Les protéines fluorescentes, comme la GFP (green fluorescent protein), sont des protéines naturellement fluorescentes qui sont utilisées pour leur rôle de marqueur, permettant de localiser des protéines dans les cellules et d'en suivre les déplacements. De nombreuses études expérimentales et théoriques ont été menées ces dix dernières années sur les protéines fluorescentes. De là, se forge une compréhension essentiellement qualitative du rôle de la protéine vis-à-vis de l’obtention ou non d’une émission radiative : il apparaît que la protéine permet la fluorescence en bloquant les processus qui la désactivent ; ces processus de désactivation sont très rapides et efficaces (à l'échelle de la picoseconde) dans le cas du chromophore seul, et ils sont bien identifiés comme étant des torsions autour des liaisons intercycles (tau et phi). Dans la protéine, la sensibilité des temps de vie de fluorescence à des mutations proches ou non du chromophore, à des modifications de pH ou de température laisse supposer un contrôle de la dynamique du chromophore par différents paramètres, sans qu’ils soient pour autant identifiés et mis en relation.Une étude de la dynamique de la protéine permettrait de faire la lumière sur les mécanismes responsables de ces phénomènes photophysiques pour lesquels une analyse structurale ne suffit pas. Cependant l'étude de la dynamique est limitée par la taille du système (>30 000 atomes), par l'échelle de temps des phénomènes photophysiques considérés (dizaine de nanosecondes) et par le fait que les deux torsions tau et phi sont fortement couplées dans l'état excité du chromophore. Ces trois facteurs excluent les méthodes de dynamique existantes aujourd'hui ; dynamique quantique (AIMD), dynamique mixte classique-quantique (QM/MD) et dynamique moléculaire classique (MD).Nous avons surmonté le problème par la modélisation de la surface d’énergie potentielle de torsion du chromophore à l’état excité basée sur des calculs quantiques de haute précision, par une interpolation des valeurs obtenues par une expression analytique appropriée en fonction des angles de torsion tau et phi et avec une précision suffisante pour reproduire des barrières de l’ordre de la kcal/mol, et enfin, par l’implémentation de cette expression analytique dans le programme parallèle AMBER. Une deuxième difficulté théorique concerne la simulation et l’analyse statistique d’événements peu fréquents à l’échelle de la nanoseconde, et dont on ne connait pas le chemin de réaction, ici les déformations de la protéine et du chromophore conduisant aux géométries favorables à la conversion interne. Grâce à ces développements et aux simulations qu'ils ont permises, nous avons réalisé la première modélisation de la désactivation non-radiative par conversion interne à l’échelle de la nanoseconde dans trois protéines fluorescentes différentes. L’analyse des dynamiques moléculaires classiques nous donne une évaluation quantitative des temps de vie de l’extinction de fluorescence, en accord avec les données expérimentales. Par ailleurs elle nous a permis d'identifier les mouvements moléculaires concertés de la protéine et du chromophore conduisant à cette extinction. De ces résultats, émerge une représentation plus complète du mécanisme qui libère la torsion du chromophore ou qui la déclenche : il peut venir d’un mouvement spécifique de la protéine, qui se produit à l’échelle de la nanoseconde, ou bien de plusieurs mouvements spécifiques, plus fréquents (rupture de liaisons hydrogène, rotation de chaînes latérales, dynamique d'agrégats d’eau), mais qui coïncident seulement à l’échelle de la nanoseconde. Ces mouvements spécifiques n’ont pas un coût énergétique important mais la nécessité de leur coïncidence crée un délai de l’ordre de quelques nanosecondes alors que dans le vide la torsion se produit en quelques picosecondes. Dans le cas des protéines étudiées, on a identifié en grande partie les mécanismes et les acides aminés qui sont impliqués. / Fluorescent proteins, like GFP (green fluorescent protein), are efficient sensors for a variety of physical-chemical properties and they are extensively used as markers in living cells imaging. These proteins have been widely studied both experimentally and theoretically the last decade. The comprehension of the protein's role in the regulation of the radiative emission is today essentially qualitative: it appears that the protein enables the fluorescence by blocking the processes that deactivates it; the deactivating processes are very quick and efficient (on the picosecond time scale) when the chromophore is isolated, and they are identified as being the torsions around the central bonds of the chromophore (tau and phi). The fluorescence lifetimes of a protein is very sensitive to mutations in the vicinity of the chromophore, to modifications in pH or in temperature. This seems to indicate a control of the dynamics of the chromophore by different parameters, that are not necessarily identified.A study of the dynamics of the protein would allow a deeper understanding of the mechanisms that are responsible for the fluorescence quenching. From a theoretical point of view, one is faced with three difficulties in this type of study: the size of the system (>30 000 atoms including a water box), the required time scale (tens of nanoseconds) and the fact that the torsions tau and phi are strongly coupled in the excited state of the chromophore. We must thus rule out the already existing dynamics methods: quantum dynamics (AIMD), mixed classical-quantum dynamics (QM/MD) and classical molecular dynamics (MD).We have overcome this problem by modeling the torsional potential energy surface of the chromophore in the first excited state trough high precision quantum calculations, by interpolating the energy values with an analytical fitting expression depending on the torsions tau and phi and with a precision high enough to reproduce barriers of the order of 1 kcal/mol, and lastly, by implementing this fitting expression in a parallelized version of the MD program AMBER. Another theoretical difficulty concerns the simulation and the statistical analysis of rare events on the nanosecond time scale without knowing the reaction path in advance, i.e. the deformations of the protein and of the chromophore leading to geometries where the internal conversion is favored. As a result of these developments and of the simulations they have enabled, we have been able to model, for the first time, the non-radiative deactivation by internal conversion at the nanosecond time scale in three different fluorescent proteins. The analysis of the classical molecular dynamics gives us a quantitative evaluation of the lifetime of the fluorescence extinction, in agreement with experimental results. In addition, it has allowed us to identify the concerted molecular movements between the protein and the chromophore leading to this extinction. A more complete representation of the mechanism that liberates or provokes the chromophore torsion emerges from these results: it could be a specific movement of the protein, that occurs on the nanosecond timescale, or several specific movements that occur more frequently (breakage of a hydrogen bond, rotation of side chains, dynamics of a water cluster), but that coincide only on the nanosecond time scale. These specific movements do not have a high energy cost but the need for them to coincide creates a delay of several nanoseconds compared to the chromophore torsion in vacuo which occurs after a few picoseconds. In the proteins we have studied (GFP, YFP and Padron), we have identified the principle components of the mechanisms and the amino acids that are implicated in this chromophore-protein interplay.

Les molécules aromatiques protonées jouent un rôle important dans les réactions de substitution électrophile aromatique, et dans différents processus biologiques. Ces molécules sont présentes aussi dans d’autres milieux tels que les flammes de combustion, les plasmas de divers hydrocarbures, les ionosphères planétaires (Titan) et le milieu interstellaire. Les molécules protonées sont très stables car elles ont des couches électroniques complètes mais elles sont en général très sensibles à leur environnement local car elles sont chargées : une étude en phase gazeuse est nécessaire pour déterminer leurs propriétés intrinsèques. Jusqu’à présent, très peu de chose était connu sur les molécules protonées isolées en phase gazeuse, seulement quelques résultats étaient disponibles. Ce manque de données venait de la difficulté de générer des molécules protonées en phase gazeuse et surtout de les produire à basse température (la protonation est une réaction exothermique). Récemment, des progrès ont permis d’étudier les molécules protonées en phase gazeuse à très basse température, en particulier par le développement des sources ioniques couplées avec des techniques d'expansion de jet supersonique. Grâce à cette technique on a enregistré le spectre photo fragmentation de l’état fondamental vers le premier état excité (S1←S0) de différentes molécules aromatiques protonées en phase gazeuse. Les molécules que nous avons étudiées peuvent être regroupées en quatre familles : Les molécules polycycliques aromatiques protonées linéaires (benzène, naphtalène, anthracène, tétracène, pentacène). Les molécules polycycliques aromatiques protonées non linéaires (fluorène, phénanthrène, pyrène). Les molécules protonées contenant un hétéro atome (benzaldéhyde, salicylaldéhyde, 1-naphthol et 2-naphthol, indole, aniline). Les agrégats protonés (dimère de benzène, naphtalène (H2O)n, n=1,2,3. naphtalène (NH3)n, n=1,2,3, benzaldéhyde (Ar , N2)). Dans les spectres enregistrés presque toutes les transitions électroniques S1←S0 sont décalées vers le rouge (basse énergie) par rapport à celui des molécules parentes neutres. Ce décalage est dû au caractère transfert de charge du premier état excité. Certains spectres sont résolus vibrationnellement, alors que pour d'autres molécules le spectre ne présente pas de progression vibrationnelle à cause d’un dynamique très rapide de l’état excité menant par des intersections coniques à l’état fondamental. Les spectres d’absorption des molécules protonées sont plus riches en vibrations par comparaison avec les molécules neutre. Cela reflète le changement relativement important de géométrie de l’état excité dû à son caractère transfert de charge. Les résultats expérimentaux ont été complétés par des calculs ab-initio qui ont permis de localiser la transition électronique, déterminer la structure géométrique et électronique, les modes de vibration et, pour certaines de ces molécules, la dynamique de l’état excité. Les calculs sont en général en très bon accord avec les expériences. / Protonated aromatic molecules play an important role in electrophilic aromatic substitution reactions, fundamental reactions in organic chemistry and in various biological processes. The interstellar medium is another environment which is likely to contain the protonated aromatic molecules, that’s because these molecules are stable chemically since they are close shell electronic structure. These molecules were also identified in others environments such as combustion flames, plasmas of various hydrocarbons and the upper atmosphere of Titan. Protonated molecules are usually very sensitive to their local environment; a gas phase study is required to determine their intrinsic properties. Until now, very little is known about the isolated protonated molecules, only a few results are available in the literature. This lack of data is due to the difficulties of the production and the cooling of these molecules in gas phase. The technical progress we have done has enabled the study of protonated molecules in the gas phase at very low temperatures, using an ion sources, supersonic jet and the laser induced photofragmentation techniques. Using this technique, we have recorded many electronic spectra (S1←S0) of different protonated molecules. We can regroup the studied molecules into four: Linear protonated polycyclic aromatic molecules (benzene, naphthalene, anthracene, tetracene, pentacene). Nonlinear protonated polycyclic aromatic molecules (fluorene, phenanthrene, pyrene). Protonated molecules containing an hetero atom (benzaldehyde, salicylaldehyde, 1-naphthol and 2-naphthol, indole, aniline). Protonated cluster (dimer of benzene, naphthalene (H2O)n, n = 1,2,3. Naphthalene (NH3)n, n = 1,2,3, benzaldehyde (Ar, N2)). Most of those spectra are red-shifted compare to the spectrums of neutral parent molecules. This red-shift is due to charge transfer character of the first excited state. Some spectra are vibrationally resolved, while for other molecules the spectrum do not shows any vibrational progression. This behaviour is explained by the dynamic of the excited state, this dynamic being usually is very fast, sometimes leading to the ground state through a conical intersection. The spectra of protonated molecules are very active vibrationally in comparison with neutral molecules, many vibrational modes forbidden for neutral molecule becomes active for the protonated one (Franck-Condon factor is not zero). This is reflecting the charge transfer character of the excited state. The experimental results were complemented by ab-initio calculations, which have allowed determining the electronic transition, the geometric and electronic structure of the molecule, the vibrational modes, and for some of these molecules the dynamics of excited state. Calculations are generally in very good agreement with experiments.

Neste trabalho, são estudadas as alterações das propriedades ópticas lineares e não lineares de soluções de azocompostos devidas aos mecanismos de isomerização e às alterações das propriedades estruturais com a temperatura. A dependência da transição pipi* com a estrutura linear dos azocompostos é notada já nas medidas dos espectros de absorção em função da temperatura para o isômero trans. Através do conhecimento dos níveis de energia e dos tempos de relaxação via isomerização, foi possível obter a dinâmica entre os isômeros cis e trans. As medidas não lineares forneceram propriedades interessantes associadas aos estados de energia dos compostos. Por exemplo, através de experimentos de varredura-z e de excitação e prova, foi possível ver que os azocompostos apresentam uma alta transparência quando excitados, a qual desaparece com o término da isomerização. Medidas em função do comprimento de onda mostraram que a transparência observada está presente em toda a banda pipi* e não ocorre na banda npi* . Também foi observado que o tempo de isomerização muda de acordo com o comprimento de onda de excitação, o que pode estar relacionado com a superposição das duas bandas. Os resultados obtidos em femtossegundos foram essenciais para descrever o processo dinâmico de fotoisomerização, observado, por completo, através de medidas com varredura-Z em picossegundos e nanossegundos. Essas medidas forneceram os valores das seções de choque dos isômeros cis, que são difíceis de serem quantificadas devido ao curto tempo de vida desse isômero. Além dos resultados ressonantes, foram feitos experimentos de absorção de dois fótons em femtossegundos usando a técnica de varredura-Z. Esses estudos mostraram a dependência das seções de choque de absorção de dois fótons com características estruturais das moléculas, tais como comprimento de conjugação, grupos push-pull e planaridade. Os resultados ressonantes e não ressonantes obtidos em femtossegundos serviram de base para a calibração da técnica de varredura-Z com pulsos de luz branca. Essa técnica se mostrou adequada para a obtenção dos espectros das não linearidades ópticas ressonantes e não ressonantes em uma única medição (de 5 minutos), diminuindo assim flutuações do laser durante o experimento. / This work reports on the temperature dependence of linear and nonlinear properties of azocompounds solutions due to isomerization mechanisms. The dependence of pipi* transitions on the linear structure of azocompounds is already noticeble in the measurements of absorption spectra as function of the temperature for the trans isomer. Knowing the energy levels and the relaxation times through isomerization, it was possible to obtain the exchange dynamics between cis and trans conformations. Nonlinear measurements provided interesting properties associated with the energy levels of de compounds. For exemple, through Z-scan and pumpprobe experiments, it was possible to verify that azocompounds present a high transparency when excited and that this transparency disapears when the izomerization ends. The wavelength change has shown that the observed transparency is present along the complete pipi* band, but not in the npi* band. It was also observed that the isomerization time changes with the exciting wavelength, which may be related to the superposition of both bands. The results obained with femtoseconds pulses were essential to completily describe the photoisomerization process observed with Z-scan measurements using picoseconds and nanoseconds pulses. These measurements provided values of the crosssection of the cis conformation, which are difficult to be quantified due to the short lifetime of this isomer. Besides ressonant results, experiments of two-photon absorption in the femtosecond regime using the Z-scan technique were made. These studies shown the dependence of the two photons absorption cross-section on structural features of molecules such as conjugation length, push-pull groups and planarity. The ressonant and nonressonant results obteined with femtoseconds have provide the calibration of the Z-scan technique with white light pulses. This technique has been found able to obtain the spectra of ressonat and nonressonant nonlinearities in a single measurement (about 5 minutes), diminishing laser fluctuation during the experiment.

No description available.

Time resolved spectroscopy is one of the crucial methods used to study processes on molecular level in biological systems. It is useful especially for monitoring fast processes that take a place in photosynthetic apparatus of photosynthetic organisms, such as electron and energy transfer. The integral parts of photosynthetic apparatus are carotenoids, whose role in the photosynthetic apparatus is not as well explored as it is for chlorophylls. It was proved that carotenoids actively participate in energy transfer processes in photosynthetic antennas. They have a crucial role in protection against excess energy damage. They are also electron donors in both antennas and reaction centers. The fact that photo-physical properties of carotenoids are much different from properties of others organic pigments, complicates studies of their functions in photosynthesis as well as in other biological systems. This thesis employs advanced methods of femtosecond spectroscopy to obtain more information about carotenoid functions in some biological systems and in solution with special focus on carotenoids containing carbonyl group.

Neste trabalho, são estudadas as alterações das propriedades ópticas lineares e não lineares de soluções de azocompostos devidas aos mecanismos de isomerização e às alterações das propriedades estruturais com a temperatura. A dependência da transição pipi* com a estrutura linear dos azocompostos é notada já nas medidas dos espectros de absorção em função da temperatura para o isômero trans. Através do conhecimento dos níveis de energia e dos tempos de relaxação via isomerização, foi possível obter a dinâmica entre os isômeros cis e trans. As medidas não lineares forneceram propriedades interessantes associadas aos estados de energia dos compostos. Por exemplo, através de experimentos de varredura-z e de excitação e prova, foi possível ver que os azocompostos apresentam uma alta transparência quando excitados, a qual desaparece com o término da isomerização. Medidas em função do comprimento de onda mostraram que a transparência observada está presente em toda a banda pipi* e não ocorre na banda npi* . Também foi observado que o tempo de isomerização muda de acordo com o comprimento de onda de excitação, o que pode estar relacionado com a superposição das duas bandas. Os resultados obtidos em femtossegundos foram essenciais para descrever o processo dinâmico de fotoisomerização, observado, por completo, através de medidas com varredura-Z em picossegundos e nanossegundos. Essas medidas forneceram os valores das seções de choque dos isômeros cis, que são difíceis de serem quantificadas devido ao curto tempo de vida desse isômero. Além dos resultados ressonantes, foram feitos experimentos de absorção de dois fótons em femtossegundos usando a técnica de varredura-Z. Esses estudos mostraram a dependência das seções de choque de absorção de dois fótons com características estruturais das moléculas, tais como comprimento de conjugação, grupos push-pull e planaridade. Os resultados ressonantes e não ressonantes obtidos em femtossegundos serviram de base para a calibração da técnica de varredura-Z com pulsos de luz branca. Essa técnica se mostrou adequada para a obtenção dos espectros das não linearidades ópticas ressonantes e não ressonantes em uma única medição (de 5 minutos), diminuindo assim flutuações do laser durante o experimento. / This work reports on the temperature dependence of linear and nonlinear properties of azocompounds solutions due to isomerization mechanisms. The dependence of pipi* transitions on the linear structure of azocompounds is already noticeble in the measurements of absorption spectra as function of the temperature for the trans isomer. Knowing the energy levels and the relaxation times through isomerization, it was possible to obtain the exchange dynamics between cis and trans conformations. Nonlinear measurements provided interesting properties associated with the energy levels of de compounds. For exemple, through Z-scan and pumpprobe experiments, it was possible to verify that azocompounds present a high transparency when excited and that this transparency disapears when the izomerization ends. The wavelength change has shown that the observed transparency is present along the complete pipi* band, but not in the npi* band. It was also observed that the isomerization time changes with the exciting wavelength, which may be related to the superposition of both bands. The results obained with femtoseconds pulses were essential to completily describe the photoisomerization process observed with Z-scan measurements using picoseconds and nanoseconds pulses. These measurements provided values of the crosssection of the cis conformation, which are difficult to be quantified due to the short lifetime of this isomer. Besides ressonant results, experiments of two-photon absorption in the femtosecond regime using the Z-scan technique were made. These studies shown the dependence of the two photons absorption cross-section on structural features of molecules such as conjugation length, push-pull groups and planarity. The ressonant and nonressonant results obteined with femtoseconds have provide the calibration of the Z-scan technique with white light pulses. This technique has been found able to obtain the spectra of ressonat and nonressonant nonlinearities in a single measurement (about 5 minutes), diminishing laser fluctuation during the experiment.

Photosensitizing effects of xenobiotics are of increasing concern in public health since modern lifestyle often associates sunlight exposure with the presence of chemical substances in the skin. An important number of chemicals like perfumes, sunscreen components, or therapeutic agents have been reported as photosensitizers. In this context, a considerable effort has been made to design a model system for photosafety assessment. Indeed, screening for phototoxicity is necessary at the early phase of drug discovery process, even before introducing drugs and chemicals into clinical therapy, to prevent undesired photoreactions in humans. In the case of new pharmaceuticals, their phototoxic potential has to be tested when they absorb in the regions corresponding to the solar spectrum, that is, for wavelengths >290 nm. So, there is an obvious need for a screening strategy based on in vitro experiments. The goal of the present thesis was the photochemical study of different photoactive drugs to investigate the key molecular aspects responsible for their photosensitivity side effects. In a first stage, rosuvastatin was considered in chapter 3 as representative compound of the statin family. This lipid-lowering drug, also known as “superstatin”, contains a 2-vinylbiphenyl-like moiety and has been previously described to decompose under solar irradiation, yielding stable dihydrophenanthrene analogues. During photophysical characterization of rosuvastatin, only a long-lived transient at ca. 550 nm was observed and assigned to the primary photocyclization intermediate. Thus, the absence of detectable triplet-triplet absorption and the low yield of fluorescence ruled out the role of the parent drug as an efficient sensitizer. In this context, the attention was placed on the rosuvastatin main photoproduct (ppRSV). Indeed, the photobehavior of this dihydrophenanthrene-like compound presented the essential components needed for an efficient biomolecule photosensitizer i.e. (i) a high intersystem crossing quantum yield (ΦISC =0.8), (ii) a triplet excited state energy of ca. 67 kcal mol−1 , and (iii) a quantum yield of singlet oxygen formation (Φ∆) of 0.3. Furthermore, laser flash photolysis studies revealed a triplet-triplet energy transfer from the triplet excited state of ppRSV to thymidine, leading to the formation of cyclobutane thymidine dimers, an important type of DNA lesion. Finally, tryptophan was used as a probe to investigate the Type I and/or Type II character of ppRSV-mediated oxidation. In this way, both an electron transfer process giving rise to the tryptophanyl radical and a singlet oxygen mediated oxidation were observed. On the basis of the obtained results, rosuvastatin, through its major photoproduct ppRSV, should be considered as a potential sensitizer. Then, itraconazole (ITZ), a broad-spectrum antifungal agent, was chosen as main character of chapter 4. Its photochemical properties were investigated in connection with its reported skin photosensitivity disorders. Steady state photolysis, fluorescence and phosphorescence experiments were performed to understand ITZ photoreactivity in biological media. The drug is unstable under UVB irradiation, suffering a primary dehalogenation of the 2,4-dichlorophenyl moiety that occurs mainly at the ortho-position. In poorly H-donating solvents, as acetonitrile, the major photoproduct arises from intramolecular attack of the initially generated aryl radical to the triazole ring. In addition, reduced compounds resulting from homolytic cleavage of the C-Cl bond in ortho or para positions and subsequent Habstraction from the medium are obtained to a lesser extent. In good H-donating solvents, such as ethanol, the main photoproducts are formed by reductive dehalogenation. Furthermore, irradiation of a model dyad containing a tryptophan unit and the reactive 2,4-dichlorophenyl moiety of itraconazole leads to formation of a new covalent link between these two substructures revealing that homolysis of the C-Cl bond of ITZ can result in alkylation of reactive amino acid residues of proteins, leading to formation of covalent photoadducts. Therefore, it has been established that the key process in the photosensitization by itraconazole is cleavage of the carbon-halogen bond, which leads to aryl radicals and chlorine atoms. These highly reactive species might be responsible for extensive free radical-mediated biological damage, including lipid peroxidation or photobinding to proteins. In chapter 5, photobehavior of imatinib (IMT) was addressed. This is a promising tyrosine kinase inhibitor used in the treatment of some types of human cancer, which constitutes a successful example of rational drug design based on the optimization of the chemical structure to reach an improved pharmacological activity. Cutaneous reactions, such as increased photosensitivity or pseudoporphyria, are among the most common nonhematological IMT side effects; however, the molecular bases of these clinical observations have not been unveiled yet. Thus, to gain insight into the IMT photosensitizing properties, its photobehavior was studied together with that of its potentially photoactive anilino-pyrimidine and pyridyl-pyrimidine fragments. In this context, steady-state and time resolved fluorescence, as well as laser flash photolysis experiments were run, and the DNA photosensitization potential was investigated by means of single strand breaks detection using agarose gel electrophoresis. The obtained results revealed that the drug itself and its anilino-pyrimidine fragment are not DNA-photosensitizers. By contrast, the pyridyl-pyrimidine substructure displayed a marked photogenotoxic potential, which was associated with the generation of a long-lived triplet excited state. Interestingly, this reactive species was efficiently quenched by benzanilide, another molecular fragment of IMT. Clearly, integration of the photoactive pyridyl-pyrimidine moiety in a more complex structure strongly modifies its photobehavior, which in this case is fortunate as it leads to an improved toxicological profile. Thus, on the bases of the experimental results, direct in vivo photosensitization by IMT seems unlikely. Instead, the reported photosensitivity disorders could be related to indirect processes, such as the previously suggested impairment of melanogenesis or the accumulation of endogenous porphyrins. Finally, a possible source of errors in the TEMPO/EPR method for singlet oxygen detection was analyzed. For many biological and biomedical studies, it is essential to detect the production of 1O2 and to quantify its production yield. Among the available methods, detection of the characteristic 1270 nm phosphorescence of singlet oxygen by time-resolved near infrared (TRNIR) emission constitutes the most direct and unambiguous approach. An alternative indirect method is electron paramagnetic resonance (EPR) in combination with trapping. This is based on the detection of the TEMPO free radical formed after oxidation of TEMP (2,2,6,6- tetramethylpiperidine) by singlet oxygen. Although the TEMPO/EPR method has been largely employed, it can produce misleading data. This was demonstrated by the present study, where the quantum yields of singlet oxygen formation obtained by TRNIR emission and by the TEMPO/EPR method were compared for a set of well-known photosensitizers. The results revealed that the TEMPO/EPR method leads to significant overestimation of singlet oxygen yield when the singlet or triplet excited state of the photosensitizers were efficiently quenched by TEMP, acting as electron donor. In such case, generation of the TEMP+• radical cation, followed by deprotonation and reaction with molecular oxygen gives rise to a EPR detectable TEMPO signal that is not associated with singlet oxygen production. This knowledge is essential for an appropriate and error-free application of the TEMPO/EPR method in chemical, biological and medical studies. / Nardi, G. (2014). MECHANISTIC STUDIES ON THE PHOTOTOXICITY OF ROSUVASTATIN, ITRACONAZOLE AND IMATINIB [Tesis doctoral no publicada]. Universitat Politècnica de València. https://doi.org/10.4995/Thesis/10251/48535 / TESIS

多数の溶媒分子に取り囲まれている溶液中において溶質分子の化学反応素過程を考える場合、溶媒分子による反応の平衡論的、動的な効果を考える必要がある。本研究では、ユニークな反応場として水や有機溶媒とは区別される、超臨界流体とイオン液体をとり上げ、溶質分子のプロトン移動反応、光解離反応について、時間分解レーザー分光と分子動力学計算、理論的解析を行い、その現象を明らかにする試みをおこなった。 / In solution, solvent molecules involve chemical reaction of solute molecules and could alter both reaction yield and kinetics. In this thesis, the author focused on fundamental chemical reactions (intermolecular proton transfer and photodissociate reaction) in a unique class of solvents, supercritical fluids and ionic liquids. By measuring time-resolved fluorescence spectrum and transient absorption spectrum of solutes, the author discusses how the reaction yield and kinetics are described by solvent physicochemical properties. / 博士(理学) / Doctor of Philosophy in Science / 同志社大学 / Doshisha University