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Over the past two decades, vibrational sum-frequency generation (VSFG) has been applied as a versatile technique for probing the structure and dynamics of molecules at surfaces and interfaces. The excellent surface specificity of the SFG allows for probing different kinds of liquid interfaces with no or negligible contribution from adjacent and much deeper bulk phase. VSFG spectroscopy has provided evidence that the structure of the water at interfaces is different from the bulk. With the ultrafast pulses, VSFG can also be used as a probe of ultrafast vibrational dynamics at interfaces. However, apart from a few pioneering studies, the extension of VSFG into time domain has not been explored extensively. Here VSFG is used as a probe of ultrafast vibrational dynamics of water at silica interfaces. Silica is an excellent model system for the solid phase where one can systematically vary the surface charge via bulk pH adjustment. The extension of the surface electric field, the interfacial thickness and surface accumulation of ions at a charged silica surface were studied using IR pump-VSFG probe spectroscopy. A vibrational lifetime (T1) of about 250 fs, similar to bulk H2O, was observed for the O-H stretch of H2O/silica interface when the silica surface is negatively charged. At the neutral surface, where the thickness of interfacial water is smaller than at the charged surface, the vibrational lifetime of O-H stretch becomes more than two times longer (T1~ 600 fs) due to the decreased number of neighboring water molecules, probed by SFG. The fast T1 at negatively charged surface begins to slow down by screening of the penetration of surface electric field via adding salt which suggests the primary reason for similar vibrational dynamics of water at charged interface with bulk water is the penetration of electric field. By decoupling of OH of HDO in D2O, a frequency dependent vibrational lifetime is observed with faster T1 at the red compared to the blue side of the hydrogen bond spectral region. This correlates with the redshift of the SFG spectra with increasing charged surface and is consistent with a theoretical model that relates the vibrational lifetime to the strength of the hydrogen bond network. / Chemistry

The distinct structure and dynamics of interfacial water are due to a break in the extended hydrogen bonding network present in bulk water. At solid-aqueous interfaces, the presence of surface charge, which induces a static electric field, and the electrolytes, which are present in most naturally relevant systems, can additionally perturb the hydrogen bonding environment due to polarization. The interplay between the surface-charge-induced electric field and the ions in changing the structure of interfacial water has important consequences in the chemistry of processes ranging from protein-water interactions to mineral-water reactivity in oil recovery. Accessing information about the first few layers of water at buried interfaces is challenging. Vibrational sum-frequency generation (vSFG) spectroscopy is a powerful technique to study exclusively the interfacial region and is used here to investigate the role of interfacial solvent structure on surface reactivity. It is known that the rate of quartz dissolution increases on addition of salt at neat water pH. The reason for this enhancement was hypothesized to be a consequence of perturbations in interfacial water structure. The vSFG spectra, which is a measure of ordering in the interfacial water structure, shows an enhanced effect of salt (NaCl) at neat pH 6~8. The trend in the effect of salt on vSFG spectra versus the bulk pH is remarkably consistent with the enhancement of rate of quartz dissolution, providing the first experimental correlation between interfacial water structure and silica dissolution. If salt alters the structure of interfacial water, it must affect the vibrational energy transfer pathways of water, which is extremely fast in bulk water (~130 fs). Thus far, the role of ions on the vibrational dynamics of water at charged surfaces has been limited to the screening effects and reduction in the depth of the region that contributes to vSFG. Here, we measure the ultrafast vibrational relaxation of the O-H stretch of water at silica at different bulk pH, using time-resolved (TR-vSFG). The fast vibrational dynamics of water (~200 fs) observed at charged silica surfaces (pH 6 and pH 12), slows down (~600 fs) on addition of NaCl only at pH 6 and not at pH 12. On the other hand at pH 2 (neutral surface), the vibrational relaxation shows an acceleration at high ionic strengths (0.5 M NaCl). The TR-vSFG results suggest that there is a surface-charge dependence on the sensitivity of the interfacial dynamics to ions and that reduction in the probe depth of vSFG alone cannot explain the changes in the vibrational lifetime of interfacial O-H. This is further supported by the cation specific effects observed in the TR-vSFG of the silica/water interface. While the vibrational relaxation of O-H stretch slows on addition of all salts (LiCl, NaCl, RbCl, and CsCl), the degree of slowing down is sensitive to the cation identity. The vibrational lifetime of O-H stretch in the presence of different cations follows the order: Li+ < Na+ < Rb+, consistent with previous Hofmeister effect reported in vSFG spectroscopy as well as AFM measurements at silica/water interface. To provide molecular insight on the effect of surface charge density and ionic strength on the changes in interfacial water structure, Molecular Dynamics (MD) simulations were performed on water at different types of surfaces. It was shown that the properties of water near the interface, e.g., a net orientation and the depth to which this persists, depend on the degree of specific adsorption of the counter ions. Our vSFG results, along with the insights from MD simulations, highlight the importance of considering the role of ions on the solvent structure within the electric double layer region, beyond the screening effects predicted by classical electrochemical models. / Chemistry

Filmes de água cobrem a maior parte das superfícies em condições ambientes. O estudo dessas interfaces é crucial em biologia e em ciência dos materiais. No entanto, o completo entendimento da adsorção da água e de suas complexas redes de ligações de hidrogênio ainda não foi alcançado. Somente recentemente possuímos técnicas com a sensibilidade e seletividade para estudar estas superfícies até a última camada atômica. A espectroscopia por geração de soma de frequências (SFG) é uma técnica óptica não linear que fornece o espectro vibracional de moléculas em interfaces, sem contribuição do volume do material. A técnica SFG foi utilizada para estudar a estrutura interfacial das moléculas de água estrutural na face livre (010) do cristal natural gipsita (CaSO4 2H2O) e a adsorção de água na mesma à temperatura ambiente. Os espectros SFG na face livre (010), em atmosfera inerte, apresentaram um arranjo com anisotropia azimutal das moléculas de água estrutural com a presença de grupos OH ligados à superfície e grupos OH livre sem formar ligação de hidrogênio, apontando para fora da superfície. O arranjo anisotrópico das moléculas na face (010) é diferente daquele para as moléculas de água no volume do cristal. A adsorção de água foi estudada em equilíbrio com vapor de água em vários valores de umidade relativa. A água adsorvida na gipsita (010) também apresenta um arranjo anisotrópico, porém, diferentemente da água estrutural na superfície livre do cristal, esta apresenta um menor grau de ordenamento e suprime consideravelmente a presença de grupos OH livre. Os resultados experimentais são analisados em conjunto com simulações por dinâmica molecular ab initio realizadas por colaboradores. As simulações apresentaram boa concordância qualitativa e quantitativa com os resultados experimentais, permitindo fazer a atribuição dos espectros vibracionais experimentais, e fornecendo informações difíceis de se obter dos experimentos, como a distribuição orientacional das moléculas de água na interface e sua dinâmica de difusão espacial. / Water films cover most of surfaces under ambient conditions. The study of these interfaces is crucial in biology and materials science. However, a complete understanding of water adsorption and its complex hydrogen bonding networks has not yet been achieved. Only recently we have techniques with the sensitivity and selectivity to study these surfaces to the last atomic layer. Sum-frequency generation (SFG) is a non-linear optical technique that provides the vibrational spectrum of molecules at interfaces, without contribution from the bulk. This technique was used to study the interfacial structure of neat (010) face of Gypsum (CaSO4 2H2O) single crystals and water adsorption on the (010) face at room temperature. The SFG spectra for the neat Gypsum face (010), in inert atmosphere, presented azimuthally anisotropy arrangement of the structural water molecules with the presence of OH groups bound to the surface and free OH groups pointing out of the surface. The arrangement of water molecules on the face (010) is anisotropic but different from that of the water molecules in the bulk crystal. Water adsorption was studied in equilibrium with water vapor at several values of relative humidity. The adsorbed water also exhibited an anisotropic arrangement, however, unlike the structural water, it presents a lower ordering and the free OH groups are strongly suppressed. The experimental results are analyzed together with ab initio molecular dynamics simulations performed by collaborators. The simulations presented good qualitative and quantitative agreement with the experimental results, elucidating the assignment of the experimental vibrational spectra and yielding information that would be difficult to get from the experiments, such as the orientational distribution of interfacial water molecules and their spatial diffusion dynamics.

Neste trabalho, aplicamos técnicas de óptica não-linear de segunda ordem, em particular a Espectroscopia por Geração de Soma de Freqüências (SFG) e a Geração de Segundo Harmônico (SHG), para investigar a adsorção e o ordenamento molecular de filmes automontados de polieletrólitos variando-se os parâmetros que influenciam a adsorção (pH, força iônica, densidade de carga), além de investigar a estabilidade térmica e possíveis transições de fases nesses filmes multicamadas como função do pH das soluções e o do número de camadas. A espectroscopia SFG de filmes dos polieletrólitos poly(allylamine hydrochloride) (PAH) e poly(styrene sulfonate) (PSS) permitiu acompanhar a adsorção das camadas pelo monitoramento do campo elétrico na interface (substrato+filme adsorvido)/solução. As medidas de fase do sinal SFG confirmaram a supercompensação de cargas em todos os valores de pH estudados, exceto a pH 12, onde a adsorção foi possível devido a interações eletrostáticas locais. Os filmes secos mostraram grande ordenamento e homogeneidade quando a secagem era espontânea (sem a ação de jato de N2), independentemente do pH. Nestes filmes, observou-se pela primeira vez que as camadas adsorvidas podem alterar o ordenamento e a conformação das cadeias previamente adsorvidas. A espectroscopia SFG também apontou para a redução da densidade de carga e do ordenamento molecular quando a força iônica era aumentada, devido ao efeito de blindagem eletrostática. Os filmes tornaram-se mais inomogêneos e desordenados em virtude da compensação extrínseca. O efeito da força iônica foi o de reduzir a densidade de carga e assim o ordenamento molecular, mesmo se a secagem fosse espontânea. A técnica de SHG foi aplicada a filmes automontados de PAH e PS-119 para confirmar sua estabilidade térmica em função do pH e do número de camadas, além de verificar o ordenamento molecular antes e após o tratamento térmico. Os resultados mostraram que os filmes não são termicamente estáveis: o sinal é completamente destruído à temperatura de 150oC aproximadamente, ao contrário do que relata a literatura. As medidas SHG também confirmaram a isotropia dos filmes no plano das amostras, independente do pH ou do número de camadas. Comparando-se o sinal SHG antes e depois do aquecimento, comprovou-se que após o resfriamento lento, o sinal era restituído a quase o mesmo valor que antes, mostrando que o processo de desordem térmica é reversível. Entretanto, nenhuma transição de fase foi observada, pois a redução do sinal SHG foi lenta e gradual, sem nenhuma variação brusca que caracterizasse uma transição vítrea. Enfim, nossas medidas do sinal SHG em função do número de camadas também discordaram dos resultados da literatura, pois a susceptibilidade de segunda ordem não cresceu linearmente com o número de bicamadas. Isso indica que as moléculas não adsorvem com mesmo ordenamento em cada bicamada. Desse modo, podemos concluir que as técnicas SFG e SHG fornecem informação a nível microscópico que podem levar ao aprimoramento das aplicações dos filmes automontados, e que seriam difíceis de obter com técnicas tradicionais. / In this study, we have applied second-order nonlinear optical techniques, in particular Sum-Frequency Generation (SFG) and Second-Harmonic Generation (SHG), to investigate the adsorption and the molecular ordering of self-assembled polyelectrolyte films varying the parameters which are relevant to polyelectrolyte adsorption (pH, ionic strength, charge density), besides investigating the thermal stability and possible phase transistions in these multilayer films as function of pH of the solutions and of the number of layers. SFG spectroscopy of films fabricated with the polyelectrolytes PAH and PSS allowed us to monitor the adsorption of each layer by the electric field at the (substrate+adsorbed film)/solution interface. Phase-measurements of the SFG signal confirmed that charge supercompensation occurred at all pH values investigated, except at pH 12, where the adsorption was possible by local electrostatic interactions. Dry films have shown great order and homogeneity if the drying was spontaneous (without blow-drying with N2), independently of pH. In these films, it was observed for the first time that layer adsorption can modify the order and the conformation of previously adsorbed chains. SFG spectroscopy also pointed to the reduction of the charge density and of the molecular order if the ionic strength was increased, due to the electrostatic screening effect. The films were more inhomogeneous and disordered due to extrinsic charge compensation. The effect of the ionic strength was to reduce the charge density and the molecular order, even if the drying were slow (spontaneous). The SHG technique was applied to LBL films of PAH and PS-119 to confirm their thermal stability as a function of pH of the solutions and the number of layers, besides comparing the molecular order before and after the thermal treatment. The results have shown that the films are not thermally stable, with the SHG signal nearly vanished if the temperature of 150 oC is reached, in contrast of what is reported in the literature. SHG measurements have also confirmed that the films are isotropic in the plan of the samples, independent of pH or the number of layers. Comparing the SHG signal before and after heating, it was found that the SHG signal was considerably reduced at high temperatures, but after slow cooling it was recovered to almost the same value as before heating, showing that the thermal disorder is reversible. However, no phase transistion was observed, since the SHG signal reduction was slow and gradual, without any sudden change that would characterize a glass transition. At last, our SHG measurements as a function of the number of layers also disagreed with results in the literature, therefore the second order susceptibility did not grow linearly with the number of bilayers. This indicates that the molecules do not adsorb with same order in each bilayer. Therefore, we can conclude that SFG and SHG techniques provide information on the film arrangement at the microscopic level which could be difficult to get with traditional techniques and could also lead to the improvement of applications of LBL films.

Neste trabalho foi utilizada Espectroscopia Vibracional por Geração de Soma de Freqüências, uma técnica óptica não-linear que é sensível à conformação molecular em interfaces e superfícies, para caracterizar o ordenamento molecular de filmes poliméricos automontados de polieletrólitos durante todos os passos do processo de fabricação, tendo como modelo o par de polieletrólitos PAH (poli(cloreto de alilamina)) / PSS (poli(estireno sulfonato de sódio)). Os espectros SFG permitiram verificar que durante o mergulho (in situ) do substrato na solução de polieletrólitos, estes adsorvem, mas se encontram numa configuração desordenada. Observou-se também que a secagem dos filmes pela ação de jato de nitrogênio produz filmes menos homogêneos do que por secagem espontânea, e às vezes até destruindo completamente o ordenamento molecular. Além disso, verificou-se também que camadas de polieletrólitos adsorvidas influenciam o ordenamento das camadas previamente adsorvidas. Com base nos resultados, modelos para a representação das estruturas desses filmes de polieletrólitos in situ e ex situ foram propostos. / In this work, Sum-Frequency Vibrational Spectroscopy, a nonlinear optical technique that is sensitive to molecular conformation at interfaces and surfaces, was used to characterize the molecular ordering of self-assembled films during all steps of self-assembly, having as model poly(allylamine hydrochloride) (PAH) / poly(styrene sulfonate) (PSS) polyelectrolyte assemble. SFG spectra showed that during immersion (in situ) of substrate in polyelectrolytes solutions, adsorption occurs but the molecules are in a disordered configuration. It was observed that the films drying by nitrogen flow are more inhomogeneous than those dried by spontaneous water evaporation. In some cases, dried films by nitrogen flow are quite disordered. Furthermore, it was observed that polyelectrolytes layers affect the ordering of the previously adsorbed layers. Based on our results, models were proposed to represent the structure of polyelectrolytes films in both: in situ and ex situ.

Neste trabalho, aplicamos técnicas de óptica não-linear de segunda ordem, em particular a Espectroscopia por Geração de Soma de Freqüências (SFG) e a Geração de Segundo Harmônico (SHG), para investigar a adsorção e o ordenamento molecular de filmes automontados de polieletrólitos variando-se os parâmetros que influenciam a adsorção (pH, força iônica, densidade de carga), além de investigar a estabilidade térmica e possíveis transições de fases nesses filmes multicamadas como função do pH das soluções e o do número de camadas. A espectroscopia SFG de filmes dos polieletrólitos poly(allylamine hydrochloride) (PAH) e poly(styrene sulfonate) (PSS) permitiu acompanhar a adsorção das camadas pelo monitoramento do campo elétrico na interface (substrato+filme adsorvido)/solução. As medidas de fase do sinal SFG confirmaram a supercompensação de cargas em todos os valores de pH estudados, exceto a pH 12, onde a adsorção foi possível devido a interações eletrostáticas locais. Os filmes secos mostraram grande ordenamento e homogeneidade quando a secagem era espontânea (sem a ação de jato de N2), independentemente do pH. Nestes filmes, observou-se pela primeira vez que as camadas adsorvidas podem alterar o ordenamento e a conformação das cadeias previamente adsorvidas. A espectroscopia SFG também apontou para a redução da densidade de carga e do ordenamento molecular quando a força iônica era aumentada, devido ao efeito de blindagem eletrostática. Os filmes tornaram-se mais inomogêneos e desordenados em virtude da compensação extrínseca. O efeito da força iônica foi o de reduzir a densidade de carga e assim o ordenamento molecular, mesmo se a secagem fosse espontânea. A técnica de SHG foi aplicada a filmes automontados de PAH e PS-119 para confirmar sua estabilidade térmica em função do pH e do número de camadas, além de verificar o ordenamento molecular antes e após o tratamento térmico. Os resultados mostraram que os filmes não são termicamente estáveis: o sinal é completamente destruído à temperatura de 150oC aproximadamente, ao contrário do que relata a literatura. As medidas SHG também confirmaram a isotropia dos filmes no plano das amostras, independente do pH ou do número de camadas. Comparando-se o sinal SHG antes e depois do aquecimento, comprovou-se que após o resfriamento lento, o sinal era restituído a quase o mesmo valor que antes, mostrando que o processo de desordem térmica é reversível. Entretanto, nenhuma transição de fase foi observada, pois a redução do sinal SHG foi lenta e gradual, sem nenhuma variação brusca que caracterizasse uma transição vítrea. Enfim, nossas medidas do sinal SHG em função do número de camadas também discordaram dos resultados da literatura, pois a susceptibilidade de segunda ordem não cresceu linearmente com o número de bicamadas. Isso indica que as moléculas não adsorvem com mesmo ordenamento em cada bicamada. Desse modo, podemos concluir que as técnicas SFG e SHG fornecem informação a nível microscópico que podem levar ao aprimoramento das aplicações dos filmes automontados, e que seriam difíceis de obter com técnicas tradicionais. / In this study, we have applied second-order nonlinear optical techniques, in particular Sum-Frequency Generation (SFG) and Second-Harmonic Generation (SHG), to investigate the adsorption and the molecular ordering of self-assembled polyelectrolyte films varying the parameters which are relevant to polyelectrolyte adsorption (pH, ionic strength, charge density), besides investigating the thermal stability and possible phase transistions in these multilayer films as function of pH of the solutions and of the number of layers. SFG spectroscopy of films fabricated with the polyelectrolytes PAH and PSS allowed us to monitor the adsorption of each layer by the electric field at the (substrate+adsorbed film)/solution interface. Phase-measurements of the SFG signal confirmed that charge supercompensation occurred at all pH values investigated, except at pH 12, where the adsorption was possible by local electrostatic interactions. Dry films have shown great order and homogeneity if the drying was spontaneous (without blow-drying with N2), independently of pH. In these films, it was observed for the first time that layer adsorption can modify the order and the conformation of previously adsorbed chains. SFG spectroscopy also pointed to the reduction of the charge density and of the molecular order if the ionic strength was increased, due to the electrostatic screening effect. The films were more inhomogeneous and disordered due to extrinsic charge compensation. The effect of the ionic strength was to reduce the charge density and the molecular order, even if the drying were slow (spontaneous). The SHG technique was applied to LBL films of PAH and PS-119 to confirm their thermal stability as a function of pH of the solutions and the number of layers, besides comparing the molecular order before and after the thermal treatment. The results have shown that the films are not thermally stable, with the SHG signal nearly vanished if the temperature of 150 oC is reached, in contrast of what is reported in the literature. SHG measurements have also confirmed that the films are isotropic in the plan of the samples, independent of pH or the number of layers. Comparing the SHG signal before and after heating, it was found that the SHG signal was considerably reduced at high temperatures, but after slow cooling it was recovered to almost the same value as before heating, showing that the thermal disorder is reversible. However, no phase transistion was observed, since the SHG signal reduction was slow and gradual, without any sudden change that would characterize a glass transition. At last, our SHG measurements as a function of the number of layers also disagreed with results in the literature, therefore the second order susceptibility did not grow linearly with the number of bilayers. This indicates that the molecules do not adsorb with same order in each bilayer. Therefore, we can conclude that SFG and SHG techniques provide information on the film arrangement at the microscopic level which could be difficult to get with traditional techniques and could also lead to the improvement of applications of LBL films.

The surface-specific technique of vibrational sum frequency spectroscopy (VSFS) can provide vibrational information about chemical bonds at surfaces and interfaces. Two photons, of visible and infrared frequency, are spatially and temporally overlapped at a surface/interface to produce a photon at the sum frequency (SF) of the two input photons. As well as this process only being allowed in non-centrosymmetric media (i.e. VSFS is surface/interface specific), the SF process is enhanced when the IR beam is resonant with vibrational resonances. Broadband VSFS has been used in this project to study surfaces of two distinct classes of materials, namely graphene and polymers. Firstly, broadband VSFS was used to investigate the heating polymeric thin films using a home-built heated sample cell. The cell was tested using self-assembled monolayers (SAMs) of 1-octadecanethiol (ODT) grown on gold substrates. It was subsequently used to investigate thin films of poly(methyl methacrylate) (PMMA) of four different thicknesses and two different molecular weights that were spin-coated onto gold substrates. It was shown that the monolayers of ODT become disordered upon heating and solidified to incorporate the disorder introduced by the heating process. The PMMA films were also shown to become more disordered as a function of temperature. Secondly, broadband VSFS was used to investigate modified graphene, motivated by the fact that modifications to pristine graphene, be it intentional (i.e. functionalisation) or unintentional (i.e. contamination), cause the properties of graphene to change. This project focused on studying hydrogenated graphene, N-methylbenzamide functionalised graphene and contamination on commercial graphene. A method for calculating the number of hydrogen atoms in a hydrogen island was developed. VSF spectra of CH stretches in N-methylbenzamide functionalised graphene were obtained. Residues on commercially bought graphene were detected using VSFS and RAIRS. These residues were assigned to PMMA that remained on the CVD graphene by the process of transferring the CVD graphene from the copper foil on which it was grown onto the gold substrates.