Ever increasing demand for more radiation resistant detectors from experiments such as those at the Large Hadron Collider has pushed the development of novel radiation resistant technologies. Recent developments in the laser processing of diamond have led to the construction of the first 3D diamond detectors: diamond detectors with graphitic electrodes embedded in the sensor material bulk rather than on the surface. This technology also presents interesting properties for the medical field, where 3D diamond detectors are also of interest. This thesis details some of the steps that were carried out between the fabrication of some of the first 3D diamond devices to the present day production and testing of the first 3D pixel devices and the first use of 3D diamond devices in Particle Physics experiments. This progress has in part been pushed by improvements in the laser processing techniques allowing the production of columns with lower resistances and more consistent properties. This thesis describes the fabrication of a number of these devices and details the experiments that these devices have undergone in a number of different conditions at the Diamond Light Source (Oxford), the Ruder Boskovic Institute (Zagreb), the Paul Scherrer Institute (Zurich), and the test beam facilities at CERN. This thesis also describes the simulations that were carried out to replicate the data obtained from some of the earlier devices, and hence understand how charge is collected in 3D diamond detectors and to explain some of the observed behavior of these devices.

<p>Dosimetric characteristics of a CVD single crystal diamond detector have been evaluated. Detector stability, linearity, optimal bias, temperature dependence, directional dependence, priming and pre-irradiation behaviour, depth dose curves and dose profiles were investigated.</p><p>The optimal bias was determined to be 50 V. The detector stability measurement showed a too large variation for absolute dosimetry in a day to day measurement, but acceptable variation during one and the same day. The linearity constant, , in the relation between signal and dose rate, (Fowler 1966), was determined to 0.978 and 0.953 for two detectors. The sub-linearity was also observed in the depth dose curves and could be eliminated with a correction method. The diamond detector showed smaller temperature dependence than the EFD silicon diode. The directional dependency was, <1 %, up to at least ± 15˚ and therefore no angular correction is needed. A priming dose of 0.6 Gy was determined, which is considerably smaller than for existing detectors on the market. After pre-irradiation with electrons (8 and 18 MeV) a large and permanent desensitization of up to 31 % / 500 Gy was detected. This is in contradiction to what previous published articles claim. 15 MV photons also reduced the sensitivity of the detector, but no evidence that 5 MV photons do has been found. A 50 Gy dose of 180 MeV protons did not reduce the sensitivity either. The detector dose rate linearity was improved by electron pre-irradiation. The dose profile penumbras of the diamond detector were, for the most part, smaller than the RK ionization chamber, indicating a better spatial resolution.</p>

Dosimetric characteristics of a CVD single crystal diamond detector have been evaluated. Detector stability, linearity, optimal bias, temperature dependence, directional dependence, priming and pre-irradiation behaviour, depth dose curves and dose profiles were investigated. The optimal bias was determined to be 50 V. The detector stability measurement showed a too large variation for absolute dosimetry in a day to day measurement, but acceptable variation during one and the same day. The linearity constant, , in the relation between signal and dose rate, (Fowler 1966), was determined to 0.978 and 0.953 for two detectors. The sub-linearity was also observed in the depth dose curves and could be eliminated with a correction method. The diamond detector showed smaller temperature dependence than the EFD silicon diode. The directional dependency was, &lt;1 %, up to at least ± 15˚ and therefore no angular correction is needed. A priming dose of 0.6 Gy was determined, which is considerably smaller than for existing detectors on the market. After pre-irradiation with electrons (8 and 18 MeV) a large and permanent desensitization of up to 31 % / 500 Gy was detected. This is in contradiction to what previous published articles claim. 15 MV photons also reduced the sensitivity of the detector, but no evidence that 5 MV photons do has been found. A 50 Gy dose of 180 MeV protons did not reduce the sensitivity either. The detector dose rate linearity was improved by electron pre-irradiation. The dose profile penumbras of the diamond detector were, for the most part, smaller than the RK ionization chamber, indicating a better spatial resolution.

Com o avanço tecnológico dos equipamentos utilizados em radioterapia tornaram-se possíveis o uso de alguns campos de radiação nomeados como campos pequenos em algumas modalidades especiais de radioterapia. Com isso, a dosimetria dos feixes de radiação também teve de ser revista, pois com estes novos tamanhos de campos, não há condição de referência como aquela dita nos protocolos e diretrizes de dosimetria. Neste trabalho foi realizado um estudo completo sobre os campos pequenos, bem como sua dosimetria, mostrando o comportamento dos detectores nessa nova condição de dosimetria através de uma comparação entre os detectores utilizados e dados já publicados na literatura. Além disso, os dados obtidos experimentalmente puderam ser validados através de comparação com dados publicados por outros autores. Na caracterização do detector de diamante o mesmo apresentou-se apropriado em todos os parâmetros para medidas com campos pequenos. Na análise do fator de qualidade Q os resultados experimentais obtidos nesta investigação mostraram diferenças percentuais de 1,8%; 4,0% e 4,9% para câmara do tipo CC01, CC13 e diodo estereotáxico respectivamente. Na avaliação de PDP e TMR foi possível observar a dificuldade nas medições com campos pequenos bem como na comparação de diferentes detectores, para PDP a maior diferença foi de 2,6% e para TMR 2,7%. / With the technological equipment used in radiotherapy became possible use of some radiation fields named small fields in some special forms of radiotherapy. Thus, the dosimetry of radiation fields also had to be revised, as with these new sizes of fields, there is no reference condition such as that expressed in dosimetry protocols and guidelines. This work represents a complete study of small fields and its dosimetry, showing the behavior of the detectors in this new condition of dosimetry through a comparison between the detectors used and data already published. Moreover, the experimental data can be validated by comparison with data published by others authors. In the characterization of the same diamond detector has been considered appropriate in all parameters measured with small fields. The analysis of the beam quality factor (Q) the experimental results obtained in this study showed differences in percentages of 1.8%, 4.0% and 4.9% for chamber-type CC01, CC13 and stereotactic diode respectively. In evaluating PDP and TMR was possible to observe the difficulty in measurements with small fields and the comparison of different detectors, the biggest difference for PDP was 2.6% and 2.7% for TMR.

Com o avanço tecnológico dos equipamentos utilizados em radioterapia tornaram-se possíveis o uso de alguns campos de radiação nomeados como campos pequenos em algumas modalidades especiais de radioterapia. Com isso, a dosimetria dos feixes de radiação também teve de ser revista, pois com estes novos tamanhos de campos, não há condição de referência como aquela dita nos protocolos e diretrizes de dosimetria. Neste trabalho foi realizado um estudo completo sobre os campos pequenos, bem como sua dosimetria, mostrando o comportamento dos detectores nessa nova condição de dosimetria através de uma comparação entre os detectores utilizados e dados já publicados na literatura. Além disso, os dados obtidos experimentalmente puderam ser validados através de comparação com dados publicados por outros autores. Na caracterização do detector de diamante o mesmo apresentou-se apropriado em todos os parâmetros para medidas com campos pequenos. Na análise do fator de qualidade Q os resultados experimentais obtidos nesta investigação mostraram diferenças percentuais de 1,8%; 4,0% e 4,9% para câmara do tipo CC01, CC13 e diodo estereotáxico respectivamente. Na avaliação de PDP e TMR foi possível observar a dificuldade nas medições com campos pequenos bem como na comparação de diferentes detectores, para PDP a maior diferença foi de 2,6% e para TMR 2,7%. / With the technological equipment used in radiotherapy became possible use of some radiation fields named small fields in some special forms of radiotherapy. Thus, the dosimetry of radiation fields also had to be revised, as with these new sizes of fields, there is no reference condition such as that expressed in dosimetry protocols and guidelines. This work represents a complete study of small fields and its dosimetry, showing the behavior of the detectors in this new condition of dosimetry through a comparison between the detectors used and data already published. Moreover, the experimental data can be validated by comparison with data published by others authors. In the characterization of the same diamond detector has been considered appropriate in all parameters measured with small fields. The analysis of the beam quality factor (Q) the experimental results obtained in this study showed differences in percentages of 1.8%, 4.0% and 4.9% for chamber-type CC01, CC13 and stereotactic diode respectively. In evaluating PDP and TMR was possible to observe the difficulty in measurements with small fields and the comparison of different detectors, the biggest difference for PDP was 2.6% and 2.7% for TMR.

<p>Due to its close tissue-equivalence, high radiation sensitivity, dose and dose-rate linearity, diamond is a very promising detector for radiation therapy applications. The present thesis focuses on the development of a chemical vapour deposited (CVD) diamond detector with special attention on the arrangement of the electrodes and encapsulation having minimal influence on the measured signal. Several prototype detectors were designed by using CVD-diamond substrates with attached silver electrodes.</p><p>Interface effects in the electrode-diamond-electrode structure are investigated using the Monte Carlo (MC) code PENELOPE. The studies cover a wide range of electrode and diamond thicknesses, electrode materials and photon beam energies. An appreciable enhancement of the absorbed dose to diamond was found for high-Z electrodes. The influence of the electrodes diminishes with decreasing atomic number difference and layer thickness, so that from this point of view thin graphite electrodes would be ideal. The effect of encapsulation, cable and electrical connections on the detector response is also addressed employing MC techniques. For Co-60, 6 and 18 MV photon beam qualities it is shown that the prototypes exhibit energy and directional dependence of about 3% and 2%, respectively. By modifying the geometry and using graphite electrodes the dependencies are reduced to 1%.</p><p>Although experimental studies disclose some limitations of the prototypes (high leakage current, priming effect and slow signal stabilisation), diamonds of higher quality, suitable for dosimetry, can be produced with better-controlled CVD process. With good crystals and a well-designed encapsulation, the CVD-diamond detector could become competitive for routine dosimetry. It is then important for correct dose determination to use a collision stopping power for diamond incorporating proper mean excitation energy and density-effect corrections. A new mean excitation energy of 88 eV has been calculated.</p>

Due to its close tissue-equivalence, high radiation sensitivity, dose and dose-rate linearity, diamond is a very promising detector for radiation therapy applications. The present thesis focuses on the development of a chemical vapour deposited (CVD) diamond detector with special attention on the arrangement of the electrodes and encapsulation having minimal influence on the measured signal. Several prototype detectors were designed by using CVD-diamond substrates with attached silver electrodes. Interface effects in the electrode-diamond-electrode structure are investigated using the Monte Carlo (MC) code PENELOPE. The studies cover a wide range of electrode and diamond thicknesses, electrode materials and photon beam energies. An appreciable enhancement of the absorbed dose to diamond was found for high-Z electrodes. The influence of the electrodes diminishes with decreasing atomic number difference and layer thickness, so that from this point of view thin graphite electrodes would be ideal. The effect of encapsulation, cable and electrical connections on the detector response is also addressed employing MC techniques. For Co-60, 6 and 18 MV photon beam qualities it is shown that the prototypes exhibit energy and directional dependence of about 3% and 2%, respectively. By modifying the geometry and using graphite electrodes the dependencies are reduced to 1%. Although experimental studies disclose some limitations of the prototypes (high leakage current, priming effect and slow signal stabilisation), diamonds of higher quality, suitable for dosimetry, can be produced with better-controlled CVD process. With good crystals and a well-designed encapsulation, the CVD-diamond detector could become competitive for routine dosimetry. It is then important for correct dose determination to use a collision stopping power for diamond incorporating proper mean excitation energy and density-effect corrections. A new mean excitation energy of 88 eV has been calculated.

Chemical Vapour Deposition (CVD) diamond detectors were modelled for dosimetry of radiotherapy beams. This was achieved by employing the EGSnrc Monte Carlo (MC) method to investigate certain properties of the detector, such as size, shape and electrode materials. Simulations were carried out for a broad 6 MV photon beam, and water phantoms with both uniform and non-uniform voxel dimensions. A number of critical MC parameters were investigated for the development of a model that can simulate very small voxels. For a given number of histories (100 million), combinations of the following parameters were analyzed: cross section data, boundary crossing algorithm and the HOWFARLESS option, with the rest of the transport parameters being kept at default values. The MC model obtained with the optimized parameters was successfully validated against published data for a 1.25 MeV photon beam and CVD diamond detector with silver/carbon/silver structure with thicknesses of 0.07/0.2/0.07 cm for the electrode/detector/electrode, respectively. The interface phenomena were investigated for a 6 MV beam by simulating different electrode materials: aluminium, silver, copper and gold for perpendicular and parallel detector orientation with regards to the beam. The smallest interface phenomena were observed for parallel detector orientation with electrodes made of the lowest atomic number material, which was aluminium. The simulated percentage depth dose and beam profiles were compared with experimental data. The best agreement between simulation and measurement was achieved for the detector in parallel orientation and aluminium electrodes, with differences of approximately 1%. In summary, investigations related to the CVD diamond detector modelling revealed that the EGSnrc MC code is suitable for simulation of small size detectors. The simulation results are in good agreement with experimental data and the model can now be used to assist with the design and construction of prototype diamond detectors for clinical dosimetry. Future work will include investigating the detector response for different energies, small field sizes, different orientations other than perpendicular and parallel to the beam, and the influence of each electrode on the absorbed dose.

Chemical Vapour Deposition (CVD) diamond detectors were modelled for dosimetry of radiotherapy beams. This was achieved by employing the EGSnrc Monte Carlo (MC) method to investigate certain properties of the detector, such as size, shape and electrode materials. Simulations were carried out for a broad 6 MV photon beam, and water phantoms with both uniform and non-uniform voxel dimensions. A number of critical MC parameters were investigated for the development of a model that can simulate very small voxels. For a given number of histories (100 million), combinations of the following parameters were analyzed: cross section data, boundary crossing algorithm and the HOWFARLESS option, with the rest of the transport parameters being kept at default values. The MC model obtained with the optimized parameters was successfully validated against published data for a 1.25 MeV photon beam and CVD diamond detector with silver/carbon/silver structure with thicknesses of 0.07/0.2/0.07 cm for the electrode/detector/electrode, respectively. The interface phenomena were investigated for a 6 MV beam by simulating different electrode materials: aluminium, silver, copper and gold for perpendicular and parallel detector orientation with regards to the beam. The smallest interface phenomena were observed for parallel detector orientation with electrodes made of the lowest atomic number material, which was aluminium. The simulated percentage depth dose and beam profiles were compared with experimental data. The best agreement between simulation and measurement was achieved for the detector in parallel orientation and aluminium electrodes, with differences of approximately 1%. In summary, investigations related to the CVD diamond detector modelling revealed that the EGSnrc MC code is suitable for simulation of small size detectors. The simulation results are in good agreement with experimental data and the model can now be used to assist with the design and construction of prototype diamond detectors for clinical dosimetry. Future work will include investigating the detector response for different energies, small field sizes, different orientations other than perpendicular and parallel to the beam, and the influence of each electrode on the absorbed dose.

L’utilisation de petits champs dans les techniques de radiothérapie a considérablement augmenté, en particulier dans les traitements stéréotaxiques et les grands champs uniformes ou non uniformes qui sont composés de petits champs tels que la radiothérapie à modulation d’intensité (IMRT) ou la radiothérapie par microfaisceaux. Pour ces champs d’irradiation, les erreurs dosimétriques ont augmenté par rapport aux faisceaux conventionnels. La raison principale en est qu’il n’existe pas de protocole dosimétrique standard. Dans le cas de la MRT, un protocole dédié a été développé sur la base d’une mesure de faisceau large avec une chambre d’ionisation PinPoint combinée à la multiplication avec un OF pour prédire la dose dans le pic. Ce protocole est pratique en ce sens qu’il permet de surmonter le manque de résolution spatiale du détecteur et de toute façon d’aller de l’avant avec les procédures pré-cliniques en permettant le calcul de la dose pic. La dose dans la vallée est ensuite récupérée à l’aide du PVDR, également basé sur des calculs MC.Au cours de la dernière décennie, des détecteurs à haute résolution spatiale permettant des mesures à l’échelle du micron sont devenus disponibles. Parmi eux, le détecteur de microdiamants PTW, les films HDV2 combinés avec le système de lecture approprié et le FNTD. Les mesures effectuées sur la ligne de lumière biomédical ID 17 avec ces trois dosimètres ont mis en évidence des divergences entre les valeurs simulées MC de OF et PVDR et les données expérimentales qui traitent d’un problème concernant la validité du protocole de dosimétrie actuel. En outre, il a été souligné que les valeurs OF et PVDR différent entre les différents codes MC, ce qui représente un problème lorsque ces valeurs sont associé au protocole de dosimétrie. Obtenir des valeurs fiables d’OF et de PVDR pour les mesures expérimentales et numériques représente le défi de ce travail.Dans ce travail, les écarts entre les simulations MC et les données mesurées sont attribués à un manque de détails dans les simulations MC et au fait que les caractéristiques spécifiques du détecteur peuvent influencer la mesure. Une série de simulations MC est mise au point pour quantifier chacun de ces effets. Le principal inconvénient d'une telle étude est le temps de simulation, de sorte que des astuces sont utilisées pour accélérer le calcul et néanmoins garder les résultats aussi précis que possible. / The use of small fields in radiotherapy techniques has increased substantially, in particular in stereotactic treatments and large uniform or nonuniform fields that are composed of small fields such as for intensity modulated radiation therapy (IMRT) or Microbeam Radiation Therapy. For these irradiation fields, dosimetric errors have increased compared to conventional beams. The main reason for this is that no standard dosimetric protocol exists. In the case of MRT, a dedicated protocol has been developed based on a broad beam measurement with a PinPoint chamber combined with the multiplication with an OF to predict the peak dose. This protocol is handy in the sense that it allows to overcome the lack of spatial resolution of the detector and anyway move forward with pre-clinical procedures by enabling the calculation of the peak dose. The valley dose is then retrieved using the PVDR also based on MC calculations.Over the last decade, detectors with high spatial resolution allowing measurements at the micron scale became available. Among them, the PTW microDiamond detector, HDV2 films combined with the appropriate read-out system and FNTD. Measurements performed at the ID 17 biomedical beamline with these three dosimeters highlighted discrepancies between the MC simulated values of OF and PVDR and experimental data which addresses an issue regarding the validity of the current dosimetry protocol. Moreover, it has been highlighted that OF and PVDR values differ between the different MC codes which represents a problem when associated with the dosimetry protocol. Obtaining reliable values of OF and PVDR for both experimental and numerical measurement represents the challenge of this work.In this work, the discrepancies between the MC simulations and measured datas are assigned to a lack of details in the MC simulations and to the fact that detector specific characteristics can influence the measurement. A series of MC simulation is developed to quantify each of these effects. The major drawback of such study is the simulation time, so tricks are used to speed up the calculation and nevertheless keep the results as accurate as possible.