Abstract Silicon carbide is a versatile material amenable to variety of applications from electrical insulation to surface passivation, diffusion-barrier in optoelectronic and high-frequency devices. This research presents a fundamental study of a-SiC:H films with variable stoichiometries deposited using novel technique, DC saddle-field plasma-enhanced chemical-vapour deposition, a departure from conventional RF PECVD commonly used in industry. DCSF PECVD is an alternative technique for low temperature large area deposition. Stoichiometric a-SiC:H obtained by fine-tuning precursor gas mixture. Annealing up to 800oC showed no significant change in elemental composition; particularly indicating thermal stability at stoichiometry. Ellipsometry showed wide range of optical gaps whose maximum surpasses values reported in literature. Refractive index measured and change in values studied as function of increasing carbon content in the films. Also attainment of very smooth surface morphology for stoichiometric a-SiC:H films reported. Surface roughness of 1 nm rms demonstrated for films grown at temperature as low as 225oC.

Abstract Silicon carbide is a versatile material amenable to variety of applications from electrical insulation to surface passivation, diffusion-barrier in optoelectronic and high-frequency devices. This research presents a fundamental study of a-SiC:H films with variable stoichiometries deposited using novel technique, DC saddle-field plasma-enhanced chemical-vapour deposition, a departure from conventional RF PECVD commonly used in industry. DCSF PECVD is an alternative technique for low temperature large area deposition. Stoichiometric a-SiC:H obtained by fine-tuning precursor gas mixture. Annealing up to 800oC showed no significant change in elemental composition; particularly indicating thermal stability at stoichiometry. Ellipsometry showed wide range of optical gaps whose maximum surpasses values reported in literature. Refractive index measured and change in values studied as function of increasing carbon content in the films. Also attainment of very smooth surface morphology for stoichiometric a-SiC:H films reported. Surface roughness of 1 nm rms demonstrated for films grown at temperature as low as 225oC.

Neste trabalho investigamos as modificações na morfologia superficial e estrutura de filmes finos de silício amorfo hidrogenado, resultantes da irradiação com pulsos ultracurtos de femtossegundos (150 fs, 775 nm e 1 kHz). Os processos de microfabricação foram conduzidos varrendo, a velocidade constante, um feixe laser com diferentes fluências (1,8 a 6,2 MJ/m2) sobre a amostra. Os espectros de transmissão apresentaram queda para amostras irradiadas, cujas imagens de microscopia eletrônica de varredura mostraram estruturas superficiais condizentes com o fenômeno de LIPSS (Laser Induced Periodic Surface Structures). Uma análise estatística das imagens de microscopia de força atômica foi realizada com um programa que identifica e caracteriza os domínios (picos) produzidos pela microfabricação. O histograma de altura da amostra irradiada com uma fluência de 3,1 MJ/m2 mostrou que a altura média dos picos produzidos é de 15 nm, menor que o centro da distribuição de alturas para uma amostra não irradiada. Porém, para fluências acima de 3,7 MJ/m2 a morfologia é dominada pela formação de agregados. Medidas de espectroscopia Raman revelaram a formação de uma fração de silício cristalino, após a irradiação com pulsos de femtossegundos, de até 77% para 6,2 MJ/m2. Determinamos ainda uma diminuição da dimensão dos nanocristais produzidos com o aumento da fluência do laser de excitação. Portanto, nossos resultados mostram que há um compromisso entre as propriedades obtidas pela microfabricação (transmissão, distribuição de picos, fração de cristalização e tamanho dos nanocristais produzidos) que deve ser levado em conta ao aplicar a técnica de microestruturação com laser de femtossegundos. / In this work we investigated surface morphology and structural modification on hydrogenated amorphous silicon (a-Si:H) thin films, resulting from femtosecond laser irradiation (150 fs, 775 nm and 1 kHz). Microfabrication processes were carried out scanning sample´s surface, at constant speed, with distinct laser fluencies (from 1.8 to 6.2 MJ/m2). A decrease was observed in the transmission spectra of irradiated samples, whose scanning electron microscopy images revealed surface structures compatible with the Laser Induced Periodic Surface Structure (LIPSS) phenomenon. A statistical analyzes of Atomic Force Microcopy images was performed using a specially developed software, that identifies and characterizes the domains (spikes) produced by the laser irradiation. The height histogram for a sample irradiated with 3.1 MJ/m2 reveals that the average height of the produced spikes is at 15 nm, which is smaller than the center of height distribution for non-irradiated sample. For fluencies higher than 3.7 MJ/m2, however, aggregation of the produced spikes dominates the sample morphology. Raman spectroscopy revealed the formation of a crystalline fraction of 77% for laser fluence irradiation of 6.2 MJ/m2, as well as a decrease in size of the produced crystals as a function of fluence. Therefore, our results indicate that there is a compromise of the sample transmission, spikes distribution, crystallization fraction and size of nanocrystals obtained by fs-laser irradiation, which has to be taken into consideration when using this material processing method.

This thesis proposes and demonstrates a hydrogenated amorphous silicon passivated, inverted photovoltaic device on n-type silicon, utilizing a Laser Fired Emitter on a rear i-a- Si:H/SiOx dielectric stack. This novel low-temperature-fabricated device architecture constitutes the first demonstration of an LFE on a dielectric passivation stack. The optimization of the device is explored through Sentaurus computational modeling, predicting a potential efficiency of >20%. Proof of concept devices are fabricated using the DC Saddle Field PECVD system for the deposition of hydrogenated amorphous silicon passivation layers. Laser parameters are explored highlighting pulse energy density as a key performance determining factor. Annealing of devices in nitrogen atmosphere shows performance improvements albeit that the maximum annealing temperature is limited by the thermal stability of the passivation. A proof of concept device efficiency of 11.1% is realized forming the basis for further device optimization.

This thesis proposes and demonstrates a hydrogenated amorphous silicon passivated, inverted photovoltaic device on n-type silicon, utilizing a Laser Fired Emitter on a rear i-a- Si:H/SiOx dielectric stack. This novel low-temperature-fabricated device architecture constitutes the first demonstration of an LFE on a dielectric passivation stack. The optimization of the device is explored through Sentaurus computational modeling, predicting a potential efficiency of >20%. Proof of concept devices are fabricated using the DC Saddle Field PECVD system for the deposition of hydrogenated amorphous silicon passivation layers. Laser parameters are explored highlighting pulse energy density as a key performance determining factor. Annealing of devices in nitrogen atmosphere shows performance improvements albeit that the maximum annealing temperature is limited by the thermal stability of the passivation. A proof of concept device efficiency of 11.1% is realized forming the basis for further device optimization.

Neste trabalho investigamos as modificações na morfologia superficial e estrutura de filmes finos de silício amorfo hidrogenado, resultantes da irradiação com pulsos ultracurtos de femtossegundos (150 fs, 775 nm e 1 kHz). Os processos de microfabricação foram conduzidos varrendo, a velocidade constante, um feixe laser com diferentes fluências (1,8 a 6,2 MJ/m2) sobre a amostra. Os espectros de transmissão apresentaram queda para amostras irradiadas, cujas imagens de microscopia eletrônica de varredura mostraram estruturas superficiais condizentes com o fenômeno de LIPSS (Laser Induced Periodic Surface Structures). Uma análise estatística das imagens de microscopia de força atômica foi realizada com um programa que identifica e caracteriza os domínios (picos) produzidos pela microfabricação. O histograma de altura da amostra irradiada com uma fluência de 3,1 MJ/m2 mostrou que a altura média dos picos produzidos é de 15 nm, menor que o centro da distribuição de alturas para uma amostra não irradiada. Porém, para fluências acima de 3,7 MJ/m2 a morfologia é dominada pela formação de agregados. Medidas de espectroscopia Raman revelaram a formação de uma fração de silício cristalino, após a irradiação com pulsos de femtossegundos, de até 77% para 6,2 MJ/m2. Determinamos ainda uma diminuição da dimensão dos nanocristais produzidos com o aumento da fluência do laser de excitação. Portanto, nossos resultados mostram que há um compromisso entre as propriedades obtidas pela microfabricação (transmissão, distribuição de picos, fração de cristalização e tamanho dos nanocristais produzidos) que deve ser levado em conta ao aplicar a técnica de microestruturação com laser de femtossegundos. / In this work we investigated surface morphology and structural modification on hydrogenated amorphous silicon (a-Si:H) thin films, resulting from femtosecond laser irradiation (150 fs, 775 nm and 1 kHz). Microfabrication processes were carried out scanning sample´s surface, at constant speed, with distinct laser fluencies (from 1.8 to 6.2 MJ/m2). A decrease was observed in the transmission spectra of irradiated samples, whose scanning electron microscopy images revealed surface structures compatible with the Laser Induced Periodic Surface Structure (LIPSS) phenomenon. A statistical analyzes of Atomic Force Microcopy images was performed using a specially developed software, that identifies and characterizes the domains (spikes) produced by the laser irradiation. The height histogram for a sample irradiated with 3.1 MJ/m2 reveals that the average height of the produced spikes is at 15 nm, which is smaller than the center of height distribution for non-irradiated sample. For fluencies higher than 3.7 MJ/m2, however, aggregation of the produced spikes dominates the sample morphology. Raman spectroscopy revealed the formation of a crystalline fraction of 77% for laser fluence irradiation of 6.2 MJ/m2, as well as a decrease in size of the produced crystals as a function of fluence. Therefore, our results indicate that there is a compromise of the sample transmission, spikes distribution, crystallization fraction and size of nanocrystals obtained by fs-laser irradiation, which has to be taken into consideration when using this material processing method.

<p>When the amorphous silicon (a-Si) dangling bonds are bonded to hydrogen the concentration of the dangling bond is decreased. The resulting film is called hydrogenated amorphous silicon (a-Si:H). The reduction in the dangling bonds concentration improves the optoelectrical properties of the film. The improved properties of a-Si:H makes it possible to manufacture electronic devices including a solar cell. A solar cell device based on the hydrogenated amorphous silicon (a-Si:H) was fabricated using the Hot-Wire Chemical Vapour Deposition (HWCVD). When an n-i-p solar cell configuration is grown, the norm is that the p-doped layer is deposited from a mixture of silane (SiH4) gas with diborane (B2H6). The boron atoms from diborane bonds to the silicon atoms and because of the number of the valance electrons, the grown film becomes a p-type film. Aluminium is a group 3B element and has the same valence electrons as boron, hence it will also produce a p-type film when it bonds with silicon. In this study the p-doped layer is grown from the co-deposition of a-Si:H from SiH4 with aluminium evaporation resulting in a crystallized, p-doped thin film. When this thin film is used in the n-i-p cell configuration, the device shows photo-voltaic activity. The intrinsic layer and the n-type layers for the solar cell were grown from SiH4 gas and Phosphine (PH3) gas diluted in SiH4 respectively. The individual layers of the solar cell device were characterized for both their optical and electrical properties. This was done using a variety of experimental techniques. The analyzed results from the characterization techniques showed the films to be of device quality standard. The analysed results of the ptype layer grown from aluminium showed the film to be successfully crystallized and doped. A fully functional solar cell was fabricated from these layers and the cell showed photovoltaic activity.<br /> &nbsp / </p>

The production of low cost, large area display systems requires a light emitting material compatible with the standard silicon (Si) based complementary metal oxide semiconductor (CMOS) technology. The crystalline bulk Si is an indirect band semiconductor with very poor optical properties. On the other hand, hydrogenated amorphous Si (a-Si:H) based wide gap alloys exhibit strong visible photoluminescence (PL) at room temperature, owing to the release of the momentum conservation law. Still, the electroluminescence (EL) intensity from the diodes based on these alloys is weak due to the limitation of the current transport by the localized states. In the frame of this work, first, the luminescent properties of amorphous silicon nitride (a-SiNx:H) thin films grown in a plasma enhanced chemical vapor deposition (PECVD) system were analyzed with respect to the nitrogen content. Then, the doping effciency of p- and n-type hydrogenated nanocrystalline Si (nc-Si:H) films was optimized via adjusting the deposition conditions. Next, the junction quality of these doped layers was checked and further improved in a homojunction pin diode. Heterojunction pin light emitting diodes (LEDs) were fabricated with a-SiNx:H as the luminescent active layer. The EL effciency of the fresh diodes was very low, as expected. As a solution, the diodes were electro-formed under high electric field leading to nanocrystallization accompanied by a strong visible light emission from the whole diode area. The current-voltage (I-V) and EL properties of these transformed diodes were investigated in detail.

<p>When the amorphous silicon (a-Si) dangling bonds are bonded to hydrogen the concentration of the dangling bond is decreased. The resulting film is called hydrogenated amorphous silicon (a-Si:H). The reduction in the dangling bonds concentration improves the optoelectrical properties of the film. The improved properties of a-Si:H makes it possible to manufacture electronic devices including a solar cell. A solar cell device based on the hydrogenated amorphous silicon (a-Si:H) was fabricated using the Hot-Wire Chemical Vapour Deposition (HWCVD). When an n-i-p solar cell configuration is grown, the norm is that the p-doped layer is deposited from a mixture of silane (SiH4) gas with diborane (B2H6). The boron atoms from diborane bonds to the silicon atoms and because of the number of the valance electrons, the grown film becomes a p-type film. Aluminium is a group 3B element and has the same valence electrons as boron, hence it will also produce a p-type film when it bonds with silicon. In this study the p-doped layer is grown from the co-deposition of a-Si:H from SiH4 with aluminium evaporation resulting in a crystallized, p-doped thin film. When this thin film is used in the n-i-p cell configuration, the device shows photo-voltaic activity. The intrinsic layer and the n-type layers for the solar cell were grown from SiH4 gas and Phosphine (PH3) gas diluted in SiH4 respectively. The individual layers of the solar cell device were characterized for both their optical and electrical properties. This was done using a variety of experimental techniques. The analyzed results from the characterization techniques showed the films to be of device quality standard. The analysed results of the ptype layer grown from aluminium showed the film to be successfully crystallized and doped. A fully functional solar cell was fabricated from these layers and the cell showed photovoltaic activity.<br /> &nbsp / </p>

It has been debated that among all the renewable energy alternatives, only solar energy offers sufficient resources to meet energy demands. Silicon thin film solar cells are at the frontier of commercial solar technology. Hot wire chemical vapour deposition (HWCVD) is the technique of choice for silicon thin film deposition due to the absence of ion bombardment and its independence toward geometry or electromagnetic properties of the substrate, as seen by plasma enhanced chemical vapour deposition (PECVD). With the implementation of nanostructures in a multi-band gap tandem solar cell, considerable improvement has been achieved over the single junction solar cells. Defect assisted tunnelling processes at the junctions between individual solar cells in a tandem structure solar cell largely affect the efficiency of these solar cells. In this contribution, the investigation toward the improvement of silicon thin films for tandem solar cell application is initiated. This study reports on the effects of hydrogen dilution and deposition time on six silicon thin films deposited at six specific deposition regimes. The thin film properties are investigated via X-Ray diffraction analysis, Raman spectroscopy, Fourier transform infra-red spectroscopy, elastic recoil detection analysis, scanning and transmission electron microscopy and UV-visible spectroscopy. This investigation revealed the dominating etching effect of atomic hydrogen with the increase in hydrogen dilution and a bonded hydrogen content (CH) exceeding 10 at.% for each of the six thin films. The optically determined void volume fraction and static refractive index remain constant, for each thin film, with the change in CH. A new deposition procedure, utilising the deposition conditions of the previously investigated thin films, is performed by HWCVD to deposit two silicon thin films. This deposition procedure involved either increasing (protocol 1) or decreasing (protocol 2) hydrogen dilution during deposition. Structural and optical variation with depth was observed for the dynamically deposited silicon thin films, with nano-voids existing across the entire cross section and bond angle variations which are indicative of good structural order. The optical absorption curves differ for the two silicon thin films whereas the optical density remains constant for both. / >Magister Scientiae - MSc