Este trabalho é uma contribuição às análises de forças de aprisionamento óptico exercidas sobre partículas esféricas por superposições discretas de feixes de Bessel. Um estudo teórico-numérico foi realizado no regime de óptica geométrica, completando as pesquisas já realizadas com tais feixes e no caso escalar, tanto no regime de Rayleigh quanto através de um formalismo eletromagnético completo. Investigam-se padrões longitudinais de intensidade de possível interesse prático, com potenciais de fornecer múltiplas armadilhas ópticas simultâneas utilizando dois métodos de análise. O primeiro parte da observação de que no regime paraxial todos os raios associados aos feixes se encontram quase paralelos entre si quando se toma como aproximação uma superposição de raios paralelos que incidem completamente sobre um hemisfério do espalhador. Tal método, entretanto, é naturalmente restrito pelas forças transversais. O segundo, que torna mais confiáveis e precisas as predições acerca da componente longitudinal de força, adota procedimentos mais robustos que levam em consideração tanto a contribuição da pressão de radiação (força de espalhamento) quanto a força gradiente devido a gradientes locais de intensidade associados a raios não-paralelos. Assim, acredita-se que este trabalho traz como contribuição um reforço a esta classe específica e promissora de feixes não difrativos como feixes de luz interessantes para aplicações em aprisionamento e micromanipulação óptica. / This work is a contribution to the analyses of optical trapping forces exerted on spherical particles by discrete superpositions of Bessel beams. A theoretical-numerical study has been carried out in the ray optics regime, completing the pre-existing research performed with such beams, in the scalar case, both in the Rayleigh regime and through a complete electromagnetic formalism. We investigate longitudinal intensity patterns of possible practical interest with potential to provide multiple simultaneous optical traps, by using two methods of analysis. The first assumes that, in the paraxial regime, all rays associated to the beams are almost parallel to each other, taking a superposition of parallel rays that are completely incident on a hemisphere of the scatterer as a suitable approximation. Such a method, however, is naturally constrained by the transverse forces. The second one, which makes the predictions about the longitudinal force component more reliable and accurate, adopts more robust procedures that take into consideration the contribution of the radiation pressure (scattering force) as well as the gradient force due to local intensity gradients associated to non-parallel rays. Thus it is hoped that this work will contribute to reinforce this specific and promising class of non-diffractive beams as interesting light beams for applications in optical trapping and micromanipulation.

Um sistema multi-feixe de pinças ópticas baseado na técnica de contraste de fase da ordem zero pode apresentar vantagens significativas sobre sistemas mecanicamente complexos e sensíveis ao alinhamento, e sobre tecnologias que, apesar de serem similares, requerem a customização de componentes ópticos. Porém, ao nosso conhecimento, este sistema até agora não tem sido implementado experimentalmente. Neste trabalho tem-se desenvolvido, como prova de princípio, o primeiro sistema baseado na técnica de contraste de fase da ordem zero gerador de múltiplas pinças ópticas. Esta técnica da óptica de Fourier utiliza conceitos do contraste de fase de Zernike e técnicas de codificação de dois pixels para gerar padrões de intensidade no plano da imagem que são diretamente relacionados a distribuições de fase no plano de entrada do sistema, o qual é formado por um modulador espacial de luz (SLM). Esta dissertação de mestrado descreve detalhadamente os passos tomados com o propósito de utilizar os campos estruturados de luz gerados pelo sistema de contraste de fase da ordem zero para aprisionar esferas de 2 µm de diâmetro de sílica fundida. Neste trabalho apresentamos os fundamentos teóricos do aprisionamento óptico e da técnica de contraste de fase da ordem zero, seguidos pela implementação de experimentos independentes em cada modalidade, e finalmente apresentamos a integração de ambos os sistemas dentro um sistema único de pinças ópticas multi-feixe. Apesar da baixa eficiência óptica do sistema, foi possível implementar um sistema de pinças ópticas duplas. Finalizamos o nosso trabalho na discussão detalhada das limitações do nosso arranjo óptico e comentamos sobre potenciais melhorias para aumentar a rigidez das pinças ópticas e a qualidade geral do sistema. / A multi-beam optical trapping system based on the zero order phase contrast technique may offer significant advantages over mechanically-complex, alignment-sensitive optical trapping systems, and over technologies that, though similar, require the customization of optics components. However, to our knowledge, such a system has not been yet implemented experimentally. We have developed, as a proof of principle, what we think is the first system based on the zero order phase contrast technique to successfully generate multiple optical traps. This Fourier optics technique makes use of existing concepts of Zernike phase contrast and two-pixel encoding techniques to generate intensity patterns in the image plane that are directly related to phase distributions in the input plane, which is comprised by a spatial light modulator (SLM). This master\'s dissertation describes in detail the steps taken towards using the structured light fields generated by a zero order phase contrast system to trap 2 µm diameter fused silica beads. We present the theoretical foundations of optical trapping and the zero order phase contrast technique, followed by the implementation of independent laboratory experiments in each modality, and finally integrate both systems into a single optical setup for multi-beam trapping. In spite of the low optical efficiency of the system, we were able to implement dual optical traps. We finalize by discussing in detail the limitations of our experimental setup in and comment on potential improvements to increase the stiffness of the optical traps and the overall quality of the system.

Orientador: Carlos Lenz Cesar / Tese (doutorado) - Universidade Estadual de Campinas, Instituto de Fisica "Gleb Wataghin" / Made available in DSpace on 2018-08-04T14:59:07Z (GMT). No. of bitstreams: 1 Fontes_Adriana_D.pdf: 3876787 bytes, checksum: 3edd1575e993d4685d7e82c8a3f77cfb (MD5) Previous issue date: 2004 / Resumo: Não informado / Abstract: Not informed. / Doutorado / Física / Doutor em Ciências

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Optical tweezers are a sensitive position and force transducer widely employed in physics and biology. In a focussed laser, forces due to radiation pressure enable to trap and manipulate small dielectric particles used as probes for various experiments. For sensitive biophysical measurements, microspheres are often used as a handle for the molecule of interest. The force range of optical traps well covers the piconewton forces generated by individual biomolecules such as kinesin molecular motors. However, cellular processes are often driven by ensembles of molecular machines generating forces exceeding a nanonewton and thus the capabilities of optical tweezers. In this thesis I focused, fifirst, on extending the force range of optical tweezers by improving the trapping e fficiency of the probes and, second, on applying the optical tweezers technology to understand the mechanics of molecular motors. I designed and fabricated photonically-structured probes: Anti-reflection-coated, high-refractive-index, core-shell particles composed of titania. With these probes, I significantly increased the maximum optical force beyond a nanonewton. These particles open up new research possibilities in both biology and physics, for example, to measure hydrodynamic resonances associated with the colored nature of the noise of Brownian motion. With respect to biophysical applications, I used the optical tweezers to study the mechanics of single kinesin-8. Kinesin-8 has been shown to be a very processive, plus-end directed microtubule depolymerase. The underlying mechanism for the high processivity and how stepping is affected by force is unclear. Therefore, I tracked the motion of yeast (Kip3) and human (Kif18A) kinesin-8s with high precision under varying loads. We found that kinesin-8 is a low-force motor protein, which stalled at loads of only 1 pN. In addition, we discovered a force-induced stick-slip motion, which may be an adaptation for the high processivity. Further improvement in optical tweezers probes and the instrument will broaden the scope of feasible optical trapping experiments in the future.

Pregnancy tests and related immunoassays are heavily dependent on specific and non-specific protein adsorption. These interfacial processes are affected by many factors that influence the in situ conformations of interfacially immobilised antibodies. This thesis examines a number of representative features with dual polarisation interferometry (DPI) and neutron reflection (NR), thus combining real-time dynamic monitoring with high interfacial structural resolution. Bovine serum albumin (BSA) was initially used as a model system to compare the surface coverage and thickness measurements of DPI and NR. The results show that DPI and NR provided similar surface coverage data but the measured thicknesses differed at BSA concentrations above 0.1 mg/ml. This discrepancy arose from the adoption of the uniform-layer model used by DPI for data analysis and the greater thickness sensitivity of NR. A model pregnancy immunoassay was built in steps on a silica surface so that the adsorption of each protein could be accurately monitored. Both DPI and NR provided evidence of BSA insertion into the gaps on the surface between the antibody molecules. This suggests that BSA adsorption is an excellent method to block the non-specific adsorption of target antigens to the immunoassay test surface. A magnetic tweezer system was designed and built in order to measure the specific antibody/antigen binding force. The antibodies and antigens were used to immuno-link magnetic beads to the experimental surface before the immuno-links were broken by increasing the attractive force between the magnetic tweezers and beads. The force per antibody/antigen immuno-link was estimated to lie between the values of 13.6 pN and 43.8 pN.Immuno-link detachment as a function of time was investigated. It was found that the immuno-link comprised both a strong and a weak interaction. The dissociation constant of the strong antibody/antigen interaction was found to equal 3E-4 /s and had an interaction length of 0.06 nm. The low population of beads bound by the second, weaker interaction meant that it was not possible to obtain accurate values of the dissociation constant and bond length of the second weaker interaction.

Les structures G-quadruplexes (G4) sont considérées comme des obstacles qui s’opposent à la progression du réplisome. Les séquences capables de former des G4 dans le génome humain se trouvent dans les régions d’ADN double brin au niveau des oncogènes et des proto-oncongènes et sur l’extrémité simple brin des télomères. La plupart des études biochimiques et biophysiques ont caractérisé les propriétés thermodynamiques des G4 en utilisant par exemple la température de fusion Tm pour déduire la thermodynamique de la formation/résolution du G4. Cependant, les expériences en solution donnent seulement une information indirecte concernant la dynamique du G4. Dans ce travail de thèse en molécule unique utilisant la technique des pinces magnétiques, nous avons pu caractériser la cinétique de la formation et résolution des G4s ainsi que la stabilité d’une structure G4 insérée dans une région d’ADN double brin : une situation qui ressemble aux G4 dans les promoteurs de gènes, où la séquence complémentaire est en compétition avec la formation de la structure de G4. Nous avons trouvé que le G4 télomérique a une très courte durée de vie (~20 s) et donc ce G4 se résout sans qu’une hélicase soit nécessaire. Au contraire, ce n’est pas le cas pour le G4 du c-MYC qui est très stable (~2h). Nous avons observé en temps réel la collision entre les hélicases et les polymérases et le G4 du c-MYC. Nous avons trouvé que l’hélicase Pif1 ouvre l’ADN puis résout le G4 après avoir effectué une pause et reprend l’ouverture de l’ADN, alors que l’hélicase RecQ et l’hélicase réplicative du bactériophage T4 ne peuvent pas le résoudre, mais peuvent le sauter. Nous avons aussi trouvé que la RPA ne peut pas résoudre le G4 du c-MYC. D’autre part, nous avons observé que la polyémrase du virus T4, la gp43, ainsi que la polymérase de T7, et la polymérase ε de la levure peuvent répliquer le G4 du c-MYC qui de façon étonnante ne constitue pas une barrière infranchissable. / G-quadruplex (G4) structures are considered as the major impediments for the replisome progression. The putative G4 forming sequences in the human genome are mostly located in the double-stranded DNA regions of oncogenes and proto-oncogenes and on the single-stranded overhangs of telomeres. Most of the biochemical and biophysical studies have characterized the G4 thermodynamics properties using melting temperature Tm as a proxy to infer thermodynamics of G4 folding/unfolding energetic. However, these thermodynamics properties give only indirect information about G4 dynamics. In this work, using single molecule magnetic tweezers technique, we first characterize the kinetics of folding and unfolding and thus the stability of a single G4 inserted in a dsDNA: a situation that mimics the G4s in promoters, where the complementary sequence competes with the G-rich structure. We find that the lifetime of telomeric G4 is short (~20 s) and thus that this G4 unfolds without the need of a helicase. This is not the case for the very stable c-MYC G4 (~2 hr). We observe in real time how helicases or polymerases behave as they collide with the c-MYC G4 on their track. We find that the Pif1 helicase unwinds dsDNA, resolves this G4 after pausing and resume unwinding, while RecQ helicase and the bacteriophage T4 replicative helicase do not resolve the G4 but may jump it. We also find that RPA does not unfold the c-MYC G4. Besides, we find that T4 bacteriophage gp43 polymerase, T7 polymerase and Yeast Pol ε can replicate the G4 which surprisingly does not appear as a major roadblock for them.

Táto práca sa zaoberá novým spôsobom manipulácie mikro a nano objektov, konkrétne tekutých AuGe ostrovčekov pomocou elektrónového zväzku. V prvej časti je diskutovaný mechanizmus manipulácie, je popísaný princíp a ďalej sú uvedené experimenty a simulácie potvrdzujúce tento princíp. Druhá časť práce sa zaoberá využitím uvedenej manipulácie k tvorenie mikro/nano štruktúr.

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