Orientador: Fernando Iikawa / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin. / Made available in DSpace on 2018-08-12T12:58:46Z (GMT). No. of bitstreams: 1 Gomes_PauloFreitas_D.pdf: 14344200 bytes, checksum: 55a7f7d3b644c0dc43151a411d53757b (MD5) Previous issue date: 2009 / Resumo: No presente trabalho apresentamos um estudo da luminescência de érbio em nanocristais de silício (nc-Si) e nanofios de óxido de zinco (nw-ZnO). Os nanocristais de silício com érbio são obtidos através do tratamento térmico de filmes finos amorfos de sub-óxidos de silício (SiOx) preparados por rf-sputtering, variando a concentração de Oxigênio e érbio durante o crescimento. O érbio é adicionado aos filmes cobrindo parcialmente a superfície do alvo de silício com pequenos cacos de érbio metálico. Medidas de espectroscopia Raman e microscopia eletrônica de alta resolução (HRTEM) fornecem o tamanho e densidade de nanocristais em cada amostra. Medidas de fotoluminescência (PL) dos nanocristais na temperatura ambiente mostram que o tamanho dos nanocristais varia com a concentração de oxigênio e temperatura de tratamento térmico. A dependência da PL dos nanocristais com a temperatura pode ser entendida considerando a competição entre processos radiativos e não-radiativos. Em amostras com érbio a taxa de recombinação não-radiativa é maior que nas amostras sem érbio. O estudo da PL dos nanocristais e dos íons Er3+ mostra que o Er3+ funciona como um centro de recombinação não-radiativa para a energia proveniente da recombinação de portadores nos nanocristais. Neste caso, parte da energia gerada nos nanocristais é transferida para os íons Er3+ ao invés de ser emitida na forma de fótons. Também é possível observar que a intensidade da PL do Er3+ depende da intensidade da PL dos nanocristais e é maior em amostras contendo nanocristais de ~3nm (que emitem em ~1,5eV), indicando que a transferência é ressonante (com a excitação 4I15/2 ---> 4I9/2 do Er3+ que corresponde a uma energia de 1,5eV). Os nanofios de ZnO com érbio são preparados por deposição vapor-liquid-solid (VLS) e por electrospinning. Em amostras preparadas por VLS, o érbio é depositado sobre os nanofios após sua preparação. No electrospinning um composto organometálico de érbio é adicionado ao polímero precursor. É observada luminescência de érbio quando as amostras são excitadas com um comprimento de onda ressonante com algum nível mais energético do Er3+. Nanocristais de E2O3 são observados por HRTEM na superfície dos nanofios preparados por VLS. Medidas de EXAFS revelam que a vizinhança do Er nessas amostras é idêntica à do óxido Er2O3, indicando que não ocorreu dopagem substitucional do ZnO. / Abstract: We present a study of erbium luminescence in silicon nanocrystals (nc-Si) and zinc oxide nanowires (nw-ZnO). Silicon nanocrystals are produced by annealing of amorphous sub-oxide thin films (SiOx) prepared by rf-sputtering varying the oxygen and erbium concentration during growth. Erbium is added by partially covering the silicon target surface with small pieces of metallic erbium. Raman spectroscopy and HRTEM measurements reveal the size and density of nanocrystals in each sample. Photoluminescence (PL) measurements at room temperature show that the nanocrystal size changes with oxygen concentration and annealing temperature. The PL dependence on the temperature can be understood considering a competition between radiative and non-radiative processes. In samples with erbium the non-radiative recombination rate is higher than in samples without erbium. The study of the nanocrystal and Er3+ PL show that Er3+ behaves as non-radiative recombination centers for excited carriers in the nanocrystals. Part of the energy from the nanocrystals is transferred to Er3+ instead of being emitted as light. The Er3+ PL intensity depends on the nanocrystal PL intensity and is higher in samples containing nanocrystals ~3nm (which emit at ~1.5eV), indicating that the energy transfer is resonant (with the 4I15/2 -----> 4I9/2 Er3+excitation at ~1.5eV) ZnO nanowires were prepared by vapor-liquid-solid (VLS) deposition and by electrospinning. In the VLS method erbium is deposited on the nanowires after growth. In the electrospinning method a metallorganic compound is added to the polymer precursor. Erbium PL is observed when the samples are excited by one of the Er3+ higher transitions. Er2O3 nano-crystals are observed by HRTEM on the surface of the nanowires prepared by VLS. EXAFS measurements in these samples show that the Erneighborhood is identical to that of E2O<>3 indicating that there was no substitutional / Doutorado / Física / Doutor em Ciências

Orientador: Mônica Alonso Cotta / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin / Made available in DSpace on 2018-08-19T18:21:16Z (GMT). No. of bitstreams: 1 Oliveira_DouglasSoaresde_M.pdf: 3151118 bytes, checksum: 954bfe85e80e3ae53e5e5c87d10aa961 (MD5) Previous issue date: 2012 / Resumo: O estudo em nanofios semicondutores é crescente, seja pelo grande potencial de aplicações previsto para eles, seja para entender a dinâmica de formação dessas nanoestruturas. Entretanto, estes dois elementos estão ligados, pois é necessário entender o processo de síntese dos nanofios semicondutores para utilizar todo o seu potencial para aplicações. Neste trabalho, crescemos e estudamos nanofios de fosfeto de índio. Os nanofios foram crescidos pela técnica vapor-líquido-sólido em uma câmara de crescimento epitaxial por feixe químico (CBE). Através de microscopia eletrônica de varredura e microscopia eletrônica de transmissão, obtivemos dados para análise dos nossos resultados. Os parâmetros de crescimento utilizados foram escolhidos de forma que nossos nanofios apresentassem um número bastante significativo de falhas de empilhamento. Utilizamos também nanopartículas catalisadoras muito pequenas (~5nm). Nosso resultado principal foi uma nova morfologia para nanofios. Obtivemos nanofios com variações periódicas de diâmetro sem modificar os parâmetros durante o crescimento. Sendo a distância entre essas variações de diâmetro crescente com o inverso do fluxo do precursor de índio (Trimetil-índio) fornecido durante o crescimento. Análise por microscopia eletrônica de transmissão nos mostrou que essas oscilações periódicas de diâmetro estão associadas com um aumento muito grande no número de falhas de empilhamento e mudanças na fase cristalográfica, de wurtzita para blenda de zinco. Esta morfologia foi modelada por nós como a nanopartícula englobando parcialmente a lateral do nanofio periodicamente durante o crescimento. Nosso modelo é baseado em considerações sobre a competição entre as rotas de incorporação de índio durante o crescimento, as condições termodinâmicas para a nucleação na linha de três fases e estabilidade mecânica da nanopartícula sobre o nanofio durante o crescimento / Abstract: The study of semiconductor nanowires is growing, either due to the great potential for applications or to understand the dynamics of formation of these nanostructures. However, these two elements are linked since it is necessary to understand the synthesis of semiconductor nanowires in order to use all its potential for applications. In this work, we studied and grew nanowires of indium phosphide. These nanowires were grown by the vapor-liquid-solid method on a chemical beam epitaxy (CBE) chamber. They were studied by scanning and transmission electron microscopy. The growth parameters used were chosen so that our NWs presented a significant number of stacking faults and very small (~5nm) catalyst nanoparticles (NPs). Our main result was the observation of a new NW morphology. We have obtained NWs with periodical variations in diameter without any changes in growth parameters during the run. The distance between these oscillations depends almost linearly on the inverse of the Indium precursor flow (TMI) provided during growth. Analysis by transmission electron microscopy has shown that the periodic oscillations in diameter are associated with a very large increase of SF densities and crystallographic phase changes, from Wurtzite to Zinc Blende phase. We have modeled the formation of this morphology as the NP partly wetting the NW sidewalls periodically during growth. Our model is based in considerations of competition between the routes of incorporation of indium during growth, the thermodynamic conditions for nucleation at the three-phase line and mechanical stability of the NP on the NW during growth / Mestrado / Física / Mestre em Física

Orientador: Monica Alonso Cotta / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin / Made available in DSpace on 2018-08-04T02:49:32Z (GMT). No. of bitstreams: 1 Bortoleto_JoseRobertoRibeiro_D.pdf: 16802950 bytes, checksum: 1ef2bf92db0b00f30e5db9c5e3e3f34d (MD5) Previous issue date: 2005 / Resumo: Neste trabalho estudamos os mecanismos de crescimento durante a epitaxia de estruturas III-V baseadas na liga InP. Em particular, o principal objetivo foi correlacionar os mecanismos cinéticos durante a nucleação de nanoestruturas auto-formadas com as propriedades estruturais da camada que serve de substrato. Todas as amostras foram crescidas usando um sistema de epitaxia por feixe químico (CBE). De forma geral as amostras foram caracterizadas usando microscopia de força atômica (AFM), microscopia eletrônica de transmissão (TEM), difração de elétrons de alta energia (RHEED) e difração de raios-X. Na primeira parte deste trabalho correlacionamos as mudanças morfológicas nos filmes homoepitaxiais de InP com o padrão de RHEED exibido durante o crescimento epitaxial. Mostramos que as mudanças morfológicas de 3D para 2D com os parâmetros de crescimento estão diretamente relacionadas com as reconstruções superficiais 2x1 e 2x4, respectivamente. Além disso, indicamos que a formação de defeitos morfológicos é devido à dimerização In-P, através da ativação local do mecanismo de bias na difusão. Por outro lado, também investigamos o efeito dos parâmetros de crescimento (temperatura, taxa de crescimento e quantidade de material) na nucleação e auto-formação de ilhas de InP sobre InGaP/GaAs. Na segunda parte desta tese concentramos nossa atenção no efeito das propriedades da camada buffer de InGaP sobre nanoestruturas auto-formadas, principalmente sobre a sua organização espacial. Para tanto, em primeiro lugar, investigamos as propriedades de bulk da liga de InGaP e a dependência com os parâmetros de crescimento. Nossos resultados mostram que o InGaP exibe tanto ordenamento atômico de rede quanto modulação de composição. Estes dois fenômenos estão correlacionados com o tipo de reconstrução superficial. Em específico, a liga de InGaP apresenta ordenamento CuPtB quando a superfície exibe reconstrução superficial 2x1, conforme descrito na literatura. Por outro lado, a reconstrução superficial 2x4 desempenha um papel importante no fenômeno de modulação de composição. De fato, tanto a modulação de composição quanto a morfologia superficial do filme depende dos mecanismos cinéticos de superfície, que envolvem tanto os átomos adsorvidos de In quanto de Ga. Por fim mostramos que a modulação de composição na liga de InGaP pode organizar espacialmente a nucleação de ilhas de InP em uma rede quadrada. Além disso, mostramos que é possível criar redes bidimensionais de pontos quânticos de InAs/GaAs a partir do arranjo espacialmente ordenado das ilhas de InP/InGaP / Abstract: In this work we study the growth mechanisms during epitaxy of III-V structures based on InP. The main goal was to correlate the kinetic mechanisms during nucleation of self-assembled nanostructures with the bulk properties of the buffer layer. All samples were grown by chemical beam epitaxy (CBE) and characterized using atomic force microscopy (AFM), transmission electron microscopy (TEM), reflection high-energy electron diffraction (RHEED) and X-ray diffraction. In the first part of this work we correlate the morphological changes in homoepitaxial InP films with the RHEED pattern during growth process. We show that the morphological transition from 3D to 2D with growth parameters is related to changes in surface reconstruction, from 2x1 to 2x4. Moreover, we point out that the formation of morphological defects is due to mixed In-P dimerization, via the local activation of the diffusion bias mechanism. On the other hand, we also investigate the influence of the growth parameters (temperature, growth rate and amount of deposited material) on the nucleation and selfassembly of InP islands grown on InGaP/GaAs layers. In the second part of this work we concentrate our attention on the InGaP bulk properties, and their effect on the self-assembled InP nanostructures, mainly regarding their spatial ordering. In this way, we first investigate the dependence of InGaP bulk properties with the growth parameters. Our results show that our InGaP layers exhibit atomic ordering as well as compositional modulation. Both phenomena are correlated to the surface reconstruction exhibited by the InGaP surface during growth process. The InGaP alloy presents CuPtB atomic ordering when the RHEED pattern shows 2x1 reconstruction, in agreement with reports in literature. On the other hand, the 2x4-type reconstruction plays an important role in the compositional modulation phenomena. Actually, both compositional modulation and surface morphology of InGaP films depend on surface kinetic mechanisms, and thus on In and Ga adatom mobilities. At last we show that the compositional modulation in the InGaP alloy can be used to organize spatially the InP islands in a square lattice. Moreover, we point out that it is possible to produce bidimensional lattices of InAs/GaAs quantum dots starting from a template of laterally organized InP/InGaP nanostructures / Doutorado / Física da Matéria Condensada / Doutor em Ciências

Orientadora: Mônica Alonso Cotta / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin / Made available in DSpace on 2018-08-31T00:06:01Z (GMT). No. of bitstreams: 1 Silva_AldelianeMariada_M.pdf: 11574559 bytes, checksum: 5c39733d3a4441b98e7edbef8adbd795 (MD5) Previous issue date: 2016 / Resumo: Este trabalho apresenta resultados de nossa investigação sobre as propriedades elétricas do biossensor do tipo transistor de efeito de campo (FET, do inglês Field Effect Transistor) baseado em fosfeto de índio (InP). A estrutura deste biossensor consiste em um filme fino de InP do tipo-n crescido por Epitaxia de Feixe Químico (CBE, do inglês Chemical Beam Epitaxy) sobre um substrato de InP semi-isolante. No nosso biosensor, o contato da porta foi substituído por uma camada de biomoléculas carregadas de interesse para a detecção, funcionalizadas na camada de óxido do InP. O campo elétrico associado a estas biomoléculas pode modular o canal de condução. O sistema de interação específica utilizado foi a hibridização de fitas de ssDNA (single stranded DNA) complementares, onde os oligonucleotídeos receptores (probe) ssDNA foram imobilizados covalentemente na superfície da amostra. Este procedimento foi realizado através da oxidação com plasma de O2, seguida da funcionalização utilizando etanolamina e polietileno glicol (PEG), que serve como linker para a imobilização de receptores na superfície. As medidas elétricas de detecção foram feitas com as moléculas de target diluídas em buffer TRIS. A hibridização do DNA provoca um aumento na densidade de cargas na superfície, que consequentemente aumenta a largura da região de depleção no semicondutor, variando a resistência medida. A resposta do biossensor corresponde à variação da resistência em função da concentração de target. O biossensor apresentou sensibilidade para medidas de concentrações entre 10 pM e 30 pM, onde ocorre a saturação, e o tempo de resposta, no qual encontramos a estabilização do sinal medido, foi de aproximadamente 20 min. Variando a concentração de portadores e a espessura da camada semicondutora, verificamos alterações no limite de saturação (até ?M) e na sensibilidade do dispositivo. O controle destas propriedades, porém, mostrou-se limitado devido à variações na dopagem residual do semicondutor, e por isso discutimos aqui alternativas à geometria do dispositivo. Analisamos também a camada funcionalizada através de medidas de topografia e potencial de superfície usando métodos de microscopia de varredura por sonda (SPM, do inglês Scanning Probe Microscopy). Pudemos identificar a variação no potencial de superfície associada à imobilização do PEG e do DNA probe, mas não obtivemos resolução para o DNA target. Esta técnica permitiu porém verificar a estratificação de quatro níveis de potencial de superfície, no caso onde a funcionalização resultou em camadas mais espessas do que os valores típicos (~2 nm de espessura), em pequenas áreas do semicondutor / Abstract: This dissertation presents our results for the electrical properties investigation of Indium Phosphide (InP) based Field Effect Transistor (FET) biosensor. The structure of this biosensor consists of a thin n-type InP film grown by Chemical Beam Epitaxy (CBE) on a semi-insulating InP substrate. In our biosensor, the gate contact has been replaced by charged biomolecules of interest for detection, functionalized to the InP oxide layer. The electric field associated with these biomolecules provides the conduction channel modulation. The specific interaction system used here was the hybridization of single stranded-DNA (ssDNA) complementary oligonucleotides, for which the ssDNA receivers (probes) were covalently immobilized on the sample surface. The functionalization was carried out by oxidation with O2 plasma, followed by grafting biomolecules using ethanolamine and polyethylene glycol (PEG), which act as a linker for immobilizing the receptors on the surface. Electrical detection measurements were made with the target molecules diluted in TRIS buffer. DNA hybridization causes an increase in the surface charge density; consequently the semiconductor depletion width increases, affecting the measured resistance. The biosensor response function corresponds to the resistance variation as a function of target concentration. Our biosensor showed measured sensitivity to concentrations between 10 pM and 30 pM, for which signal saturation occurs. The response time, for which the measured signal stabilization was observed, was approximately 20 min. By varying the carrier concentration and the thickness of the semiconductor layer, we observed changes in the saturation limit (up ?M) and device sensitivity. The control of these properties, however, is limited due to variations in the residual doping of the semiconductor. Therefore we discuss here alternative device geometries. We also analyzed the functionalized layer by topography and surface potential measurements obtained using scanning probe microscopy (SPM) methods. We were able to identify the change in surface potential associated with the immobilization of PEG and probe DNA, but not for the target DNA. These techniques have however shown four surface potential levels in the case when the functionalization resulted in non-uniform layers, thicker than the typical values (~ 2 nm), in small areas of the semiconductor / Mestrado / Física / Mestra em Física / 165741/2014-7 / CNPQ

京都大学 / 0048 / 新制・課程博士 / 博士(エネルギー科学) / 甲第22795号 / エネ博第409号 / 新制||エネ||78(附属図書館) / 京都大学大学院エネルギー科学研究科エネルギー基礎科学専攻 / (主査)教授 萩原 理加, 教授 佐川 尚, 教授 野平 俊之 / 学位規則第4条第1項該当 / Doctor of Energy Science / Kyoto University / DFAM

No description available.

No description available.

A series of iron, cobalt and nickel transition metal phosphides was synthesized by means of temperature-programmed reduction (TPR) of the corresponding phosphates. The same materials, Fe₂P, CoP and Ni₂P, were also prepared on a silica (SiO₂) support. The phase purity of these catalysts was established by x-ray diffraction (XRD), and the surface properties were determined by N₂ BET specific surface area (Sg) measurements and CO chemisorption. The activities of the silica-supported catalysts were tested in a three-phase trickle bed reactor for the simultaneous hydrodenitrogenation (HDN) of quinoline and hydrodesulfurization (HDS) of dibenzothiophene using a model liquid feed at realistic conditions (30 atm, 370 °C). The reactivity studies showed that the nickel phosphide (Ni₂P/SiO₂) was the most active of the catalysts. Compared with a commercial Ni-Mo-S/g-Al₂O₃ catalyst at the same conditions, Ni₂P/silica had a substantially higher HDS activity (100 % vs. 76 %) and HDN activity (82 % vs. 38 %). Because of their good hydrotreating activity, an extensive study of the preparation of silica supported nickel phosphides, Ni₂P/SiO₂, was carried out. The parameters investigated were the phosphorus content and the weight loading of the active phase. The most active composition was found to have a starting synthesis Ni/P ratio close to 1/2, and the best loading of this sample on silica was observed to be 18 wt.%. Extended x-ray absorption fine structure (EXAFS) and x-ray absorption near edge spectroscopy (XANES) measurements were employed to determine the structures of the supported samples. The main phase before and after reaction was found to be Ni₂P, but some sulfur was found to be retained after reaction. A comprehensive scrutiny of the HDN reaction mechanism was also made over the Ni₂P/SiO₂ sample (Ni/P = 1/2) by comparing the HDN activity of a series of piperidine derivatives of different structure. It was found that piperidine adsorption involved an a-H activation and nitrogen removal proceeded mainly by means of a b-H activation though an elimination (E2) mechanism. The relative elimination rates depended on the type and number of b-hydrogen atoms. Elimination of b-H atoms attached to tertiary carbon atoms occurred faster than those attached to secondary carbon atoms. Also, the greater the number of the b-H atoms, the higher the elimination rates. The nature of the adsorbed intermediates was probed by Fourier transform infrared spectroscopy (FTIR) and temperature-programmed desorption (TPD) of the probe molecule, ethylamine. This measurement allowed the determination of the likely steps in the hydrodenitrogenation reaction. / Ph. D.

No / Cd3P2 quantum dots (QDs) have been synthesized in both aqueous and high boiling point surfactant solutions via a gas-bubbling method. The synthesized QDs exhibit photoluminescent wavelengths spanning across the visible red to the near-infrared (NIR) spectral region. Two types of shell materials, SiO2 nanobeads and PS micro-spheres, have been employed to encapsulate the Cd3P2 QDs which provide protecting layers against physiological solutions. The coating layers are proven to enhance the optical and chemical stability of Cd3P2 QDs, and make the fluorescent particles capable of sustaining long-term photo-oxidation. To demonstrate the applicability of the bio-labelling, the fluorescent composite particles (PS@QDs, SiO2@QDs) were injected into a culture medium of colorectal carcinoma (LoVo) cells. The results demonstrated that the PS@QDs exhibited a brighter fluorescence, but the SiO2@QDs provided a better photostability which consequently led to long-term cancer cell detection as well as a much lower release of toxic Cd2+ into the PBS solutions.

Ce travail de thèse porte sur la synthèse organo-métallique de nanoparticules (NPs) semi-conductrices colloïdales de phosphures d’indium (InP), de zinc (Zn3P2) et de structures cœur/coquille obtenues par la croissance d’une couche de sulfure de zinc (ZnS) à la surface des NPs. Les objectifs consistent à comprendre et maîtriser la synthèse dans le but de décaler les longueurs d’onde d’absorption et d’émission vers le proche infra-rouge, domaine spectral intéressant pour l’imagerie biomédicale.Le premier chapitre présente l’état de l’art sur les nanocristaux (NCx) d’InP et d’InP/ZnS. Un bref rappel sur les propriétés physico-chimiques des NCx semi-conducteurs est présenté et différentes synthèses sont décrites. Une attention toute particulière a été portée sur la taille des NCx, le décalage de l’émission de fluorescence vers les plus grandes longueurs d’onde et l’optimisation des rendements quantiques. Les potentialités offertes par ces objets soit pour les diodes électroluminescentes (LED) blanches soit pour l’imagerie biomédicale montrent l’intérêt d’utiliser les NCx de type InP/ZnS plutôt que d’autres matériaux à base d’éléments toxiques (Cd, Pb, …).Le deuxième chapitre porte sur une synthèse à partir des carboxylates d’indium connue de la littérature. Le but est alors de caractériser la structure des NPs pour comprendre le déroulement de la synthèse et de l’enrobage. Des mesures par résonance magnétique nucléaire (RMN) en phase solide et spectroscopie photo-électronique par rayons X (XPS) révèlent l’oxydation des NPs d’InP. La couche d’oxyde qui se forme durant la synthèse des NPs d’InP s’épaissit lors de l’enrobage. Cette oxydation provient d’un couplage décarboxylant des acides carboxyliques à haute température en présence des NPs. Elle serait à l’origine de l’inhibition de croissance des objets, ce qui limiterait les gammes de longueurs d’onde atteignables.Le troisième chapitre concerne une nouvelle synthèse à partir d’amidinate d’indium au lieu des carboxylates d’indium. L’intérêt de cette approche est la possibilité d’abaisser considérablement la température de réaction (150°C au lieu de 280°C) et ainsi d’éviter la réaction secondaire de décarboxylation. Un enrobage à basse température (150°C) est aussi mis en place. La synthèse induit également une oxydation de la surface des NPs d’InP. Un nouveau couplage a lieu entre les ligands, l’acide palmitique et l’hexadécylamine, et donne de nouvelles conditions oxydantes. Le jeu sur les ratios des ligands montre qu’en bouleversant le milieu réactionnel, les NPs d’InP ne présentent pas de réponse en luminescence concluante. La synthèse et l’enrobage sont alors réalisés sous atmosphère de dihydrogène (H2) en réacteur Fisher-Porter dans le but de contrer ces conditions oxydantes. La synthèse et l’enrobage donnent des tailles de NPs de l’ordre de 3,4 nm (condition nécessaire pour s’approcher d’une émission dans l'infra-rouge) et un rendement quantique de 18-20 %, résultats encore jamais atteints lors de cette thèse.Le dernier chapitre est consacré à une étude exploratoire sur les NPs de Zn3P2. Le phosphure de zinc est un matériau prometteur du fait de l’abondance de ses constituants non toxiques et des longueurs d’onde potentiellement accessibles. Différents paramètres de synthèse sont étudiés et les propriétés structurales et optiques sont caractérisées. Des résultats préliminaires sur l’enrobage montrent des difficultés liées à la stabilité des NPs de Zn3P2. L’utilisation de l’oxyde de trioctylphosphine (TOPO) semble permettre la passivation de ces NPs à l’air et en travaillant sous H2 une meilleure stabilité est envisageable / Résumé de la thèse en anglais : This PhD investigation focuses on organometallic synthesis of indium phosphide (InP), zinc phosphide (Zn3P2) colloidal semiconductor nanoparticles (NPs) and core/shell structures which were obtained by the growth of a layer of zinc sulfide (ZnS) on the surface. The objectives are to understand and control the synthesis in order to shift the absorption and emission wavelengths to the near infra-red range, interesting for biomedical imaging.The first chapter presents the state of the art on the InP and InP/ZnS nanocrystals (NCx). A brief recall on the physical and chemical properties of semiconductor NCx is presented and various syntheses are described. Particular attention was paid to the size of NCx, the shift of the fluorescence emission to higher wavelengths and the optimization of quantum yields. The potential of these objects for white light emitting diodes (LED) or biomedical imaging shows the value added of using InP/ZnS NCx rather than other materials based on toxic elements such as cadmium, lead elements…The second chapter focuses on a synthesis from indium carboxylates known in the literature. The goal is to characterize the structure of NPs to understand the procedure of the synthesis and the coating. Measurements by Nuclear Magnetic Resonance (NMR) in solid state and Photoelectronic X-ray spectroscopy (XPS) revealed the oxidation of InP of the NPs. This oxide layer increases during the coating. This originates from a decarboxylating coupling of carboxylic acids at high temperature in the presence of NPs. This oxidation is believed to inhibit the growth of the object, which restricts the attainable range of wavelengths.The third chapter provides a novel synthesis from indium amidinate instead of indium carboxylate. The advantage of this approach is the potential to lower significantly the reaction temperature (150°C instead of 280°C) and to avoid secondary decarboxylation reaction. A coating with ZnS at low temperature (150°C) is also developed. The synthesis of InP NPs also causes an oxidation of the surface. A coupling takes place again between the ligands, palmitic acid and hexadecylamine providing new oxidizing conditions. The study of different ratios of ligands shows that when the reaction medium is modified, the InP NPs do not exhibit a conclusive luminescence response. Synthesis and coating are carried out under an atmosphere of hydrogen (H2) in Fisher-Porter reactor in order to counter these oxidizing conditions. NPs with diameters of the order of 3,4 nm (a necessary condition to approach the infra-red emission) and a quantum yield of 18-20% are thus obtained. These had never been observed before during this thesis.The last chapter is devoted to an exploratory study on Zn3P2 NPs. Zinc phosphide is a promising material because of non-toxic and abundant constituents, and potential access to near infra-red wavelengths. Different synthesis parameters are studied and the structural and optical properties are characterized. Preliminary results on the coating show instabilities of the Zn3P2 NPs. The use of trioctylphoshine oxide (TOPO) appears to allow the passivation of the NPs in the air and a better stability is possible under an atmosphere of H2