Abstract This thesis deals with infrared spectroscopy investigations on the linear DCCI molecule. The high resolution spectra between 200–5200 cm-1 were measured with the Fourier transform spectrometer at the University of Oulu. The spectra were analyzed taking into account various types of resonances between rovibrational energy levels. As a result, a set of molecular constants and resonance parameters describing the rotational and vibrational energy states of the molecule were obtained. From the resulting molecular constants, together with previous results from literature for HCCI, the structure of monoiodoacetylene was calculated. In addition, eight harmonic force constants with estimated uncertainties for monoiodoacetylene were determined.

Neste trabalho realizou-se um estudo espectroscópico vibracional do dissulfeto de carbono, CS2, puro e em misturas binárias com diferentes solventes moleculares, a fim de investigar as interações soluto/soluto e soluto/solvente. Os solventes utilizados para esse estudo foram diclorometano (CH2Cl2), clorofórmio (CHCl3), clorofórmio deuterado (CDCl3), benzeno (C6H6) e tetracloreto de carbono (CCl4); e as técnicas utilizadas foram as espectroscopias Raman e infravermelho (IV). A análise das bandas Raman do CS2 que formam o dubleto de Fermi (v1-2v2) permite determinar uma série de valores empíricos, chamados de parâmetros de ressonância de Fermi, dentre os quais, o coeficiente de acoplamento de Fermi (W) foi o mais utilizado neste trabalho. Os diferentes valores de W nos diferentes meios são consequência das forças das interações intermoleculares existentes entre CS2/CS2 e CS2/solvente. Os experimentos demonstraram que os valores de W em todas as misturas binárias investigadas aumentam à medida que a fração molar de CS2 diminui. Isto sugere que quando o CS2 é solvatado por diferentes moléculas, há um aumento da anarmonicidade, dependendo do tipo de interação. A análise da banda atribuída ao modo de deformação angular do CS2, v2, realizada a partir dos espectros no infravermelho sugere que em misturas binárias existem dois regimes de solvatação na solução, uma referente às interações CS2/ CS2, onde as moléculas de CS2 estão preferencialmente solvatadas por moléculas de CS2 e outro regime de solvatação referente às interações CS2/solvente, onde CS2 está solvatado por moléculas do solvente em questão. / In this work has performed a vibrational spectroscopic investigation of carbon disulphide, CS2, neat and in binary mixtures with different molecular solvents, aiming at understanding the solute/solute and solute/solvent interactions. The solvents considered for this study were dichloromethane (CH2Cl2), chloroform (CHCl3), deuterated chloroform (CDCl3), benzene (C6H6) and carbon tetrachloride (CCl4); and the techniques used were Raman and infrared (IR) spectroscopies. The analysis of the Raman bands that compose the Fermi doublet (v1-2v2) allows the determination of a series of empirical values, including the coefficient of Fermi coupling (W), used along this work. The different values of W within the different solvents are consequence of the intermolecular forces between CS2/CS2 and CS2/solvent. The experimental data showed that the W values in all investigated binary mixtures increase as the CS2 molar fraction decreases. It suggests that when CS2 is solvated by different molecules, there is an increase of the anarmonicity, depending on the type of the interaction. The analysis of the band assigned to the CS2 bending mode, v2, performed from infrared spectra, suggests that in the binary mixtures there are two solvation regimes in solution, one related to the CS2/CS2 interactions, where the CS2 molecule is preferentially solvated by CS2 molecules, and one where the CS2 is solvated by the respective solvent molecules.

Neste trabalho realizou-se um estudo espectroscópico vibracional do dissulfeto de carbono, CS2, puro e em misturas binárias com diferentes solventes moleculares, a fim de investigar as interações soluto/soluto e soluto/solvente. Os solventes utilizados para esse estudo foram diclorometano (CH2Cl2), clorofórmio (CHCl3), clorofórmio deuterado (CDCl3), benzeno (C6H6) e tetracloreto de carbono (CCl4); e as técnicas utilizadas foram as espectroscopias Raman e infravermelho (IV). A análise das bandas Raman do CS2 que formam o dubleto de Fermi (v1-2v2) permite determinar uma série de valores empíricos, chamados de parâmetros de ressonância de Fermi, dentre os quais, o coeficiente de acoplamento de Fermi (W) foi o mais utilizado neste trabalho. Os diferentes valores de W nos diferentes meios são consequência das forças das interações intermoleculares existentes entre CS2/CS2 e CS2/solvente. Os experimentos demonstraram que os valores de W em todas as misturas binárias investigadas aumentam à medida que a fração molar de CS2 diminui. Isto sugere que quando o CS2 é solvatado por diferentes moléculas, há um aumento da anarmonicidade, dependendo do tipo de interação. A análise da banda atribuída ao modo de deformação angular do CS2, v2, realizada a partir dos espectros no infravermelho sugere que em misturas binárias existem dois regimes de solvatação na solução, uma referente às interações CS2/ CS2, onde as moléculas de CS2 estão preferencialmente solvatadas por moléculas de CS2 e outro regime de solvatação referente às interações CS2/solvente, onde CS2 está solvatado por moléculas do solvente em questão. / In this work has performed a vibrational spectroscopic investigation of carbon disulphide, CS2, neat and in binary mixtures with different molecular solvents, aiming at understanding the solute/solute and solute/solvent interactions. The solvents considered for this study were dichloromethane (CH2Cl2), chloroform (CHCl3), deuterated chloroform (CDCl3), benzene (C6H6) and carbon tetrachloride (CCl4); and the techniques used were Raman and infrared (IR) spectroscopies. The analysis of the Raman bands that compose the Fermi doublet (v1-2v2) allows the determination of a series of empirical values, including the coefficient of Fermi coupling (W), used along this work. The different values of W within the different solvents are consequence of the intermolecular forces between CS2/CS2 and CS2/solvent. The experimental data showed that the W values in all investigated binary mixtures increase as the CS2 molar fraction decreases. It suggests that when CS2 is solvated by different molecules, there is an increase of the anarmonicity, depending on the type of the interaction. The analysis of the band assigned to the CS2 bending mode, v2, performed from infrared spectra, suggests that in the binary mixtures there are two solvation regimes in solution, one related to the CS2/CS2 interactions, where the CS2 molecule is preferentially solvated by CS2 molecules, and one where the CS2 is solvated by the respective solvent molecules.

The work carried out during this thesis focuses on the quantum dynamics of the diffusion of hydrogen atoms on a surface of palladium (111). The study of the 3D system allowed us to detail the infrared spectrum of H/Pd (111), showing the existence of different adsorption sites on which localized states exist that are strongly coupled (Fermi resonance). This phenomenon governs the diffusion of hydrogen atoms in an ultra-fast time scale (fs).The study of the (6D) H2/Pd(111) system has shown that the transitions observed are in fact transition bands between several quasi-degenerate adsorption states. The agreement between the calculated and measured values is significantly less good than that between the data calculated for the 3D system and the measured data. Does adsorbed hydrogen on palladium exist in the form of a weakly bound H2 molecule? This thesis has provided some answers to this question, which remains open, hovewer, to some extent.

In this thesis, I have investigated gas phase infrared spectroscopy of environmentally as well as astrophysical important large organic molecules such as naphthalene, methy-lated naphthalene, fluorine, methyalted fluorine etc. which are commonly known as polycyclic aromatic hydrocarbons (PAHs). Depending upon the molecular weight these organic molecules can exist both in gaseous as well as in the particulate state at room temperature hence they are the major environmental pollutants. They are also responsible for the unidentified infrared emission bands in the interstellar medium. Chapter 1 provides a brief introduction to my thesis work. A detailed literature survey on the importance, abundance of the PAHs in the environment as well as various spectroscopic techniques useful for identifying the PAHs has been done. Since the objective of my thesis work is to assign the observed fundamental infrared bands of large organic molecules with the help of high level quantum mechanical calculations, a brief introduction to the various high level quantum mechanical techniques that I have used in assigning the bands have been described in this chapter. In Chapter 2 I have presented the experimental and the theoretical methodologies in details. The chapter begins with a detailed description of the experimental procedure used for recording the infrared spectrum of these molecules followed by the theoretical methodologies used for the assignment of the observed infrared bands as well as for identifying the Fermi resonances. In Chapters 3 and 4, of this thesis I have recorded infrared spectrum of 1-and 2-methylnaphthalene (1-and 2-MN), fluorine (FL), 1-methylfluorene (1-MFL) and 1,8-dimethylfluorene (1,8-DMF) in the gas phase. The observed bands were assigned with the help of scaled harmonic frequency, scaled quantum mechanical harmonic force field (SQMFF) and enharmonic frequency calculations. The first two methods are based on the harmonic approximation, whereas the enharmonic frequency calculation is based on the standard second order perturbation theory. All these calculations gave me a partial fit to the fundamental bands in both aromatic and aliphatic C-H stretching as well as in the non C-H stretching region. At the end of both the chapters an error analysis in fitting the spectrum from all the three different calculations have been presented. Evidently the non linear least square fitting method employed in SQMFF calculation gives much better agreement between the experiment and theory than the other two methods. It has been observed in the experimental spectrum of methylated naphthalene that the band structure near the C-H stretch around 3000 cm−1 is very complicated and many bands and shoulders remain unassigned by the methods described in Chapters 3 and 4. Fermi resonance is one of the potential reason for the complicated band structure in this region. In Chapter 5, I have taken naphthalene and have investigated the Fermi resonance around the C-H stretching region using an effective vibrational hamiltonian (EVH) approach. In this method I have constructed an EVH consisting of 8 C-H stretches and 8 H-C-C in-plane bend overtones and 28 H-C-C in-plane bend combination modes as the basis. Both type 1 (stretch overtone) and type 2 (stretch combination) Fermi resonances were investigated. Calculated frequencies belonging to B1u and B2u irreducible representation were compared with the observed bands. Many bands and shoulders have been assigned as the overtone and combination modes of low frequency H-C-C bend motion obtained from the EVH approach. How-ever some bands remain unassigned in this method. This is perhaps due to the neglect of the carbon framework motion in the construction of the EVH. To improve upon the results obtained from the EVH formalism I included the carbon frame degrees of freedom and have carried out a full variation treatment in curvilinear coordinates. I have considered the 8 C-H stretches and 8 H-C-C in-plane bends of naphthalene as local mode oscillators and 17 coordinates belonging to the carbon framework motion as curvilinear normal mode oscillators. A quartic hamiltonian in a mixed local mode -normal mode basis was constructed including up to three body terms in both kinetic and potential energy part. The hamiltonian was subsequently recast into the ladder operator form and diagonal zed in a symmetry adapted basis with polyad constraints. Frequencies so obtained were compared to the experiment All these findings have been presented in Chapter 6 of this thesis. The concluding remark of the thesis and the future direction is presented in Chapter 7

Die Energierelaxationsdynamik und strukturelle Dynamik der DNA spielen eine entscheidende Rolle für das Verständnis der photochemischen Eigenschaften und biologischen Funktion von DNA. Die schnellsten Prozesse geschehen dabei auf Zeitskalen im Femto- bis Pikosekundenbereich und können durch zeitaufgelöste (ultraschnelle) Messungen an molekularen Schwingungsanregungen in Echtzeit beobachtet werden. In dieser Arbeit werden NH-Streck Schwingungsmoden der Nukleobasen sowie OH-Streckmoden der Hydrathülle mittels linearer infrarot (IR) Spektroskopie sowie ultraschneller Pump-Probe und zweidimensionaler IR Spektroskopie untersucht. Messungen an monomerartigen Nukleobasen, wasserstoffverbrückten Nukleobasenpaaren und kurzen DNA Fragmenten in Doppelhelixstruktur ermöglichen es, die Effekte der verschiedenen Wasserstoffbrücken und Schwingungskopplungen separat voneinander zu untersuchen. Im Zusammenspiel mit exzitonischen und quantenchemischen Rechnungen werden so weitreichende Einsichten in die spektroskopischen Eigenschaften und die Relaxationsdynamik von Schwingungsanregungen in DNA gewonnen. Es wird u.a. gezeigt, dass Wasserstoffbrücken zwischen Nukleobasen eine Lebensdauer größer 1 ps besitzen und eine beschleunigte Energierelaxation durch Fermiresonanzen mit niederfrequenten Schwingungsmoden des Fingerprintbereichs bewirken. Die DNA-Hydrathülle zeigt eine ultraschnelle strukturelle Dynamik unabhängig von der Basenpaarzusammensetzung und fungiert als effiziente Wärmesenke für hochfrequente Schwingungsanregungen. / Energy relaxation and structural dynamics in DNA play a crucial role for the understanding of the photochemical properties and biological function of DNA. The fastest of such processes occur on the femto- to picosecond time scale and can be followed in real time through time-resolved (ultrafast) measurements on molecular vibrations. In this work, NH stretching excitations of nucleobases and OH stretching modes of the hydration shell are analyzed through linear infrared (IR) spectroscopy as well as ultrafast pump-probe and two-dimensional IR spectroscopy. Measurements on monomeric nucleobases, hydrogen-bonded nucleobase pairs, and short DNA fragments in double helix structure allow one to examine the effects of the different hydrogen bonds and vibrational couplings separately from each other. The combination with excitonic and quantum chemical calculations provides profound new insights into the spectroscopic properties and relaxation dynamics of vibrational excitations in DNA. This work shows that hydrogen bonds between nucleobases have a lifetime greater than 1 ps and lead to an accelerated dissipation of energy due to Fermi resonances with vibrational modes in the fingerprint range. The hydration shell of DNA exhibits ultrafast structural dynamics independent of the base pair composition and serves as an efficient heat sink for high-energy vibrational excitations.

A presente tese trata da análise conformacional e estudo das interações eletrônicas de algumas 2-(fenilselanil)-2-(metoxi)-4\'-substituídas-acetofenonas (série I) e das 2-(4-substituídasfenilsulfanil)-2-(metoxi)-4\'-substituídas-acetofenonas (série II) contendo grupos doadores, hidrogênio e atraentes de elétrons na posição para dos anéis fenacílico [4\'-Y-PhC(O)] e fenilsulfanílico (S-Ph-4-X). Através da resolução das bandas de νCO, foi constatada a ocorrência de isomerismo conformacional nos solventes de constante dielétrica crescente (n-C6H14, CCl4, CHCl3, CH2Cl2, CH3CN) em ambas as séries. Cinco compostos da série II apresentaram ressonância de Fermi (RF) no infravermelho e precisaram ser deuterados. Os dados espectroscópicos são concordantes tanto com os resultados dos cálculos de otimização e frequência em fase gasosa quanto com a simulação do efeito do solvente (PCM), no nível de teoria B3LYP/6-31+G(d,p). Em ambas as séries, foram encontradas três conformações estáveis c1, c2 e c3, sendo que c2 é significativamente mais estável que c1 e c3. O confôrmero c1 possui o oxigênio metoxílico e o carbonílico em sinperiplanar enquanto os grupos -SePh/- SPh estão em anticlinal. Os confôrmeros c2 e c3 possuem o hidrogênio metínico em sinperiplanar com a carbonila enquanto os grupos -OMe e -SePh/-SPh estão na anticlinal. O confôrmero c1 pode ser atribuído ao componente de banda (IR) de maior frequência νCO. Da mesma forma, c2 e c3 são o componente de frequência intermediária e de menor frequência, respectivamente, na série I enquanto que na série II eles coalescem em apenas um componente de menor frequência. Os cálculos de PCM mimetizam os dados espectroscópicos, i.e. é possível constatar a inversão populacional entre c1 e c2, conforme a polaridade do solvente aumenta. Através do cálculo de frequências anarmônicas e construção da PED, foram encontrados dois modos vibracionais que combinados interagem com νCO originando a RF (série II). Um modo é de alta frequência e envolve uma porcentagem considerável de &#948C-H(metínico), o outro modo é esqueletal. A análise das interações orbitalares (NBO) mostrou que os confôrmeros c1 e c2 são estabilizados pela transferência de cargas entre LpO5→σ*CS/Se (ca. 18 kcal mol-1) enquanto c3 é estabilizado pela interação menos intensa LpO5→σ*C-C (ca. 9,5 kcal mol-1). As interações eletrônicas foram investigadas a partir dos contatos interatômicoscurtos com apoio das cargas atômicas parciais. Apesar de c1 e c2 apresentarem praticamente a mesma estabilidade em termos de interações orbitalares, o primeiro é fortemente desestabilizado pela repulsão eletrostática entre os átomos O&#948-CO...O&#948-OMe negativamente carregados separados por uma distância menor que a soma dos raios de van der Waals. Este contato curto entre os dipolos C&#948+=O&#948- e C&#948+−O&#948- é responsável pela maior frequência de νCO de c1 frente c2 e c3. A maior estabilidade de c1 nos solventes mais polares, porém, deve-se à melhor solvatação local destes dipolos. As análises dos monocristais (raios-X) indicou que os compostos assumem, no estado sólido, a conformação menos estável c1, obtida em fase gasosa. Não foram encontradas diferenças significativas no que se refere aos substituintes Y e X. Conclui-se que a estabilidade global das conformações é determinada pelo balanço energético entre as interações orbitalares e eletrostáticas, nas duas séries estudadas. / This thesis reports the conformational analysis and the electronic interactions study of some 2-(phenylselanyl)-2-(methoxy)-4\'-substituted-acetophenones (series I) and 2-(4-substitutedphenylsulphanyl)-2-(methoxy)-4\'-substituted-acetophenones (series II) bearing electron donating, hydrogen and electron attracting substituents in the para position of the phenacyl [4\'-Y-PhC(O)] and phenylsulphanyl (S-Ph-4-X). The occurrence of conformational isomerism in crescent dielectric constant solvents (n-C6H14, CCl4, CHCl3, CH2Cl2, CH3CN) in the two series was studied through the νCO infrared band decomposition. From the series II compounds, five presented Fermi resonance (FR) and had to be deuterated. The spectroscopic data are in line with theoretical calculations results for optimization and frequency in gas phase as well as for solvent effect simulation (PCM), both in B3LYP/6-31+G(d,p) level. Three stable conformers (c1, c2 and c3) were found for both series being the c2 significantly more stable than c1 and c3. Particularly in the c1 conformer, the methoxyl and the carbonyl oxygens are in sinperiplanar orientation while the -SePh/-SPh groups are in anticlinal. In the c2 and c3 conformers the methyne hydrogen assume a sinperiplanar geometry with respect to the carbonyl whereas both -OMe and -SePh/-SPh are in anticlinal. The c1 conformer can be ascribed to the highest frequency νCO band component (IR). So, c2 and c3 ones can be ascribed to the medium and the lowest frequency νCO component, respectively, in the series I whereas in the series II they come together (coalescence) in one single band component. The PCM calculations are in good agreement with spectroscopic data i.e. it is possible to observe a populational inversion between c1 and c2 conformers as the solvent polarity increases. The anharmonic frequencies and PED theoretical treatment revealed that the combination of two vibrational modes interact with the νCO giving rise to the FR (series II): the high frequency one involves a considerable δC-H(methyne) percentage; whilst the other is skeletal. The orbital interactions analysis (NBO) showed that the c1 and c2 conformers are mainly stabilized by charge transfer LpO5→σ*CS/Se (ca. 18 kcal mol-1) while c3 is stabilized by the less intense interaction LpO5→σ*C-C (ca. 9,5 kcal mol-1). The electronic interactions were investigated by means of interatomic short contacts supported by partial atomic charges calculations. In contrast with the almost similar orbital interactions stability of c1 and c2, the former is strongly destabilized by the electrostatic repulsion between Oδ-CO...Oδ-OMe atoms which are negatively charged separated by a distance shorter than the van der Waals radius sum. This short contact between Cδ+=Oδ- and Cδ+−Oδ- dipoles is responsible for the highest νCO frequency of c1 compared to c2 and c3. In the other hand, the greater stabilization of c1 in the more polar solvents is due to the better solvation of those local dipoles. Last, but not least, the X-ray analysis showed that the compounds in the solid state assume the less stable conformation c1, obtained in gas phase. No significative differences were found in terms of the Y and X substituents. It is suggestive that an energetic balance between orbital and electrostatic interactions determines the global stability of conformations in both studied series.

A presente tese trata da análise conformacional e estudo das interações eletrônicas de algumas 2-(fenilselanil)-2-(metoxi)-4\'-substituídas-acetofenonas (série I) e das 2-(4-substituídasfenilsulfanil)-2-(metoxi)-4\'-substituídas-acetofenonas (série II) contendo grupos doadores, hidrogênio e atraentes de elétrons na posição para dos anéis fenacílico [4\'-Y-PhC(O)] e fenilsulfanílico (S-Ph-4-X). Através da resolução das bandas de νCO, foi constatada a ocorrência de isomerismo conformacional nos solventes de constante dielétrica crescente (n-C6H14, CCl4, CHCl3, CH2Cl2, CH3CN) em ambas as séries. Cinco compostos da série II apresentaram ressonância de Fermi (RF) no infravermelho e precisaram ser deuterados. Os dados espectroscópicos são concordantes tanto com os resultados dos cálculos de otimização e frequência em fase gasosa quanto com a simulação do efeito do solvente (PCM), no nível de teoria B3LYP/6-31+G(d,p). Em ambas as séries, foram encontradas três conformações estáveis c1, c2 e c3, sendo que c2 é significativamente mais estável que c1 e c3. O confôrmero c1 possui o oxigênio metoxílico e o carbonílico em sinperiplanar enquanto os grupos -SePh/- SPh estão em anticlinal. Os confôrmeros c2 e c3 possuem o hidrogênio metínico em sinperiplanar com a carbonila enquanto os grupos -OMe e -SePh/-SPh estão na anticlinal. O confôrmero c1 pode ser atribuído ao componente de banda (IR) de maior frequência νCO. Da mesma forma, c2 e c3 são o componente de frequência intermediária e de menor frequência, respectivamente, na série I enquanto que na série II eles coalescem em apenas um componente de menor frequência. Os cálculos de PCM mimetizam os dados espectroscópicos, i.e. é possível constatar a inversão populacional entre c1 e c2, conforme a polaridade do solvente aumenta. Através do cálculo de frequências anarmônicas e construção da PED, foram encontrados dois modos vibracionais que combinados interagem com νCO originando a RF (série II). Um modo é de alta frequência e envolve uma porcentagem considerável de &#948C-H(metínico), o outro modo é esqueletal. A análise das interações orbitalares (NBO) mostrou que os confôrmeros c1 e c2 são estabilizados pela transferência de cargas entre LpO5→σ*CS/Se (ca. 18 kcal mol-1) enquanto c3 é estabilizado pela interação menos intensa LpO5→σ*C-C (ca. 9,5 kcal mol-1). As interações eletrônicas foram investigadas a partir dos contatos interatômicoscurtos com apoio das cargas atômicas parciais. Apesar de c1 e c2 apresentarem praticamente a mesma estabilidade em termos de interações orbitalares, o primeiro é fortemente desestabilizado pela repulsão eletrostática entre os átomos O&#948-CO...O&#948-OMe negativamente carregados separados por uma distância menor que a soma dos raios de van der Waals. Este contato curto entre os dipolos C&#948+=O&#948- e C&#948+−O&#948- é responsável pela maior frequência de νCO de c1 frente c2 e c3. A maior estabilidade de c1 nos solventes mais polares, porém, deve-se à melhor solvatação local destes dipolos. As análises dos monocristais (raios-X) indicou que os compostos assumem, no estado sólido, a conformação menos estável c1, obtida em fase gasosa. Não foram encontradas diferenças significativas no que se refere aos substituintes Y e X. Conclui-se que a estabilidade global das conformações é determinada pelo balanço energético entre as interações orbitalares e eletrostáticas, nas duas séries estudadas. / This thesis reports the conformational analysis and the electronic interactions study of some 2-(phenylselanyl)-2-(methoxy)-4\'-substituted-acetophenones (series I) and 2-(4-substitutedphenylsulphanyl)-2-(methoxy)-4\'-substituted-acetophenones (series II) bearing electron donating, hydrogen and electron attracting substituents in the para position of the phenacyl [4\'-Y-PhC(O)] and phenylsulphanyl (S-Ph-4-X). The occurrence of conformational isomerism in crescent dielectric constant solvents (n-C6H14, CCl4, CHCl3, CH2Cl2, CH3CN) in the two series was studied through the νCO infrared band decomposition. From the series II compounds, five presented Fermi resonance (FR) and had to be deuterated. The spectroscopic data are in line with theoretical calculations results for optimization and frequency in gas phase as well as for solvent effect simulation (PCM), both in B3LYP/6-31+G(d,p) level. Three stable conformers (c1, c2 and c3) were found for both series being the c2 significantly more stable than c1 and c3. Particularly in the c1 conformer, the methoxyl and the carbonyl oxygens are in sinperiplanar orientation while the -SePh/-SPh groups are in anticlinal. In the c2 and c3 conformers the methyne hydrogen assume a sinperiplanar geometry with respect to the carbonyl whereas both -OMe and -SePh/-SPh are in anticlinal. The c1 conformer can be ascribed to the highest frequency νCO band component (IR). So, c2 and c3 ones can be ascribed to the medium and the lowest frequency νCO component, respectively, in the series I whereas in the series II they come together (coalescence) in one single band component. The PCM calculations are in good agreement with spectroscopic data i.e. it is possible to observe a populational inversion between c1 and c2 conformers as the solvent polarity increases. The anharmonic frequencies and PED theoretical treatment revealed that the combination of two vibrational modes interact with the νCO giving rise to the FR (series II): the high frequency one involves a considerable δC-H(methyne) percentage; whilst the other is skeletal. The orbital interactions analysis (NBO) showed that the c1 and c2 conformers are mainly stabilized by charge transfer LpO5→σ*CS/Se (ca. 18 kcal mol-1) while c3 is stabilized by the less intense interaction LpO5→σ*C-C (ca. 9,5 kcal mol-1). The electronic interactions were investigated by means of interatomic short contacts supported by partial atomic charges calculations. In contrast with the almost similar orbital interactions stability of c1 and c2, the former is strongly destabilized by the electrostatic repulsion between Oδ-CO...Oδ-OMe atoms which are negatively charged separated by a distance shorter than the van der Waals radius sum. This short contact between Cδ+=Oδ- and Cδ+−Oδ- dipoles is responsible for the highest νCO frequency of c1 compared to c2 and c3. In the other hand, the greater stabilization of c1 in the more polar solvents is due to the better solvation of those local dipoles. Last, but not least, the X-ray analysis showed that the compounds in the solid state assume the less stable conformation c1, obtained in gas phase. No significative differences were found in terms of the Y and X substituents. It is suggestive that an energetic balance between orbital and electrostatic interactions determines the global stability of conformations in both studied series.

Les travaux réalisés au cours de cette thèse portent sur la dynamique quantique de diffusion d'atomes d'hydrogène sur une surface de palladium (111). L'étude du système 3D a permis de détailler le spectre infrarouge de H/Pd(111) en mettant en évidence l'existence sur différents sites d'adsorption d'états localisés fortement couplés (résonance de Fermi). Ce phénomène gouverne la diffusion des atomes d'hydrogène sur une échelle de temps ultra-rapide (fs).L'étude du système 6D (H2/Pd(111)) a montré que les transitions observées sont, en fait, des bandes de transition entre plusieurs états d'adsorption quasi-dégénérés. L'accord entre les valeurs calculées et mesurées est, par contre, significativement moins bon qu'entre celles calculées pour le système 3D et les données mesurées. Est-ce que l'hydrogène adsorbé sur le palladium existe sous la forme d'une molécule diatomique faiblement lié? Cette thèse a fourni certains éléments de réponse à cette question, qui reste cependant encore ouverte. / The work carried out during this thesis focuses on the quantum dynamics of the diffusion of hydrogen atoms on a surface of palladium (111). The study of the 3D system allowed us to detail the infrared spectrum of H/Pd (111), showing the existence of different adsorption sites on which localized states exist that are strongly coupled (Fermi resonance). This phenomenon governs the diffusion of hydrogen atoms in an ultra-fast time scale (fs).The study of the (6D) H2/Pd(111) system has shown that the transitions observed are in fact transition bands between several quasi-degenerate adsorption states. The agreement between the calculated and measured values is significantly less good than that between the data calculated for the 3D system and the measured data. Does adsorbed hydrogen on palladium exist in the form of a weakly bound H2 molecule? This thesis has provided some answers to this question, which remains open, hovewer, to some extent.