Made available in DSpace on 2014-10-09T12:33:19Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:06:27Z (GMT). No. of bitstreams: 0 / Tese (Doutoramento) / IPEN/T / Instituto de Pesquisas Energeticas e Nucleares - IPEN-CNEN/SP

Made available in DSpace on 2014-10-09T12:33:19Z (GMT). No. of bitstreams: 0 / Made available in DSpace on 2014-10-09T14:06:27Z (GMT). No. of bitstreams: 0 / Neste trabalho apresentamos um estudo das reações nucleares de alta energia que são fundamentais na definição do termo fonte dos reatores nucleares subcríticos acionados por fonte externa. Estas reações nucleares, também conhecidas como \"spallation\", consistem na interação de hádrons de alta energia com os núcleons do núcleo atômico. A fenomenologia destas reações consiste em duas etapas, sendo que à primeira, o próton interage através de espalhamentos múltiplos, em um processo denominado cascata intra-nuclear seguido da etapa na qual o núcleo excitado oriundo da cascata intranuclear ou evapora partículas de forma a atingir estados energéticos moderados ou fissiona, em um processo conhecido como competição entre evaporação e fissão. Neste trabalho os principais modelos nucleares, os modelos de Bertini e Cugnon, são revistos, pois estes modelos são fundamentais para propósito de projeto devido à falta de dados nucleares avaliados para estas reações. A implementação e validação dos métodos de cálculo para o projeto destas fontes são realizadas. A implementação da metodologia é realizada utilizando o programa MCNPX ( \"Monte Carlo N-Particle eXtended\"), dedicado para cálculos de transporte destas partículas e a validação é realizada mediante uma cooperação internacional junto a um projeto coordenado de pesquisa da Agencia Internacional de Energia Atômica e trabalhos disponíveis. O objetivo é qualificar os cálculos relacionados às reações nucleares e os canais de desexcitação envolvidos. O CRISP, um código nacional para a descrição da fenomenologia das reações envolvidas, também foi estudado e os modelos implementados no código foram revistos e melhorados de forma a dar continuidade ao seu processo de qualificação. Devido às limitações dos principais modelos na descrição de produção de nuclídeos leves, a reação de multi-fragmentação foi estudada. As discrepâncias nos cálculos de produção destes nuclídeos são atribuídas à falta do canal de multi-fragmentação estatística do núcleo. A implementação deste canal foi realizada para a aplicação em reações de altas energias junto ao código CRISP de forma a reproduzir a produção de nuclídeos leves, bem como sua validação mediante a comparação com dados experimentais disponíveis para este fenômeno, obtendo com isso uma melhor reprodução de todo o espectro de produção de nuclídeos do processo. / Tese (Doutoramento) / IPEN/T / Instituto de Pesquisas Energeticas e Nucleares - IPEN-CNEN/SP

Apesar do grande volume de pesquisas e dos avanços da produção in vitro (PIV) de embriões bovinos, a eficiência da técnica ainda está distante do desejável, principalmente quando comparada a embriões produzidos in vivo. A maturação in vitro é etapa importante da PIV, visto que a qualidade dos embriões é dependente da qualidade do oócito e, assim, modificações nas condições de maturação in vitro podem trazer avanços à produção de embriões. A melatonina é um hormônio que foi detectado no fluido folicular de humanos, suínos e, mais recentemente, de bovinos. Ainda, seus receptores foram localizados em oócitos e células da granulosa. Estudos in vitro apontam efeitos benéficos de sua utilização na maturação e cultivo in vitro de oócitos e embriões, embora os resultados sejam por vezes contraditórios. O presente trabalho teve por objetivo avaliar o efeito da melatonina na maturação in vitro (MIV) de oócitos bovinos e também seu potencial como indutor de genes de enzimas antioxidantes e inibidor de fragmentação nuclear em células do cumulus. Para tanto, complexos cumulus-oócitos (CCOs), obtidos de ovários de abatedouro, foram maturados in vitro na presença de melatonina (10-9 e 10-6 M), FSH (controle positivo) ou sem hormônios (controle negativo). As taxas de maturação nuclear foram avaliadas às 6, 12, 18 e 24 horas de cultivo (Experimento 1). No Experimento 2, os mesmos grupos experimentais foram avaliados quanto à abundância relativa de transcritos de genes de enzimas antioxidantes (Cu,ZnSOD, MnSOD e GPx) em oócitos e células do cumulus (24 horas de MIV) por PCR em tempo real. No Experimento 3 foi avaliado o efeito dos tratamentos sobre a fragmentação nuclear em células do cumulus pela técnica de TUNEL e citometria de fluxo (24 horas de MIV). A taxa de maturação avaliada às 6 h de MIV foi de 100% de oócitos imaturos em vesícula germinativa (VG) (P>0,05). Às 12 horas de cultivo foi observado o efeito da melatonina similar ao FSH, variando a proporção de oócitos em metáfase I (MI) de 54,0 a 80,7 % entre os grupos (P<0,05). Após 18 h de MIV observou-se que a maioria dos oócitos já havia atingindo o estádio de metáfase II (MII) variando de 57,2 a 74,2 % (P>0,05). Após 24 h de MIV, observou-se que a maioria dos oócitos atingiu o estádio de MII (50,7 a 89,5%), sendo que a melatonina na maior concentração apresentou efeito similar ao da gonadotrofina (P<0,05). Em relação à expressão de enzimas antioxidantes em oócitos não houve efeito de nenhum tratamento (P>0,05%). Já em células do cumulus houve maior expressão do MnSOD no grupo com FSH em relação ao grupo maturado sem hormônios ou imaturo (P<0,05). A melatonina nas diferentes concentrações apresentou efeito similar ao da gonadotrofina (P>0,05). Transcritos para a enzima Cu,ZnSOD foram mais abundantes em cumulus de CCOs maturados com a maior concentração de melatonina (10-6 M) em relação ao grupo imaturo (P<0,05), não havendo variação nos demais (P>0,05). GPX4 não foi afetado pelos tratamentos (P>0,05). A quantidade de células do cumulus com fragmentação nuclear não foi afetada por nenhum tratamento (33,4 a 41,5/10.000 células; P>0,05) Com base nestes resultados conclui-se que a melatonina nas concentrações avaliadas (10-9 e 10-6 M), embora seja capaz de estimular a maturação nuclear e induzir a expressão de alguns genes antioxidantes em células do bovinas, ainda que de forma semelhante ao FSH, não provocou redução da fragmentação nuclear nestas células. / Nevertheless the great volume of research and the advances in in vitro production (IVP) of bovine embryos, the efficiency of this techinque is still beyond the desireable, specially when compared to embryos produced in vivo. in vitro maturation (IVM) is an important step in IVP, since the quality of embryos is dependent on the quality of oocytes, and, therefore, modifications to in vitro maturation conditions can bring improvements to embryo production. Melatonin is a hormone which has been detected in the folicular fluid of humans, pigs, and more recently, in bovine. Also, its receptores have been identified in oocytes and granulosa cells. Studies in vitro have shown that melatonin may have beneficial effects when used in oocyte maturation and embryo culture, although results are sometimes contradictory. The aim of the present work was to assess the effect of melatonin during IVM on nuclear maturation of bovine oocytes as well as its potential to induce expression of antioxidant enzymes and to reduce nuclear fragmentation in cumulus cells. Cumulus-oocyte comprexes (COCs), obtained from abbattoir ovaries, were matured in vitro in the presence of melatonin (10-9 e 10-6 M), FSH (positive controle) or without hormones (negative control). Maturation rates were evaluated at 6, 12, 18 and 24 h (Experiment 1). In Experiment 2, the same groups were evaluated for the relative abundance of transcripts encoding antioxidant enzymes (Cu,ZnSOD, MnSOD and GPx) in oocytes and cumulus cells (24 h IVM) by real time PCR. In Experiment 3, the effect of treatments on nuclear fragmentation in cumulus cells was determined by TUNEL and flow cytometry (24 h IVM). At 6 h IVM, all oocytes were at immature germinal vesicle (GV) stage. After 12 h of cuture the effect of melatonin was similar to that of FSH, with proportions of oocytes in metaphase I (MI) varying from 54.0 to 80.7% between groups (P>0.05). After 18 h IVM most oocytes had reached metaphase II (MII) stage (57.2 to 74.2%, P>0.05). At 24 h IVM, oocytes were also mostly in MII stage (50.7 to 89.5%), and the highest melatonin concentration was similar to the gonadotrophin (P>0.05). Regarding expression of antioxidant enzymes in oocytes there was no effect of treatments for any of the genes (P>0.05). However, in cumulus cells MnSOD expression was higher in FSH compared with the groups matured without hormones or immature cells (P<0.05). Melatonin in both concentrations were similar to FSH (P>0.05). Transcripts for Cu,ZnSOD were more abundant in cumulus from COCs matured with the highest melatonin concentration (10-6 M) in relation to immature cells (P<0.05), but was not diferent from other groups (P>0.05). GPx was not affected by treatments (P>0.05). The number of nuclear fragmentation in cumulus cells was also not affected by treatments (33.4 to 41.5/10,000 cells; P>0.05). According to these results it is concluded that melatonin is able to induce meiosis resumption in oocytes (10-9 and 10-6 M) and expression of some antioxidant genes in bovine cumulus cells, similar to the effect of FSH, but was ineffective in reducing nuclear fragmentation in these cells.

Lors du traitement d'une tumeur par radiothérapie utilisant des ions comme le 12C, le faisceau peut subir des réactions nucléaires avec les noyaux des tissus menant à la création de particules secondaires plus légères. Cela a pour conséquences de délocaliser une partie de la dose dans les tissus sains et de créer un champ d'irradiation mixte. Afin d'améliorer les connaissances sur la fragmentation du projectile, une expérience a été réalisée par notre collaboration en Mars 2015 au GANIL avec un faisceau de 12C à 50 MeV/n. Cette expérience a permis de mesurer les sections efficaces doublement différentielles en angle et en énergie pour tous les isotopes créés, et ce, sur différentes cibles d'intérêt médical (C, H, O et Ca). Les distributions angulaires et les taux de production ont également été obtenus pour chaque fragment et pour chaque cible. Les résultats ont ensuite été comparés à différents modèles de réactions nucléaire disponibles dans les outils de simulation Monte Carlo GEANT4 et PHITS. Des écarts importants ont été observés avec les résultats expérimentaux, mais aussi entre les différents modèles. Ces conclusions avaient déjà poussé notre collaboration à créer un nouveau modèle, appelé SLIIPIE, spécialisé dans les réactions d'ions légers aux énergies intermédiaires. Les paramètres de ce modèle ont ainsi été ajustés de façon à reproduire au mieux les données expérimentales obtenues. / During the treatment of cancerous diseases using ions such as 12C, the beam will undergo nuclear reactions with the tissues leading to the production of lighter secondary fragments. This tends to delocate a part of the dose into healthy tissues and create a mixed radiation field. In order to improve the knowledge on the projectile fragmentation, an experiment was performed by our collaboration in March 2015 with a 50 MeV/n 12C beam at GANIL. This led to the measurement of double differential cross sections in angle and energy of every isotope created by the fragmentation of carbon on targets of medical interest (C, H, O and Ca). Energy and angular distributions, as well as production rates have also been obtained for every fragment and every target. Experimental data were then compared with nuclear reaction models included in the Monte-Carlo (MC) simulation codes, GEANT4 and PHITS. Important discrepancies were observed with our data, as well as between models. These observations had already led our collaboration in creating a new MC model called SLIIPIE, specialized in intermediate energies reactions with light ions. The parameters of this model were then adjusted in order to best fit the experimental data.

Today, the application of particle beams in cancer therapy is a well-established strategy and its combination with surgery and chemotherapy is becoming an increasingly reliable approach for some several clinical cases (e.g. skull base tumors). Currently, protons and 12C ions are used for patients’ treatment, due to their characteristic depth-dose deposition profile featuring a pronounced peak (the Bragg Peak) at the end of range. Clinical energies typically span between 60 and 250 MeV for protons and up to 400 MeV/u for 12C ions, in order to deliver treatments to various disease sites. Interactions between the primary beam and the patient’s body always occur during treatment, changing the primary radiation composition, energy and direction and thus affecting its depth dose and lateral profile. In carbon therapy, both projectile and target fragments can be generated during a treatment: the former are characterized by a kinetic energy spectrum peaked at the same energy of the primary beam and are mostly emitted in the forward direction; the latter are emitted with a much lower energy because they are produced from the target, which is at rest before the collision, and they are generated isotropically in the target frame. Moreover, the interaction of carbon ions with the patient's body is currently modeled in the treatment planning on the basis of experimental data measured in water. For all other biological materials, the contribution of nuclear interactions is taken into account by rescaling the values measured in water with a density factor. This approximation neglects the influence of the elemental composition, which might become relevant in cases where the material encountered by the beam significantly differs from water (e.g. bone or lung tissues) and result in a non-uniform and incorrect dose profile. Thus, experimental data with target different from water are clearly needed in order to correctly evaluate the contribution of all biological elements inside the human body. Treatments with protons can only generate target fragments, leading to the production of low-energy and therefore short-range fragments. Heavy secondary fragments will have a higher biological effectiveness than to protons, thus affecting the proton Relative Biological Effectiveness (RBE, i.e. the ratio of photon to charged particles dose necessary to achieve the same biological effect), nowadays assumed as a constant value (RBE=1.1) in clinical practice. Another aspect related to nuclear interactions is the overlap between radiotherapy and space radiation protection. The group of particle species either currently available in radiotherapy or considered promising alternative candidates (i.e. Helium, Lithium and Oxygen) are among the most abundant in the space radiation environment. Moreover, the proton energy range used in radiotherapy is similar to that of Solar Particle Events (SPEs) and Van Allen trapped protons. The radiation environment in space can lead to serious health risks for astronauts, especially in long duration and far from Earth space missions (like human explorations to Mars). Protection against space radiation are of paramount importance for preserving the astronauts’ life. Today, the only possible countermeasure is passive shielding. Nuclear fragmentation processes can occur inside the spaceship hull, causing the production of lighter and highly penetrating radiation that must be considered when a shielding is designed. Therefore, experimental data for beam and targets combinations relevant in space radiation applications must be collected for characterizing the interaction of mixed generated radiation field and assess the radiation-induced health risk. Despite the many fundamental open issues in particle therapy and space radiation protection fields, such the ones mentioned above, the current lack of experimental fragmentation cross section data in their energy range of interest is undeniable. Thus, accurate measurements for different ions species with energies up to 1000 MeV/u would be of great importance in order to further optimize particles treatments and improve the shielding design of spaceship. Moreover, additional experimental data would be of great importance for benchmarking Monte Carlo codes, which are extensively used by the scientific communities in both research fields. In fact, the available transport codes suffer from many uncertainties and they need to be verified with reliable experimental data. Due to high energy and long range of projectile fragments, the standard approach for their identification is collect data from several detector types, usually two plastic scintillators coupled with a Barium Fluoride or LYSO crystal, placed both upstream or downstream the target, providing information about the charge, energy loss, the residual kinetic energy and the time of flight of the emitted fragments. This experimental setup allows the identification of particle species in terms of charge, isotope, emission angle and kinetic energy and it has been widely exploited to perform several fragmentation measurements, both in particle therapy and space application fields. An example is the ROSSINI (RadiatiOn Shielding by ISRU and/or INnovative materIals for EVA, Vehicle and Habitat) project financed by the European Space Agency (ESA) to select innovative shielding materials and provide recommendations on space radioprotection for different mission scenarios. However, such standard approach is not useful for the characterization of target fragments. In fact, because of their low energy and short range, a much more complex setup and finer experimental strategies are required for their detection. The FOOT (FragmentatiOn Of Target) experiment has been designed to measure fragment production cross sections with ~5% uncertainty. Target fragmentation induced by 50-250 MeV proton beams will be studied taking advantage of an inverse kinematic approach. Specifically, O, C and He beams impinging on different targets (e.g., C, C2H4) will be employed, thus boosting the fragments energy and making their detection possible. Fragmentation cross section of hydrogen will be then obtained by subtraction. The same configuration provides also a measurement of projectile fragments with the direct kinematics approach. FOOT experimental setup consists of two different apparatus: a dedicated “table-top” electronic setup, based on a magnetic spectrometer, were conceived for the detection of heavier fragments (Z≥3). Alternatively, an emulsion spectrometer was designed in order to measure the production of low Z fragments (Z≤3) that would not cross the whole magnetic spectrometer. The purpose of the work presented in this doctoral thesis is the experimental characterization of particles originated in nuclear fragmentation processes for targets and beams of interest for particle therapy and space radiation protection, providing inputs to improve the accuracy of Monte Carlo transport codes presently used. Data collected in experimental campaigns using the standard setup to study the interaction of 400 MeV/u 12C ions beam with bone-like materials and 1000 MeV/u 58Ni ions beam with targets relevant for space applications have been analyzed. The presented fragments characterization comprehends the fraction of primary particles surviving the target and the yield and kinetic energy spectra of charged particles emitted at several angles with respect to the primary beam direction. The )*Ni beam data were collected in the frame of the ROSSINI experiment and focused on characterizing secondary neutrons production. Moreover, the analysis of the performances and fragments reconstruction capabilities of the FOOT electronic setup has been accomplished with Monte Carlo simulations. A dedicated analysis software has been developed in order to reconstruct fragments charge and mass, energy yields and production cross sections. A preliminary analysis of experimental data collected by a partial FOOT electronic setup is presented as well.

La toxine stable à la chaleur de type b (STb) est une des toxines produites par les souches Enterotoxigenic Escherichia coli (ETEC) impliquée dans le développement de la diarrhée. Une étude antérieure par Goncalves et al. (2009) a démontré que les cellules ayant internalisé la toxine STb démontraient une morphologie qui rappelle l’apoptose. Le changement du potentiel membranaire observé par Goncalves et al. (2009) nous a incité à vérifier la capacité de la toxine STb à induire l’apoptose des cellules HRT-18 et IEC-18 par la voie intrinsèque. Les cellules HRT-18 et IEC-18 ont été traitées avec de la toxine purifiée pour une durée de 24 heures puis ells ont été récoltées et examinées pour des caratéristiques de l’apoptose. L’activation des caspases-9 et -3, mais pas de la caspase-8, a été observée dans les deux lignées cellulaires à l’aide des substrats fluorescents spécifiques pour chaque caspase. L’ADN extrait des cellules HRT-18 et IEC-18 a révélé une fragmentation lorsque migré sur gel d’agarose. La condensation et la fragmentation des noyaux ont été observées en microscopie à fluorescence suite à une coloration de l’ADN au Hoechst 33342. Les indices apoptotiques des cellules HRT-18 et IEC-18 traitées avec des quantités croissantes de STb montrent une dose-réponse pour les deux lignées. L’activation de la caspase-9 est une indication que la voie intrinsèque de l’apoptose est activée dans les cellules HRT-18 et IEC-18. L’absence de l’activation de la caspase-8 démontre que la voie extrinsèque n’est pas impliquée dans la mort cellulaire médiée par STb. / Heat-stable toxin b (STb) is one of the toxins produced by Enterotoxigenic Escherichia coli (ETEC) strains implicated in the development of diarrhea. A previous study conducted by Goncalves et al. (2009) showed that cells having internalized STb toxin demonstrated apoptotic-like morphology. The change in the mitochondrial membrane potential observed by Goncalves et al. (2009) prompted us to verify the ability of STb toxin to induce apoptosis via the intrinsic pathway in HRT-18 and IEC-18 cells. Both cell lines were treated with purified STb toxin for a period of 24 hours, harvested, and examined for apoptotic features. Activation of caspases-9 and -3, but not -8, was observed in HRT-18 and IEC-18 cells as determined with the use of fluorescent substrates specific to each caspase. Extracted DNA revealed DNA laddering when migrated on agarose gels. Nuclear condensation and fragmentation of Hoechst 33342 stained DNA of HRT-18 and IEC-18 cells were visualized by fluorescence microscopy. Apoptotic indexes of HRT-18 and IEC-18 cells treated with increasing amounts of STb toxin revealed dose-dependent responses in both cell lines. The activation of caspase-9 is an indication of the intrinsic pathway being activated in HRT-18 and IEC-18 cells by STb toxin. The lack of caspase-8 activation demonstrates that the extrinsic pathway of apoptosis is not involved in the programmed cell death mediated by STb.

Foi investigada a correlação entre a energia transversa (ET) produzida e a energia de partículas neutras (En) emitidas em colisões de íons de 28Si (plab=14.6 GeV/c por nucleon) com alvos de Al, Cu e Pb, estudadas pelo Experimento 814 no acelerador AGS do Laboratório Nacional de Brookhaven. A correlação entre a energia transversa e a energia dianteira produzida em colisões com emissão dos fragmentos 2H, 3H, 3He, 4He, 6He, 5Li e 6Li também foi investigada. Foi observado que a energia En dianteira produzida pelas partículas neutras tem uma forte dependência com a energia transversa ET produzida na colisão. Uma parametrização eficiente dos dados é obtida utilizando um modelo estatístico que relaciona o numero de espectadores da colisão com o numero de nêutrons detectados na região dianteira. As distribuições de momento desses fragmentos foram investigadas através do modelo de Goldhaber e os seus respectivos parâmetros 0 foram calculados para os eventos referentes as colisões de 28Si com alvos de Al, Cu e Pb. / We carried out a study of the forward neutral energy (En) and its correlation with the produced transverse energy (ET ) in collisions of 28Si ions (plab=14.6 GeV/c per nucleon) with Al, Cu, and Pb targets, investigated by Experiment 814 at the Brookhaven AGS. The correlation of the produced transverse energy with forward neutral energy from fragments 2H, 3H, 3He, 4He, 6He, 5Li and 6Li was also investigated. We find that the forward neutral energy En has a strong dependence on transverse energy ET produced in the collision. An efficient parametrization of this data set is accomplished through the use of a statistical model which relates the number of spectators in the collision to the number of neutrons detected in the forward direction. Momentum distributions of the fragments were investigated through the use of the Goldhaber model and the 0 parameter was calculated to each of the fragments in reactions of 28Si with Al, Cu and Pb targets.

La toxine stable à la chaleur de type b (STb) est une des toxines produites par les souches Enterotoxigenic Escherichia coli (ETEC) impliquée dans le développement de la diarrhée. Une étude antérieure par Goncalves et al. (2009) a démontré que les cellules ayant internalisé la toxine STb démontraient une morphologie qui rappelle l’apoptose. Le changement du potentiel membranaire observé par Goncalves et al. (2009) nous a incité à vérifier la capacité de la toxine STb à induire l’apoptose des cellules HRT-18 et IEC-18 par la voie intrinsèque. Les cellules HRT-18 et IEC-18 ont été traitées avec de la toxine purifiée pour une durée de 24 heures puis ells ont été récoltées et examinées pour des caratéristiques de l’apoptose. L’activation des caspases-9 et -3, mais pas de la caspase-8, a été observée dans les deux lignées cellulaires à l’aide des substrats fluorescents spécifiques pour chaque caspase. L’ADN extrait des cellules HRT-18 et IEC-18 a révélé une fragmentation lorsque migré sur gel d’agarose. La condensation et la fragmentation des noyaux ont été observées en microscopie à fluorescence suite à une coloration de l’ADN au Hoechst 33342. Les indices apoptotiques des cellules HRT-18 et IEC-18 traitées avec des quantités croissantes de STb montrent une dose-réponse pour les deux lignées. L’activation de la caspase-9 est une indication que la voie intrinsèque de l’apoptose est activée dans les cellules HRT-18 et IEC-18. L’absence de l’activation de la caspase-8 démontre que la voie extrinsèque n’est pas impliquée dans la mort cellulaire médiée par STb. / Heat-stable toxin b (STb) is one of the toxins produced by Enterotoxigenic Escherichia coli (ETEC) strains implicated in the development of diarrhea. A previous study conducted by Goncalves et al. (2009) showed that cells having internalized STb toxin demonstrated apoptotic-like morphology. The change in the mitochondrial membrane potential observed by Goncalves et al. (2009) prompted us to verify the ability of STb toxin to induce apoptosis via the intrinsic pathway in HRT-18 and IEC-18 cells. Both cell lines were treated with purified STb toxin for a period of 24 hours, harvested, and examined for apoptotic features. Activation of caspases-9 and -3, but not -8, was observed in HRT-18 and IEC-18 cells as determined with the use of fluorescent substrates specific to each caspase. Extracted DNA revealed DNA laddering when migrated on agarose gels. Nuclear condensation and fragmentation of Hoechst 33342 stained DNA of HRT-18 and IEC-18 cells were visualized by fluorescence microscopy. Apoptotic indexes of HRT-18 and IEC-18 cells treated with increasing amounts of STb toxin revealed dose-dependent responses in both cell lines. The activation of caspase-9 is an indication of the intrinsic pathway being activated in HRT-18 and IEC-18 cells by STb toxin. The lack of caspase-8 activation demonstrates that the extrinsic pathway of apoptosis is not involved in the programmed cell death mediated by STb.

Foi investigada a correlação entre a energia transversa (ET) produzida e a energia de partículas neutras (En) emitidas em colisões de íons de 28Si (plab=14.6 GeV/c por nucleon) com alvos de Al, Cu e Pb, estudadas pelo Experimento 814 no acelerador AGS do Laboratório Nacional de Brookhaven. A correlação entre a energia transversa e a energia dianteira produzida em colisões com emissão dos fragmentos 2H, 3H, 3He, 4He, 6He, 5Li e 6Li também foi investigada. Foi observado que a energia En dianteira produzida pelas partículas neutras tem uma forte dependência com a energia transversa ET produzida na colisão. Uma parametrização eficiente dos dados é obtida utilizando um modelo estatístico que relaciona o numero de espectadores da colisão com o numero de nêutrons detectados na região dianteira. As distribuições de momento desses fragmentos foram investigadas através do modelo de Goldhaber e os seus respectivos parâmetros 0 foram calculados para os eventos referentes as colisões de 28Si com alvos de Al, Cu e Pb. / We carried out a study of the forward neutral energy (En) and its correlation with the produced transverse energy (ET ) in collisions of 28Si ions (plab=14.6 GeV/c per nucleon) with Al, Cu, and Pb targets, investigated by Experiment 814 at the Brookhaven AGS. The correlation of the produced transverse energy with forward neutral energy from fragments 2H, 3H, 3He, 4He, 6He, 5Li and 6Li was also investigated. We find that the forward neutral energy En has a strong dependence on transverse energy ET produced in the collision. An efficient parametrization of this data set is accomplished through the use of a statistical model which relates the number of spectators in the collision to the number of neutrons detected in the forward direction. Momentum distributions of the fragments were investigated through the use of the Goldhaber model and the 0 parameter was calculated to each of the fragments in reactions of 28Si with Al, Cu and Pb targets.

The 12C+16O breakup of 28Si and the 12C+12C breakup of 24Mg have been studied following the interaction of a 170 MeV 24Mg beam with 7Li, 9Be,12C and 16O target nuclei. The measurements were performed at the Australian National University in Canberra, using the technique of Resonant Particle Spectroscopy. The breakup fragments from the decay of the resonant nuclei were detected in two Gas-Si-CsI telescopes positioned on opposite sides of the beam axis. The data suggest that the same states in 28Si are populated via the 7Li(24Mg, 12C 16O)3H, 9Be(24Mg,12C 16O)5He and 12c(24Mg,12C 16O)8Be reactions. This implies that the cluster decaying states are populated by direct a-transfer. Breakup has been observed from states in 28Si at excitation energies (spins) of (26.15), 28.17 (13-, 29.51, 29.95, 30.45, 30.76, (31.3), 31.65, 31.90, 32.51, 33.14, 33.41, 33.77, 34.45 (12+,14+) and 35.13 MeV. A consistent theoretical interpretation of the 28Si molecular structures has been given, taking into account the predictions of Nilsson-Strutinsky, a-cluster model and two centre shell model calculations. The present results for the 12C(24Mg,12C 12C)12C reaction agree with previous measurements. In addition, new spin assignments have been proposed for several of the breakup states in 24Mg. States have been observed at excitation energies (spins) of 20.54 (2+), 21.07 (4+), 21.88 (4+), 22.33 (4+), 22.90 (6+), 23.80 (6+,(8+)), 24.56 (8+), 25.14 (6+), 25.72, 26.41 (8+) and 27.12 MeV. Evidence for the population of many of these states via the 16O(24Mg,12C 12C)16O reaction has also been observed. However, the data gave no evidence for either the 7Li(24Mg,12C 12C)7Li or 9Be(24Mg,12C 12C)9Be reactions. The presently available information did not allow an unambiguous determination of the reaction mechanism responsible for the population of the 24Mg breakup states. The performance of the Gas-Si-Csl telescopes has been investigated. For multiplicity 2 events in the silicon strip detectors, a crosstalk has been observed between the two active strips. The energy calibration of the silicon strip detectors for penetrating particles has also been found to differ to that for stopped particles. Empirical corrections for both of these effects have been deduced allowing the simultaneous detection and identification of heavy and light ions within a single telescope. These techniques have been extended to the detection of 8Be → alpha+alpha events over a wide range of alpha-particle energies.