Βασικός στόχος της παρούσας διατριβής είναι η αποσαφήνιση του τρόπου της διεπιφανειακής εναπόθεσης του νικελίου στην επιφάνεια της τιτάνιας, η οποία λαμβάνει χώρα στη διεπιφάνεια “τιτάνιας / ηλεκτρολυτικού διαλύματος”. Ο στόχος αυτός επιτεύχθηκε μέσω μιας κατάλληλης θεωρητικής και υπολογιστικής επεξεργασίας δεδομένων, που προέρχονται από την εφαρμογή ηλεκτροχημικών και φασματοσκοπικών τεχνικών, την εκτέλεση πειραμάτων προσρόφησης, καθώς επίσης και σε ab – initio υπολογισμούς για την εξακρίβωση της δομής των συμπλόκων εσωτερικής σφαίρας τα οποία σχηματίζονται και των συγκεντρώσεών τους στη διεπιφάνεια. Δείγματα βιομηχανικής τιτάνιας (Degussa, P 25) πλούσιας σε ανατάση χρησιμοποιήθηκαν για το σκοπό αυτό. Η μελέτη πραγματοποιήθηκε για μια ευρεία περιοχή παραμέτρων εμποτισμού και πιο συγκεκριμένα τιμές pH, ιονικής ισχύος και συγκέντρωσης του υδατικού συμπλόκου [Ni(H2O)6]2+ στο διάλυμα. Μεταβάλλοντας τις παραμέτρους αυτές ρυθμίστηκε η επιφανειακή συγκέντρωση των ιόντων Ni(II). Χρησιμοποιήθηκε μια πληθώρα μεθοδολογιών στηριγμένες σε δεδομένα εναπόθεσης, μετρήσεις τιμών pH, ποτενσιομετρικές τιτλοδοτήσεις μάζας και πειράματα μικροηλεκτροφόρησης σε συνδυασμό με φασματοσκοπία διάχυτης ανάκλασης (DRS). Ο συνδυασμός όλων των παραπάνω φαίνεται πως υποδεικνύει το σχηματισμό μονοπυρηνικών / ολιγοπυρηνικών συμπλόκων εσωτερικής σφαίρας κατά την εναπόθεση των ιόντων [Ni(H2O)6]2+ στη διεπιφάνεια “τιτάνιας / ηλεκτρολυτικού διαλύματος”. Η μοντελοποίηση της διαδικασίας εναπόθεσης η οποία βασίστηκε στα προαναφερθέντα πειραματικά αποτελέσματα, αποκάλυψε την ακριβή δομή αυτών των επιφανειακών συμπλόκων και κατέστησε δυνατό τον προσδιορισμό της κατανομής των εναποτιθέμενων ειδών και ειδικότερα των σχετικών τους συγκεντρώσεων για διάφορες τιμές της επιφανειακής συγκέντρωσης Ni(II). Στο συμπαγές τμήμα της διεπιφάνειας “τιτάνιας / ηλεκτρολυτικού διαλύματος” σχηματίζονται τρία μονοπυρηνικά σύμπλοκα εσωτερικής σφαίρας: ένα μονο - υποκατεστημένο, δι - υδρολυμένο σύμπλοκο πάνω από τις ακραίες οξο - ομάδες ανταλλάσοντας ένα υδατικό υποκαταστάτη με ένα επιφανειακό άτομο οξυγόνου (διαμόρφωση TiO), ένα δι - υποκατεστημένο, δι - υδρολυμένο σύμπλοκο πάνω από δύο ακραίες γειτονικές οξο - ομάδες ανταλλάσοντας δύο υδατικούς υποκαταστάτες με δύο επιφανειακά άτομα οξυγόνου (διαμόρφωση TiO - TiO) και ένα δι - υποκατεστημένο μη υδρολυμένο σύμπλοκο πάνω από μία ακραία και μία γεφυρωμένη οξο - ομάδα (διαμόρφωση Ti2O - TiO). Επιπρόσθετα, σχηματίζονται ένα διπυρηνικό και ένα τριπυρηνικό σύμπλοκο εσωτερικής σφαίρας κατά την εναπόθεση των ιόντων [Ni(H2O)6]2+ στο συμπαγές τμήμα της διεπιφάνειας “τιτάνιας / ηλεκτρολυτικού διαλύματος”. Στην πρώτη περίπτωση η θέση υποδοχής συμπεριλαμβάνει μία γεφυρωμένη και δύο ακραίες οξο - ομάδες (διαμόρφωση Ti2O-TiO—TiO), ενώ στη δεύτερη περίπτωση δύο γεφυρωμένες και τρεις ακραίες οξο - ομάδες (διαμόρφωση Ti2O-TiO—TiO—TiO-Ti2O). Η διαμόρφωση TiO κυριαρχεί σε όλο το εύρος της περιοχής επιφανειακών συγκεντρώσεων το οποίο μελετήθηκε. Η συνεισφορά των διαμορφώσεων TiO - TiO και Ti2O - TiO είναι επίσης σημαντική σε πολύ χαμηλές τιμές επιφανειακής συγκέντρωσης Ni(II), μειώνεται όμως σε μεγάλο βαθμό καθώς αυτή αυξάνεται. Οι σχετικές επιφανειακές συγκεντρώσεις των διαμορφώσεων Ti2O-TiO--TiO και Ti2O-TiO—TiO--TiO-Ti2O αρχικά αυξάνουν με την επιφανειακή συγκέντρωση Ni(II) και μετά μένουν πρακτικά σταθερές. Η προαναφερθείσα κατανομή των εναποτιθέμενων ειδών στη διεπιφάνεια εξηγήθηκε με τη χρήση στερεοχημικών όρων. Επιπρόσθετα, η δομή των επιφανειακών συμπλόκων εσωτερικής σφαίρας και η κατανομή αυτή είναι σε γενική συμφωνία με εκείνες οι οποίες προβλέφθηκαν με την εκτέλεση ημιεμπειρικών κβαντομηχανικών υπολογισμών για την εναπόθεση του Ni στο TiO2. Το μοντέλο εναπόθεσης το οποίο αναπτύχθηκε περιέγραψε πολύ καλά τις adsorption edges, τις τιτλοδοτήσεις “πρωτονίου - ιόντος” και τις ισόθερμες εναπόθεσης, ενισχύοντας επιπλέον την αξιοπιστία και ορθότητά του. / The main goal of this work is the elucidation of the mode of interfacial deposition of nickel on the surface of titania, which takes place in the “titania / electrolytic solution” interface. This goal was achieved through the use of several methodologies combined with spectroscopic techniques, as well as ab – initio calculations in order to determine the structure of the inner sphere complexes formed as well as their relative interfacial concentrations. Samples of titania (Degussa, P 25) rich in anatase were used for this purpose. The study was performed over a quite wide range of impregnation parameters namely pH, ionic strength and concentration of the [Ni(H2O)6]2+ aqua complex in the solution. By changing these parameters, the Ni(II) surface concentration was regulated. Several methodologies based on deposition data, pH measurements, potentiometric mass titrations and microelectrophoresis have been used in conjunction with diffuse reflectance spectroscopy. These suggested the formation of mono - nuclear / oligo - nuclear inner sphere complexes upon deposition of the [Ni(H2O)6]+2 ions at the “titania / electrolytic solution” interface. The modelling of the deposition process based on the aforementioned experimental results revealed the exact structure of these surface complexes and allowed the determination of their relative concentrations at various values of Ni(II) surface concentration (interfacial speciation). Three mono-nuclear inner sphere complexes are formed at the compact layer of the “titania / electolytic solution” interface; one mono - substituted, di - hydrolyzed complex above the terminal oxo - groups by exchanging one water ligand with a surface oxygen atom (TiO configuration), a di - substituted, di - hydrolyzed complex above two terminal adjacent oxo - groups by exchanging two water ligands with the two surface oxygen atoms (TiO-TiO configuration) and one di - substituted, non - hydrolyzed complex above one terminal and one bridging adjacent oxo - groups ( Ti2O-TiO configuration). One binuclear and one three - nuclear complex are formed, in addition, at the compact layer. In the first case the receptor site involves one bridging and two terminal oxo- groups (Ti2O-TiO--TiO configuration) whereas in the second case the receptor site involves two bridging and three terminal oxo - groups (Ti2O-TiO--TiO--TiO-Ti2O configuration). The TiO configuration predominates in the whole range of the surface concentration studied. The contribution of the TiO-TiO and Ti2O-TiO configurations is also important at very low Ni(II) surface concentration, but this contribution is rapidly decreased as the Ni(II) surface concentration increases. The relative surface concentrations of the Ti2O-TiO--TiO and Ti2O-TiO--TiO--TiO-Ti2O configurations initially increase with the Ni(II) surface concentration and then remain practically constant. The aforementioned interfacial speciation was explained in stereochemical terms. Moreover, the structure of the inner sphere surface complexes and the interfacial speciation are in general agreement with those predicted by performing semi-empirical quantum chemical calculations of the deposition process. The deposition model developed has described the ‘adsorption edges’, the ‘proton–ion titration curves’ and the deposition isotherms well, further corroborating its validity.

Plasmonic properties and the related novel applications are studied on various types of metallic nano-structures in one, two, or three dimensions. For 1D nanostructure, the motion of free electrons in a metal-film with nanoscale thickness is confined in its normal dimension and free in the other two. Describing the free-electron motion at metal-dielectric surfaces, surface plasmon polariton (SPP) is an elementary excitation of such motions and is well known. When further perforated with periodic array of holes, periodicity will introduce degeneracy, incur energy-level splitting, and facilitate the coupling between free-space photon and SPP. We applied this concept to achieve a plasmonic perfect absorber. The experimentally observed reflection dip splitting is qualitatively explained by a perturbation theory based on the above concept. If confined in 2D, the nanostructures become nanowires that intrigue a broad range of research interests. We performed various studies on the resonance and propagation of metal nanowires with different materials, cross-sectional shapes and form factors, in passive or active medium, in support of corresponding experimental works. Finite- Difference Time-Domain (FDTD) simulations show that simulated results agrees well with experiments and makes fundamental mode analysis possible. Confined in 3D, the electron motions in a single metal nanoparticle (NP) leads to localized surface plasmon resonance (LSPR) that enables another novel and important application: plasmon-heating. By exciting the LSPR of a gold particle embedded in liquid, the excited plasmon will decay into heat in the particle and will heat up the surrounding liquid eventually. With sufficient exciting optical intensity, the heat transfer from NP to liquid will undergo an explosive process and make a vapor envelop: nanobubble. We characterized the size, pressure and temperature of the nanobubble by a simple model relying on Mie calculations and continuous medium assumption. A novel effective medium method is also developed to replace the role of Mie calculations. The characterized temperature is in excellent agreement with that by Raman scattering. If fabricated in an ordered cluster, NPs exhibit double-resonance features and the double Fano-resonant structure is demonstrated to most enhance the four-wave mixing efficiency.

A new method, probability distribution of diffusivities (time scaled square displacements between succeeding video frames), was developed to analyze single molecule tracking (SMT) experiments. This method was then applied to SMT experiments on ultrathin liquid tetrakis(2-ethylhexoxy)silane (TEHOS) films on Si wafer with 100 nm thermally grown oxide, and on thin semectic liquid crystal films. Spatial maps of diffusivities from SMT experiments on 220 nm thick semectic liquid crystal films reveal structure related dynamics. The SMT experiments on ultrathin TEHOS films were complemented by fluorescence correlation spectroscopy (FCS). The observed strongly heterogeneous single molecule dynamics within those films can be explained by a three-layer model consisting of (i) dye molecules adsorbed to the substrate, (ii) slowly diffusing molecules in the laterally heterogeneous near-surface region of 1 - 2 molecular diameters, and (iii) freely diffusing dye molecules in the upper region of the film. FCS and SMT experiments reveal a strong influence of substrate heterogeneity on SM dynamics. Thereby chemisorption to substrate surface silanols plays an important role. Vertical mean first passage times (mfpt) in those films are below 1 µs. This appears as fast component in FCS autocorrelation curves, which further contain a contribution from lateral diffusion and from adsorption events. Therefore, the FCS curves are approximated by a tri-component function, which contains an exponential term related to the mfpt, the correlation function for translational diffusion and a stretched exponential term for the broad distribution of adsorption events. Lateral diffusion coefficients obtained by FCS on 10 nm thick TEHOS films, thereby, are effective diffusion coefficients from dye transients in the focal area. They strongly depend on the substrate heterogeneity. Variation of the frame times for the acquisition of SMT experiments in steps of 20 ms from 20 ms to 200 ms revealed a strong dependence of the corresponding probability distributions of diffusivities on time, in particular in the range between 20 ms and 100 ms. This points to average dwell times of the dye molecules in at least one type of the heterogeneous regions (e.g. on and above silanol clusters) in the range of few tens of milliseconds. Furthermore, time series of SM spectra from Nile Red in 25 nm thick poly-n-alkyl-methacrylate (PnAMA) films were studied. In analogy to translational diffusion, spectral diffusion (shifts in energetic positions of SM spectra) can be studied by probability distributions of spectral diffusivities, i.e. time scaled square energetic displacements. Simulations were run and analyzed to study contributions from noise and fitting uncertainty to spectral diffusion. Furthermore the effect of spectral jumps during acquisition of a SM spectrum was investigated. Probability distributions of spectral diffusivites of Nile Red probing vitreous PnAMA films reveal a two-level system. In contrast, such probability distributions obtained from Nile Red within a 25 nm thick poly-n-butylmethacrylate film around glass transition and in the melt state, display larger spectral jumps. Moreover, for longer alkyl side chains a solvent shift to higher energies is observed, which supports the idea of nanophase separation within those polymers.

A new method, probability distribution of diffusivities (time scaled square displacements between succeeding video frames), was developed to analyze single molecule tracking (SMT) experiments. This method was then applied to SMT experiments on ultrathin liquid tetrakis(2-ethylhexoxy)silane (TEHOS) films on Si wafer with 100 nm thermally grown oxide, and on thin semectic liquid crystal films. Spatial maps of diffusivities from SMT experiments on 220 nm thick semectic liquid crystal films reveal structure related dynamics. The SMT experiments on ultrathin TEHOS films were complemented by fluorescence correlation spectroscopy (FCS). The observed strongly heterogeneous single molecule dynamics within those films can be explained by a three-layer model consisting of (i) dye molecules adsorbed to the substrate, (ii) slowly diffusing molecules in the laterally heterogeneous near-surface region of 1 - 2 molecular diameters, and (iii) freely diffusing dye molecules in the upper region of the film. FCS and SMT experiments reveal a strong influence of substrate heterogeneity on SM dynamics. Thereby chemisorption to substrate surface silanols plays an important role. Vertical mean first passage times (mfpt) in those films are below 1 µs. This appears as fast component in FCS autocorrelation curves, which further contain a contribution from lateral diffusion and from adsorption events. Therefore, the FCS curves are approximated by a tri-component function, which contains an exponential term related to the mfpt, the correlation function for translational diffusion and a stretched exponential term for the broad distribution of adsorption events. Lateral diffusion coefficients obtained by FCS on 10 nm thick TEHOS films, thereby, are effective diffusion coefficients from dye transients in the focal area. They strongly depend on the substrate heterogeneity. Variation of the frame times for the acquisition of SMT experiments in steps of 20 ms from 20 ms to 200 ms revealed a strong dependence of the corresponding probability distributions of diffusivities on time, in particular in the range between 20 ms and 100 ms. This points to average dwell times of the dye molecules in at least one type of the heterogeneous regions (e.g. on and above silanol clusters) in the range of few tens of milliseconds. Furthermore, time series of SM spectra from Nile Red in 25 nm thick poly-n-alkyl-methacrylate (PnAMA) films were studied. In analogy to translational diffusion, spectral diffusion (shifts in energetic positions of SM spectra) can be studied by probability distributions of spectral diffusivities, i.e. time scaled square energetic displacements. Simulations were run and analyzed to study contributions from noise and fitting uncertainty to spectral diffusion. Furthermore the effect of spectral jumps during acquisition of a SM spectrum was investigated. Probability distributions of spectral diffusivites of Nile Red probing vitreous PnAMA films reveal a two-level system. In contrast, such probability distributions obtained from Nile Red within a 25 nm thick poly-n-butylmethacrylate film around glass transition and in the melt state, display larger spectral jumps. Moreover, for longer alkyl side chains a solvent shift to higher energies is observed, which supports the idea of nanophase separation within those polymers.