Wang Yuhao = 利用X光电子谱和导电原子力显微镜对聚3, 4-乙烯二氧噻酚 : 聚苯磺酸改性的研究 / 王宇昊. / Thesis (M.Phil.)--Chinese University of Hong Kong, 2005. / Includes bibliographical references. / Text in English; abstracts in English and Chinese. / Wang Yuhao = Li yong X guang dian zi pu he dao dian yuan zi li xian wei jing dui ju 3, 4-yi xi er yang sai fen : ju ben huang suan gai xing de yan jiu / Wang Yuhao. / Abstract --- p.ii / 論文摘要 --- p.iii / Acknowledgements --- p.iv / Table of Contents --- p.v / List of Figures --- p.ix / List of Tables --- p.xiii / Chapter CHAPTER 1 --- INTRODUCTION --- p.1 / Chapter 1.1 --- Review of conducting conjugated polymers --- p.1 / Chapter 1.1.1 --- Development of conjugated polymer --- p.1 / Chapter 1.1.2 --- Basic concepts in independent-electron theories of conducting conjugated polymers --- p.2 / Chapter 1.1.2.1 --- "Huckel model and its difficulty, the importance of election-phonon" --- p.2 / Chapter 1.1.2.2 --- The SSH model and dimerization --- p.3 / Chapter 1.1.2.3 --- "Charge carriers in conducting conjugated polymers: soliton, polaron and bipolaron" --- p.5 / Chapter 1.1.3 --- "Poly(3,4-ethylenedioxythiophene) or PEDT" --- p.5 / Chapter 1.1.4 --- Derivatives of PEDT --- p.6 / Chapter 1.1.5 --- Application of PEDT and its derivatives --- p.7 / Chapter 1.2 --- Polymeric light emitting diodes (PLED) --- p.7 / Chapter 1.2.1 --- Invention Polymeric light emitting diodes (PLED) --- p.7 / Chapter 1.2.2 --- Electric structure of PLEDs --- p.7 / Chapter 1.2.3 --- Transition from excitons to photons --- p.8 / Chapter 1.2.4 --- Controlling electron and hole injection --- p.8 / Chapter 1.2.5 --- Application of PEDT-PSS as hole transporting layer in PLED --- p.9 / Chapter 1.2.6 --- "Phase separating in PEDT-PSS blend, removing the PSS rich layer" --- p.9 / Chapter 1.3 --- Motivations of the thesis work --- p.10 / References --- p.10 / Chapter CHAPTER 2 --- INSTRUMENTATION --- p.27 / Chapter 2.1 --- X-ray Photoelectron Spectroscopy --- p.27 / Chapter 2.1.1 --- History of XPS techniques --- p.27 / Chapter 2.1.2 --- Physical Basis --- p.28 / Chapter 2.1.3 --- Chemical Shift of Binding Energy in XPS --- p.29 / Chapter 2.1.4 --- Binding Energy Referencing in XPS --- p.29 / Chapter 2.1.5 --- Sampling Depth of XPS --- p.30 / Chapter 2.1.6 --- Instrumental Setup of XPS --- p.30 / Chapter 2.2 --- Scanning Probe Microscopy --- p.31 / Chapter 2.2.1 --- Introduction --- p.31 / Chapter 2.2.2 --- Atomic Force Microscopy and Conductive Atomic Force Microscopy --- p.31 / Chapter 2.2.3 --- Instrumental Setup for Conductive AFM --- p.32 / Chapter 2.3 --- The Low Energy Ion Beam (LEIB) system at CUHK --- p.32 / Chapter 2.3.1 --- Introduction --- p.32 / Chapter 2.3.2 --- Principle --- p.33 / Chapter 2.3.3 --- Instrumentation Setup --- p.33 / References --- p.33 / Chapter CHAPTER 3 --- Effects of Ar+ bombardment at 500 and 100eV --- p.42 / Chapter 3.1 --- Introduction --- p.42 / Chapter 3.2 --- Sample Preparation --- p.42 / Chapter 3.3 --- Ar+ sputtering and XPS measurement of the sputtered sample. --- p.43 / Chapter 3.4 --- Results and Discussion --- p.44 / References --- p.49 / Chapter CHAPTER 4 --- Effects of annealing on PEDT-PSS thin films studied by XPS and AFM --- p.60 / Chapter 4.1 --- Introduction --- p.60 / Chapter 4.2 --- Sample Preparation --- p.60 / Chapter 4.3 --- XPS measurements and results --- p.61 / Chapter 4.3.1 --- XPS of C 1s core level of PEDT-PSS --- p.61 / Chapter 4.3.2 --- XPS of O 1s core level of PEDT-PSS --- p.62 / Chapter 4.3.3 --- XPS of S 2p core level of PEDT-PSS --- p.62 / Chapter 4.3.4 --- XPS of Valence Band of PEDT-PSS --- p.64 / Chapter 4.4 --- C-AFM measurements and results --- p.65 / Chapter 4.4.1 --- C-AFM measurements on PEDT-PSS --- p.65 / Chapter 4.5 --- Measurements and results about film insolubility and conductivity --- p.65 / Chapter 4.5.1 --- Insolubility measurements --- p.66 / Chapter 4.5.2 --- Conductivity measurements --- p.66 / Chapter 4.5.3 --- Results from the film insolubility and conductivity measurements --- p.66 / Chapter 4.6 --- Conclusion --- p.67 / References --- p.68 / Chapter CHAPTER 5 --- Effects of low energy proton bombardment of PEDT-PSS films studied by XPS and AFM --- p.90 / Chapter 5.1 --- Introduction --- p.90 / Chapter 5.2 --- XPS and c-AFM studies of PEDT-PSS films bombarded by H+ --- p.90 / Chapter 5.2.1 --- Sample preparation --- p.90 / Chapter 5.2.2 --- Results and discussion --- p.90 / Chapter 5.3 --- Conductivity measurements --- p.92 / Chapter 5.3.1 --- Sample preparation for conductivity measurements --- p.92 / Chapter 5.3.2 --- Results and discussion --- p.93 / Chapter 5.4 --- Conclusion --- p.93 / References --- p.93 / Chapter CHAPTER 6 --- Concluding Remarks and Future Works --- p.106 / Chapter 6.1 --- Concluding Remarks --- p.106 / Chapter 6.2 --- Future Work --- p.106 / Chapter APPENDIX --- The SSH model in describing polyacetylene --- p.108 / Chapter Part 1 --- Assumptions of the SSH model --- p.108 / Chapter Part 2 --- Bloch model and SSH model. --- p.113 / Reference --- p.117

>Magister Scientiae - MSc / Solar cells offer SA an additional energy source. While Si cells are abundantly available they are not at an optimal efficiency and the cost is still high. One technology that can enhance their performance is SiNW. However, material properties such as the diameter, porosity and length determine their effectiveness during application to solar cell technology. One method of growing SiNW uses Sn catalysts on a Si substrate. As the properties of the Sn nanoparticle govern the properties of the SiNW, this thesis investigates their formation and properties by depositing a Sn layer on a Si wafer and then subjecting it to different temperatures, during process the layer forms into nanoparticles. At each temperature the morphology, composition and crystallinity will be determined using XPS, SEM, TEM and EDS. Thus, in Chapter 1 there is an overview, Chapter 2 deals with techniques used in this study, Chapter 3 will give the quantitative and qualitative results on the XPS analysis and Chapter 4 will illustrate the structural behaviour of the annealed Sn film samples.

<p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>M-DNA is a novel complex formed between DNA and transition metal ions under alkaline conditions.<span style='mso-spacerun:yes'>  </span>The unique properties of M-DNA were manipulated in order to rationally place metal ions at specific regions within a double-stranded DNA helix.<span style='mso-spacerun:yes'>   </span>Investigations using thermal denaturation profiles and the ethidium fluorescence assay illustrate that the pH at which M-DNA formation occurs is influenced heavily by the DNA sequence and base composition.<span style='mso-spacerun:yes'>  </span>For instance, DNA with a sequence consisting of poly[d(TG)d(CA)] is completely converted to M-DNA at pH 7.9 while DNA consisting entirely of poly[d(AT)] remains in the B-DNA conformation until a pH of 8.6 is reached.<span style='mso-spacerun:yes'>  </span>The pH at which M-DNA formation occurs is further decreased by the incorporation of 4-thiothymine (s⁴T).<span style='mso-spacerun:yes'>  </span>DNA oligomers with a mixed sequence composed of </span>half d(AT) and the other half d(TG)d(CA)<span style='mso-bidi-font-weight: bold'> showed that only 50% of the DNA is able to incorporate Zn²⁺ ions at pH 7.9.<span style='mso-spacerun:yes'>  </span>This suggests that only regions corresponding to the tracts of <span class=GramE>d(</span>TG)d(CA) are being transformed.<span style='mso-spacerun:yes'>   </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-fareast-language:ZH-CN'>Duplex DNA monolayers were self-assembled on gold through <span class=GramE>a</span> Au-S linkage and both B- and M-DNA conformations were studied using X-ray photoelectron spectroscopy (XPS) in order to better elucidate the location of the metal ions.<span style='mso-spacerun:yes'>  </span>The film thickness, density, elemental composition and ratios for samples were analyzed and compared.<span style='mso-spacerun:yes'>  </span>The DNA surface coverage, calculated from both XPS and electrochemical measurements, was <span class=GramE>approximately 1.2 x 10¹³molecules/cm²</span>for B-DNA.<span style='mso-spacerun:yes'>  </span>All samples showed distinct peaks for C 1s, O 1s, N 1s, P 2p and S 2p as expected for a thiol-linked DNA.<span style='mso-spacerun:yes'>  </span></span><span style='mso-bidi-font-weight: bold'>On addition of Zn²⁺ to form M-DNA the C 1s, P 2p and S 2p showed only small changes </span><span style='mso-fareast-language:ZH-CN'>while both the N 1s and O 1s spectra changed considerably.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ interacting with oxygen on the phosphate backbone as well as replacing the imino protons of thymine (T) and guanine (G) in M-DNA.<span style='mso-spacerun:yes'>   </span>Analysis of the Zn 2p spectra also demonstrated that the concentration of Zn²⁺ present under M-DNA conditions is consistent with Zn²⁺ binding to both the phosphate backbone as well as replacing the imino protons of T or G in each base pair.<span style='mso-spacerun:yes'>  </span>After the M-DNA monolayer is washed with a buffer containing only Na⁺ the Zn²⁺ bound to the phosphate backbone is removed while the Zn²⁺ bound internally still remains. </span><span style='mso-bidi-font-weight:bold'>Variable angle x-ray photoelectron spectroscopy (VAXPS) was also used to examine monolayers consisting of mixed sequence oligomers.<span style='mso-spacerun:yes'>  </span>Preliminary results suggest that under M-DNA conditions, the zinc to phosphate ratio changes relative to the position of the <span class=GramE>d(</span>TG)d(CA) tract being at the top or bottom of the monolayer.<span style='mso-spacerun:yes'>  </span><span style='mso-spacerun:yes'> </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>Electrochemistry was also used to investigate the properties of M-DNA monolayers on gold and examine how the localization of metal ions affects the resistance through the DNA monolayer.<span style='mso-spacerun:yes'>  </span>T</span>he effectiveness of using the IrCl₆^2-/3-redox couple to investigate DNA monolayers and the potential advantages of this system over the standard Fe(CN)₆^3-/4- redox couple are demonstrated.<span style='mso-spacerun:yes'>  </span>B-DNA monolayers were converted to M-DNA by incubation in buffer containing 0.4 mM Zn²⁺ at pH 8.6 and studied by cyclic voltammetry (CV), electrochemical impedance spectroscopy (EIS) and chronoamperometry (CA) with IrCl₆^2-/3-.<span style='mso-spacerun:yes'>  </span>^{<span style='mso-spacerun:yes'> </span>}Compared to B-DNA, M-DNA showed significant changes in CV, EIS and CA spectra.<span style='mso-spacerun:yes'>  </span>However, only small changes were observed when the monolayers were incubated in Mg²⁺at pH 8.6 or in Zn²⁺ at pH 6.0.<span style='mso-spacerun:yes'>  </span>The heterogeneous electron-transfer rate (<i style='mso-bidi-font-style:normal'>k</i>_ET) between the redox probe and the surface of a bare gold electrode was determined to be 5.7 x 10^-3 cm/s.<span style='mso-spacerun:yes'>  </span>For a B-DNA modified electrode, the <i style='mso-bidi-font-style:normal'>k</i>_ET through the monolayer was too slow to be measured.<span style='mso-spacerun:yes'>  </span>However, under M-DNA conditions, a <i style='mso-bidi-font-style:normal'>k</i>_ET of 1.5 x 10^-3 cm/s was reached.<span style='mso-spacerun:yes'>  </span>As well, the percent change in resistance to charge transfer (R_CT), measured by EIS, <span class=GramE>was</span> used to illustrate the dependence of M-DNA formation on pH.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ ions replacing the imino protons on thymine and guanine residues.<span style='mso-spacerun:yes'>  </span>Also, at low pH values, the percent change in R_CT seems to be greater for <span class=GramE><span style='mso-bidi-font-weight:bold'>d(</span></span><span style='mso-bidi-font-weight: bold'>TG)₁₅d(CA)₁₅ compared to oligomers with mixed d(AT) and d(TG)d(CA) tracts.<span style='mso-spacerun:yes'>  </span></span>The IrCl₆^2-/3-redox couple was also effective in differentiating between single-stranded and double-stranded DNA during dehybridization and rehybridization experiments.<span style='mso-spacerun:yes'>  </span><span style='mso-bidi-font-weight:bold'><o:p></o:p></span></p>

<p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>M-DNA is a novel complex formed between DNA and transition metal ions under alkaline conditions.<span style='mso-spacerun:yes'>  </span>The unique properties of M-DNA were manipulated in order to rationally place metal ions at specific regions within a double-stranded DNA helix.<span style='mso-spacerun:yes'>   </span>Investigations using thermal denaturation profiles and the ethidium fluorescence assay illustrate that the pH at which M-DNA formation occurs is influenced heavily by the DNA sequence and base composition.<span style='mso-spacerun:yes'>  </span>For instance, DNA with a sequence consisting of poly[d(TG)d(CA)] is completely converted to M-DNA at pH 7.9 while DNA consisting entirely of poly[d(AT)] remains in the B-DNA conformation until a pH of 8.6 is reached.<span style='mso-spacerun:yes'>  </span>The pH at which M-DNA formation occurs is further decreased by the incorporation of 4-thiothymine (s⁴T).<span style='mso-spacerun:yes'>  </span>DNA oligomers with a mixed sequence composed of </span>half d(AT) and the other half d(TG)d(CA)<span style='mso-bidi-font-weight: bold'> showed that only 50% of the DNA is able to incorporate Zn²⁺ ions at pH 7.9.<span style='mso-spacerun:yes'>  </span>This suggests that only regions corresponding to the tracts of <span class=GramE>d(</span>TG)d(CA) are being transformed.<span style='mso-spacerun:yes'>   </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-fareast-language:ZH-CN'>Duplex DNA monolayers were self-assembled on gold through <span class=GramE>a</span> Au-S linkage and both B- and M-DNA conformations were studied using X-ray photoelectron spectroscopy (XPS) in order to better elucidate the location of the metal ions.<span style='mso-spacerun:yes'>  </span>The film thickness, density, elemental composition and ratios for samples were analyzed and compared.<span style='mso-spacerun:yes'>  </span>The DNA surface coverage, calculated from both XPS and electrochemical measurements, was <span class=GramE>approximately 1.2 x 10¹³molecules/cm²</span>for B-DNA.<span style='mso-spacerun:yes'>  </span>All samples showed distinct peaks for C 1s, O 1s, N 1s, P 2p and S 2p as expected for a thiol-linked DNA.<span style='mso-spacerun:yes'>  </span></span><span style='mso-bidi-font-weight: bold'>On addition of Zn²⁺ to form M-DNA the C 1s, P 2p and S 2p showed only small changes </span><span style='mso-fareast-language:ZH-CN'>while both the N 1s and O 1s spectra changed considerably.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ interacting with oxygen on the phosphate backbone as well as replacing the imino protons of thymine (T) and guanine (G) in M-DNA.<span style='mso-spacerun:yes'>   </span>Analysis of the Zn 2p spectra also demonstrated that the concentration of Zn²⁺ present under M-DNA conditions is consistent with Zn²⁺ binding to both the phosphate backbone as well as replacing the imino protons of T or G in each base pair.<span style='mso-spacerun:yes'>  </span>After the M-DNA monolayer is washed with a buffer containing only Na⁺ the Zn²⁺ bound to the phosphate backbone is removed while the Zn²⁺ bound internally still remains. </span><span style='mso-bidi-font-weight:bold'>Variable angle x-ray photoelectron spectroscopy (VAXPS) was also used to examine monolayers consisting of mixed sequence oligomers.<span style='mso-spacerun:yes'>  </span>Preliminary results suggest that under M-DNA conditions, the zinc to phosphate ratio changes relative to the position of the <span class=GramE>d(</span>TG)d(CA) tract being at the top or bottom of the monolayer.<span style='mso-spacerun:yes'>  </span><span style='mso-spacerun:yes'> </span><o:p></o:p></span></p> <p class=MsoNormal style='text-align:justify;text-indent:.5in;line-height:150%'><span style='mso-bidi-font-weight:bold'>Electrochemistry was also used to investigate the properties of M-DNA monolayers on gold and examine how the localization of metal ions affects the resistance through the DNA monolayer.<span style='mso-spacerun:yes'>  </span>T</span>he effectiveness of using the IrCl₆^2-/3-redox couple to investigate DNA monolayers and the potential advantages of this system over the standard Fe(CN)₆^3-/4- redox couple are demonstrated.<span style='mso-spacerun:yes'>  </span>B-DNA monolayers were converted to M-DNA by incubation in buffer containing 0.4 mM Zn²⁺ at pH 8.6 and studied by cyclic voltammetry (CV), electrochemical impedance spectroscopy (EIS) and chronoamperometry (CA) with IrCl₆^2-/3-.<span style='mso-spacerun:yes'>  </span>^{<span style='mso-spacerun:yes'> </span>}Compared to B-DNA, M-DNA showed significant changes in CV, EIS and CA spectra.<span style='mso-spacerun:yes'>  </span>However, only small changes were observed when the monolayers were incubated in Mg²⁺at pH 8.6 or in Zn²⁺ at pH 6.0.<span style='mso-spacerun:yes'>  </span>The heterogeneous electron-transfer rate (<i style='mso-bidi-font-style:normal'>k</i>_ET) between the redox probe and the surface of a bare gold electrode was determined to be 5.7 x 10^-3 cm/s.<span style='mso-spacerun:yes'>  </span>For a B-DNA modified electrode, the <i style='mso-bidi-font-style:normal'>k</i>_ET through the monolayer was too slow to be measured.<span style='mso-spacerun:yes'>  </span>However, under M-DNA conditions, a <i style='mso-bidi-font-style:normal'>k</i>_ET of 1.5 x 10^-3 cm/s was reached.<span style='mso-spacerun:yes'>  </span>As well, the percent change in resistance to charge transfer (R_CT), measured by EIS, <span class=GramE>was</span> used to illustrate the dependence of M-DNA formation on pH.<span style='mso-spacerun:yes'>  </span>This result is consistent with Zn²⁺ ions replacing the imino protons on thymine and guanine residues.<span style='mso-spacerun:yes'>  </span>Also, at low pH values, the percent change in R_CT seems to be greater for <span class=GramE><span style='mso-bidi-font-weight:bold'>d(</span></span><span style='mso-bidi-font-weight: bold'>TG)₁₅d(CA)₁₅ compared to oligomers with mixed d(AT) and d(TG)d(CA) tracts.<span style='mso-spacerun:yes'>  </span></span>The IrCl₆^2-/3-redox couple was also effective in differentiating between single-stranded and double-stranded DNA during dehybridization and rehybridization experiments.<span style='mso-spacerun:yes'>  </span><span style='mso-bidi-font-weight:bold'><o:p></o:p></span></p>

Although silicon (Si) nanostructures exhibit size dependent light emission, which can be attributed to quantum confinement, the role of surface passivation is not yet fully understood. This understanding is central to the development of nanocrystal-based detectors. This study investigated the growth, surface chemistry, passivation with deuterium (D2), ammonia (ND3) and diborane (B2D6) and the resulting optical properties of Si nanostructures. Si nanocrystals less than 6 nm in diameter are grown on SiO2 surfaces in an ultra high vacuum chamber using hot-wire chemical vapor deposition and the as grown surfaces are exposed to atomic deuterium. Temperature programmed desorption (TPD) spectra show that that the nanocrystals surfaces are covered by a mix of monodeuteride, dideuteride and trideuteride species. The manner of filling of the deuteride states on nanocrystals differs from that for extended surfaces as the formation of the dideuteride and trideuteride species is facilitated by the curvature of the nanocrystal. No photoluminescence (PL) is observed from the as grown unpassivated nanocrystals. As the deuterium dose is increased, the PL intensity also begins to increase. This can be associated with increasing amounts of mono-, di- and trideuteride species on the nanocrystal surface, which results in better passivation of the dangling bonds and relaxing of the reconstructed surface. At high deuterium doses, the surface structure breaks down and amorphization of the top layer of the nanocrystal takes place. Amorphization reduces the PL intensity. Finally, as the nanocrystal size is varied, the PL peak shifts, which is characteristic of quantum confinement. The dangling bonds and the reconstructed bonds at the NC surface are also passivated and transformed with D and NDx by using deuterated ammonia (ND3), which is predissociated over a hot tungsten filament prior to adsorption. At low hot wire ND3 doses PL emission is observed at 1000 nm corresponding to reconstructed surface bonds capped by predominantly monodeuteride and Si-ND2 species. As the hot wire ND3 dose is increased, di- and trideuteride species form and intense PL is observed around 800 nm that does not shift with NC size and is associated with defect levels resulting from NDx insertion into the strained Si-Si bonds forming Si2=ND. The PL intensity at 800 nm increases as the ND3 dose is increased and the intensity increase is correlated to increasing concentrations of deuterides. At extremely high ND3 doses PL intensity decreases due to amorphization of the NC surface. In separate experiments, Si NCs were subjected to dissociative (thermal) exposures of ammonia followed by exposures to atomic deuterium. These NCs exhibited size dependent PL and this can be attributed to the prevention of the formation of Si2=ND species. Finally, deuterium-passivated Si NCs are exposed to BDx radicals formed by dissociating deuterated diborane (B2D6) over a hot tungsten filament and photoluminescence quenching is observed. Temperature programmed desorption spectra reveal the presence of low temperature peaks, which can be attributed to deuterium desorption from surface Si atoms bonded to subsurface boron atoms. The subsurface boron likely enhances nonradiative Auger recombination. / text

This work describes the synthesis of dendrimer-encapsulated nanoparticles (DENs) and the expansion of the characterization ability for these materials. The dendrimer-template method for the synthesis of nanoparticles allows precise control over the size, composition and structure of nanoparticles in the 40-250 atom range. In this size regime, the surface structure of the nanoparticles dominates their catalytic properties. The long term goal of this research is to correlate the structure of these nanoparticles to their catalytic activity, improving the ability to predict superior catalysts a priori. As a prerequisite for this analysis, the precise structure of the catalytically active nanoparticle must be determined. Characterization of nanoparticles in the 1-2 nm region is significantly more difficult than more commonly used nanoparticles of 3-5 nm diameter or larger. Typical characterization of these nanoparticles involves UV-vis spectroscopy for Mie absorbance and transmission electron microscopy for size analysis. This work involves the use of extended X-ray absorption-fine structure (EXAFS) to determine the local structure of the nanoparticles. For monometallic Pt DENs, EXAFS was combined with UV-vis, TEM, X-ray photoelectron spectroscopy (XPS) and electrochemistry to determine that the Pt system is not simply nanoparticles but a more complex, bimodal state. EXAFS has also been used to differentiate between different bimetallic structures. For PdAu DENs, there are two synthetic methods used. When both metals are reduced simultaneously, the resulting nanoparticles have a quasi-random alloy structure. These nanoparticles were then extracted from the dendrimer into an organic solvent by use of alkanethiols. The extraction process changed the alloy structure into Au-core/Pd-shell. When Pd and Au were reduced in sequence, the DENs were formed as a Au-core/Pd-shell material, regardless of the order of the reduction of the metals. The Au-core/Pd-shell structure was also present after extraction. In addition to structural analysis to determine the result of different synthetic methods, EXAFS was also used in situ to measure the structure of Pt DENs during the oxidation of absorbed CO. These in situ measurements are important for determining the structure of the actual catalyst rather than the precursor nanoparticle. In this case, the Pt DENs changed from a bimodal distribution into fully reduced nanoparticles by the application of a reducing potential. The binding of CO to the Pt DENs and subsequent oxidation did not cause measurable agglomeration of the nanoparticles. This reduction of the Pt system by electrochemical means was also explored as a synthetic method. The Pt-dendrimer complex was placed on a TEM grid for electrochemical treatment. A potential step was shown to reduce some of the Pt-dendrimer complexes into Pt nanoparticles of the expected size. However, most of the complexes were not reduced. Therefore, only the standard chemical reduction followed by electrochemical treatment is sufficient to fully reduce the nanoparticle samples. This work has explored additional synthetic methods for the synthesis of monometallic and bimetallic DENs. The use of EXAFS, as well as other advanced characterization techniques, has advanced knowledge of the structure of various DENs. Both the characterization toolset and the synthetic methods will provide a basis for investigations of catalytically active materials. / text

Στην παρούσα διπλωματική εργασία αναλύονται λεπτά υμένια (thin films) διαφόρων πολυμερικών ή ολιγομερών οργανικών ενώσεων, με την επεξεργασία μετρήσεων που είχαν ληφθεί με την επιφανειακά ευαίσθητη τεχνική της φασματοσκοπίας φωτοηλεκτρονίων από ακτίνες Χ (XPS). Από την ανάλυση των φασμάτων XPS προκύπτουν συμπεράσματα τόσο για την παρουσία συγκεκριμένων χημικών στοιχείων στα δείγματα (ποιοτική ανάλυση) όσο και για την συγκέντρωση των στοιχείων αυτών στην περιοχή ανάλυσης (ποσοτική ανάλυση). / This thesis analyzed thin films (thin films) various polymeric or oligomeric organic compounds, the processing of measurements taken with the surface sensitive technique of spectroscopy X-ray photoelectron (XPS). From the analysis of XPS spectra resulting conclusions as to the presence of certain chemical elements in samples (qualitative analysis) and for the concentration of these elements in the analysis (quantitative analysis).

The mechanism by which chiral selectivity takes place is complicated by the surface morphology, the possible involvement of the solvent, and the characteristics of the chiral molecules at the surface. My goal is to model and understand the factors which lead to significant discrimination in the case of three closely related chiral stationary phases: N-(1-phenylethyl)-N’-[3-(triethoxysilyl)propyl]-urea (PEPU), [(3,5-dinitrobenzoyl)-amino]-N-[3-(triethoxysilyl)propyl]-2-phenylacetamide (DNB-phenyglycine), and [(3,5-dinitrobenzoyl)amino]-N-[3-(triethoxysilyl)propyl]-4-methylpentanamide (DNB-leucine). Ab initio calculations are used to develop molecular models of these chiral selectors. These models are employed in molecular dynamics (MD) simulations, which provide the theoretical framework for modelling chiral interfaces in different solvent mixtures. The MD simulations of PEPU interfaces show that, in alcohol/water mixtures, the alcohols form domains at the interface with the hydrophobic portions of the molecule tending to orient towards the surface. This disrupts the water hydrogen bonding networks at the interface and leads to the exclusion of water from the surface region relative to the bulk. The MD simulations of DNB-phenylglycine and DNB-leucine selectors in hexane/2-propanol mixtures demonstrate that the interfaces are distinct both in terms of the selector orientations at the surface and in the number of hydrogen bonds formed with 2-propanol. This occurs despite the structural similarity between these two selectors. The interfaces are also prepared experimentally by attaching the chiral selectors onto oxidized Si(111) samples and AFM tips. In particular, for DNB-phenylglycine and DNB-leucine samples, two synthetic routes have been explored. Using AFM, the morphologies of the resulting chiral interfaces are obtained. X-ray photoelectron spectroscopy and refraction-absorption infrared spectroscopy provide information regarding the relative distribution of the compounds on the surface. Using chemical force microscopy (CFM) measurements, chiral self-selectivity is examined in various solvent mixtures. For PEPU interfaces, the extent of hydrogen bonding at the surface is the dominant contributor to the measured forces. In the case of DNB-phenylglycine and DNB-leucine, CFM measurements of the chiral self-selectivity in 2-propanol demonstrate that chiral discrimination is present in both systems, but larger forces are observed for DNB-phenylglycine, consistent with the molecular dynamics study that shows much weaker solvent interactions with this species. / Thesis (Ph.D, Chemistry) -- Queen's University, 2008-08-14 11:26:37.436

Darbo tikslas yra ištirti etaloninių vanadžio pentoksido ir dioksido Rentgeno fotoelektronų spektrus siekiant nustatyti cheminį poslinkį tarp oksidų V 2p spektrų smailių. Darbe išsamiai aprašytos vanadžio dioksido ir prntoksido struktūros, oksidų savybės, Rentgeno fotoelektronų spektroskopijos metodo pagrindai bei V2O5 ir VO2 Rentgeno fotoelektronų spektrų ypatumai. Aprašyti atliktų eksperimentų metodai. Pateikti eksperimentų ir literatūrinės duomenų bazės analizės rezultatai. Atliktas darbas leido nustatyti sekančius faktus: cheminis poslinkis tarp vanadžio dioksido ir pentoksido etaloninių bandinių Rentgeno fotoelektronų spektrų V 2p3/2 smailių lygus 0.7 eV matuojant spektrus spektrometru XSAM 800 (Kratos Analytical, Anglija); literatūrinių duomenų analizę parodė, kad tikimiausia cheminio poslinkio vertė tarp V 2p3/2 smailių įvairiuose vanadžio junginiuose lygi 1.1 eV; skirtumas tarp eksperimentiškai gautos cheminio poslinkio vertės ir analogiško dydžio gauto iš literatūrinių duomenų analizės sąlygotas tuo, kad buvo matuojami gryni VO2 ir V2O5 bandiniai, o analizei buvo naudojama duomenų visumą apie įvairius vanadžio junginius. / The main aim of the presented work was to investigate the chemical shift between XPS V 2p peaks of standard V2O5 and VO2 samples. The structure and physical properties of vanadium dioxide and pentoxide, X-ray photoelectron spectroscopy basis and some singularities of these oxides XPS spectra are presented. The experimental methods, the results of experiments and the literature analysis results are described. The executed work has allowed establishing following facts: the chemical shift between vanadium dioxide and pentoxide standard samples XPS V 2p peaks is equal to 0.7 eV; the analysis of the literature base shows that this shift for various vanadium compounds is 1.1 eV; the difference between measured chemical shift and chemical shift value established from literature analysis is caused because XPS spectra of pure oxides samples was measured in present work and the analysis of the literature base was performed for various vanadium compounds.

No description available.