on the basis of the time scale of the laser sintering, which affects the formation and distribution of defects during the process, and results in a particular microstructure.

Cette thèse a pour objectif de caractériser un système dosimétrique in vivo implantable pour la radiothérapie externe capable de réaliser, en temps réel, une mesure directe de la dose absorbée dans le volume cible. Ce système, nommé SECURIDOSE, met en œuvre une sonde implantable qui comporte à son extrémité distale un cristal de nitrure de gallium radioluminescent. La transduction par radioluminescence du nitrure de gallium a été étudiée et ses performances intrinsèques ont été comparées avec celles d'autres techniques de transduction mises en œuvre en dosimétrie in vivo. Ce mode de transduction offre un avantage en termes de un rendement de transduction qui est de 100000 photons/MeV. Le GaN a un temps de réponse très court (<1ns). Son émission bande à bande dans le UV est bien adaptée à une mesure en temps réel de la dose. Son spectre d'émission est étroit ce qui facilité la réjection spectrale des luminescences parasites. Le système proposé offre une réponse linéaire avec la dose d'irradiation qui ne dépend pas du débit de dose. Cette réponse reste linéaire même pour des doses d'irradiation très supérieures à celles délivrées au patient. De plus, les sondes SECURIDOSE restent opérationnelles après un cycle de stérilisation Gamma avec une irradiation par une source de 60Co à une dose de 29 kGy. Le GaN n'a pas une dépendance angulaire. Le seul désavantage du système, est la dépendance à l'énergie du faisceau du fait que le GaN n'est pas équivalent tissu. Une variation de 4.5% de la réponse du système a été observée entre deux énergies de faisceaux de photons 6MV et 18MV.

Os objetivos deste trabalho foram a implantação e a otimização da técnica de sinterização a laser de corpos cerâmicos, o estudo da cinética do processo e a avaliação de propriedades físicas dos compostos Bi4Ti3O12 e Bi4Ge3O12 sinterizadas a laser, em comparação com as cerâmicas processadas em forno convencional. A escolha dos materiais baseou-se em seu potencial de aplicação: o Bi4Ge3O12 como dispositivo cintilador e o Bi4Ti3O12 como cerâmica eletrônica. A sinterização a laser mostrou-se eficiente para estes materiais, produzindo cerâmicas com densidade superior a 98 % e pequeno tamanho de grão. A combinação de pré-aquecimento e subida gradual da potência do laser evitou gradientes de temperatura e taxas de aquecimento excessivos, e reduziu consideravelmente a incidência de trincas e a porosidade nas cerâmicas. No estudo cinético da sinterização a laser, registraram-se energias de ativação inferiores às observadas no processamento convencional, exceto para o BIT no estágio final de sinterização, e os resultados sugerem um adiantamento no processo de sinterização, provocado por efeito da irradiação a laser. A caracterização física do BIT foi feita por espectroscopia de impedância e medidas de histerese ferroelétrica. Comparado à cerâmica convencional, o corpo cerâmico sinterizado a laser apresentou condutividade elétrica 3 vezes menor na região de bulk, maior permissividade dielétrica acima de 300 °C, com igual perda dielétrica, mesmo campo coercitivo e polarização remanescente 35 % superior. A caracterização física do BGO foi feita por medidas de absorção óptica, radioluminescência e termoluminescência. Os resultados mostraram que a cerâmica de BGO sinterizada a laser possui grau de transparência 50 % maior, densidade de defeitos estruturais 2 vezes menor, eficiência levemente superior e mesmo dano por radiação, se comparada à cerâmica sinterizada em forno elétrico. Os resultados obtidos foram interpretados com base na escala de tempo característica da sinterização a laser, que afeta a formação e distribuição dos defeitos durante o processo, e resulta em cerâmicas com microestrutura diferenciada. / The goals of this work were the implantation and optimization of the laser sintering technique for ceramic bodies, the kinetic study of the process and the evaluation of the physical properties of the laser sintered compounds Bi4Ti3O12 and Bi4Ge3O12, compared to ceramics sintered in conventional furnace. The choice of the materials was based on their potential applications: Bi4Ge3O12 as scintillator device and Bi4Ti3O12 as an electronic ceramic. Laser sintering showed to be efficient for these materials, producing ceramics with density higher than 98 % and small grain sizes. The combination of pre-heating with a gradual rising of the laser power prevented excessive temperature gradient and heating rate, and reduced considerably the incidence of cracks and pores in the ceramics. The kinetic study of the laser sintering revealed lower activation energies than that observed in the conventional processing, except for BIT ceramics during the final stage of sintering. The results suggest that the laser irradiation anticipates the stages of the sintering process. The physical characterization of BIT was done through impedance spectroscopy and ferroelectric hysteresis measurements. Compared to the conventional sample, this material presented bulk electrical conductivity 3 times smaller, higher dielectric permittivity above 300 °C, comparable dielectric loss, the same coercive field and 35 % higher remanent polarization. The physical characterization of BGO was done through optical absorption, radioluminescence and thermoluminescence measurements. The results showed that the transparency of the laser sintered BGO ceramic was 50 % higher than the transparency of the conventional BGO ceramic, the density of structural defects is 2 times lower, the radiation damage levels are comparable and the overall scintillating efficiency is slightly higher. The obtained results were interpreted on the basis of the time scale of the laser sintering, which affects the formation and distribution of defects during the process, and results in a particular microstructure.