The purpose of this dissertation is to advance the understanding of SrS-based a. c. thin film electroluminescent (ACTFEL) devices. The role of traps in the bulk phosphor layer in the light emission mechanism from ACTFEL devices is studied, characterized and modeled. Experiments were performed to observe the response of the ACTFEL devices to tailored voltage excitations. A physical model was developed to describe the optoelectronic processes taking place in the phosphor; analytical equations were written and numerically simulated to plot the flux and luminance responses of the device to similarly tailored voltage excitations. The voltage excitation parameters such as amplitude, rise times and fall times were varied both experimentally and in simulations and their effect on the opto-electronic response of the device was studied. Thermally stimulated luminance studies were performed to determine critical device parameters. Theoretical predictions matched the experimental data in a qualitative manner. A much improved quantitative accuracy is obtained when the role of dipoles in the EL mechanisms is incorporated into the model.

Medidas de corrente termoestimuladas e de carga a temperatura constante, sob campo elétrico constante externo, foram realizadas no intuito de identificar além de cargas espaciais existentes em amostras comerciais de PVDF, também estudar o pico anômolo de corrente que se apresentou nas medidas isotérmicas. Este pico desaparecia em medidas subseqüentes, mas sua recuperação, apesar de lenta, foi registrada, principalmente se a amostra era conservada em ambiente úmido. Uma série de medidas feitas em diferentes umidades relativas do ar, cuidadosamente controladas, evidenciou que este fenômeno estava diretamente ligado à água absorvida pela amostra do ambiente externo. O efeito mostrou também ser fortemente dependente do campo aplicado. Um modelo baseado em dissociação iônica da água, provavelmente fracamente ligada a estrutura do polímero, foi desenvolvido, levando em consideração que o coeficiente de dissociação depende do campo elétrico, bem como do tempo de extração dos portadores dissociados da amostra. Nesta cinética controladora da corrente, é considerada também recombinação bi-iônica. / Thermally stimulated current and depolarization measurements were carried on commercially available samples of PVDF. The measurements were conducted under constant temperature and constant applied field in order to investigate an anomolous peak which appears in isothermal measurements, and also identify the presence of space charge. This peak is observed only in the first measurements, but it can recover if the sample is stored in a humid environment. Series of measurements was carried out with carefully controlled relative humidity from which one can conclude that the peak is directly linked to water absorved by the sample. This effect is shown to depend strongly on the applied electric field. A theoretical model based on ionic dissociation of water molecules - probably weakly attached to the polymer structure is developed to explain the experimental results. In the model, the dissociation coefficient and the time of escape of dissociated carriers are assumed to depend on the electric field. Bi-ionic recombination is also assumed to play an important role in the control of the kinetics of the process.

Medidas de corrente termoestimuladas e de carga a temperatura constante, sob campo elétrico constante externo, foram realizadas no intuito de identificar além de cargas espaciais existentes em amostras comerciais de PVDF, também estudar o pico anômolo de corrente que se apresentou nas medidas isotérmicas. Este pico desaparecia em medidas subseqüentes, mas sua recuperação, apesar de lenta, foi registrada, principalmente se a amostra era conservada em ambiente úmido. Uma série de medidas feitas em diferentes umidades relativas do ar, cuidadosamente controladas, evidenciou que este fenômeno estava diretamente ligado à água absorvida pela amostra do ambiente externo. O efeito mostrou também ser fortemente dependente do campo aplicado. Um modelo baseado em dissociação iônica da água, provavelmente fracamente ligada a estrutura do polímero, foi desenvolvido, levando em consideração que o coeficiente de dissociação depende do campo elétrico, bem como do tempo de extração dos portadores dissociados da amostra. Nesta cinética controladora da corrente, é considerada também recombinação bi-iônica. / Thermally stimulated current and depolarization measurements were carried on commercially available samples of PVDF. The measurements were conducted under constant temperature and constant applied field in order to investigate an anomolous peak which appears in isothermal measurements, and also identify the presence of space charge. This peak is observed only in the first measurements, but it can recover if the sample is stored in a humid environment. Series of measurements was carried out with carefully controlled relative humidity from which one can conclude that the peak is directly linked to water absorved by the sample. This effect is shown to depend strongly on the applied electric field. A theoretical model based on ionic dissociation of water molecules - probably weakly attached to the polymer structure is developed to explain the experimental results. In the model, the dissociation coefficient and the time of escape of dissociated carriers are assumed to depend on the electric field. Bi-ionic recombination is also assumed to play an important role in the control of the kinetics of the process.

This thesis describes firstly, a study involving the thermal rearrangement of substituted 6-e̲x̲o̲-(1-alkenyl) bicyclo-[3.1.0]hexenes, and secondly, the application of this type of transformation to a total synthesis of (±)-sinularene (1̲2̲5̲). The 6-e̲x̲o̲-(1-alkenyl)bicyclo[3.1.0]hexenes (1̲8̲7̲, 1̲8̲9̲, 1̲9̲2̲, 1̲9̲4̲, 2̲4̲0̲, 2̲7̲4̲ and 340) were prepared and thermolyzed in sealed tubes to afford the corresponding bicyclo[3.2.1]octa-2,6-dienes (1̲8̲8̲, 1̲9̲0̲, 1̲9̲3̲, 1̲9̲5̲, 2̲4̲1̲, 2̲7̲6̲ and 3̲4̲1̲) in generally excellent yields. With the exception of 1̲9̲0̲, the thermolysis products were subjected to acid-catalyzed hydrolysis to give the respective bicyclo[3.2.1]octenones. From this study, it is clear that a) the Cope rearrangement of substrates, such as 2̲7̲4̲ and 3̲4̲0̲, containing even sterically bulky substituents on the 6-alkenyl side chain presents a viable means of generating functionalized bicyclo [ 3.2.1] octa-2 , 6-dienes, b) this methodology provides for the placement of synthetically useful functionalities on any of the carbon bridges of the bicyclo-[3.2.1]octane skeleton, and c) the transformations 2̲4̲0̲→2̲4̲1̲ and 2̲7̲4̲→2̲7̲6̲ provide strong evidence for the stereospecificity of the rearrangement process. In the total synthesis of (±)-sinularene (1̲2̲5̲), the key step involved the thermal rearrangement of 3̲2̲2̲ to afford the bicyclo[3.2.1]octadiene 3̲2̲1̲. The compound 3̲2̲2̲̲ was readily prepared as follows. 1-Lithio-3-methyl-1-butyne was treated with methacrolein to furnish the allylic alcohol 3̲3̲1̲, which was transformed into the ester 3̲3̲2̲ v̲i̲a̲ an orthoester Claisen rearrangement (hot triethyl .orthoacetate, propionic acid). Hydrolysis of the ester 3̲3̲2̲, followed by reaction of the resultant acid with oxalyl chloride in refluxing hexane gave the corresponding acid chloride 3̲3̲4̲. Treatment of 3̲3̲4̲ with a cold, ethereal solution of diazomethane afforded the diazo ketone 3̲3̲5̲, which in the presence of copper (II) acetoacetonate in refluxing benzene, underwent an intramolecular carbenoid cyclization to furnish the bicyclic ketone 3̲3̲6̲. Semihydrogenation of 3̲3̲6̲ using Lindlar’s catalyst gave stereoselectively the c̲i̲s̲-alkenyl ketone 3̲3̲7̲. The enone 3̲3̲8̲ was obtained by oxidizing the trimethylsilyl enol ether of 3̲3̲7̲ using palladium (II) acetate in acetonitrile. When the enone 3̲3̲8̲ was treated with lithium divinylcuprate, the two epimeric products 3̲3̲9̲ and 3̲4̲6̲ were obtained in a ratio of 9:1, respectively, and were sus-sequently separated by column chromatography. Trapping the lithium enolate of 3̲3̲9̲ with t̲-butyldimethylsilyl chloride led to the required enol ether 3̲3̲2̲. Thermolysis (220°C, sealed tube) of 3̲3̲2̲ in benzene produced exclusively in 86% yield the desired bicyclic triene 3̲2̲1̲. Subjection of 3̲2̲1̲ to hydroboration using disiamylborane gave, after oxidative workup, the alcohol 3̲4̲7̲, which on treatment with p̲-toluenesulfonyl chloride in the presence of 4-dimethylaminopyridine, afforded the ketone 3̲4̲9̲. Successive hydrogenation of 3̲4̲9̲ and Wittig olefination of the resultant ketone 2̲8̲0̲ completed the total synthesis of (±)-sinularene (1̲2̲5̲). [formula omitted] / Science, Faculty of / Chemistry, Department of / Graduate

TSDC (thermally stimulated depolarization current) is one of the most important and popular technique for investigating electret materials. TSDC technique can indicate the magnitude of polarization and depolarization, relaxation time, charge-storage, glass transition, and activation energy. To fully investigate polarization and relaxation for pure epoxy and filled epoxy materials, a TSDC system was built and verified by the research. The article describes the building processes and verification of the TSDC system. TSDC, TSPC, and TWC tests data for epoxy and filled epoxy samples are presented in the article. To compare TSDC technique with other related techniques, DEA (dielectric analysis), DMA (dynamic mechanical analysis), and DSC (differential scanning calorimetry) tests are introduced.

In den letzten Jahren ist eine Vielzahl neuer organischer Polymere und niedermolekularer Verbindungen synthetisiert worden, die sich als aktive Komponente für Elektrolumineszenz-Bauelemente und andere elektronische Anwendungen eignen. Trotz der großen technologischen Bedeutung und des erheblichen Fortschrittes, der bei der Herstellung solcher Materialien erzielt worden ist, sind grundlegende physikalische Eigenschaften dieser Materialklassen noch nicht ausreichend erforscht. Insbesondere das Auftreten lokalisierter Zustände innerhalb der Bandlücke hat besondere Bedeutung für ihre elektronischen Eigenschaften. Sowohl die Präsenz dieser flachen traps (Fallen, Löcher) als auch der Einfluß der Herstellungsbedingungen auf die tiefen und flachen lokalisierten Zustände wurden bisher nicht systematisch untersucht.<br /> Thermische Techniken sind wichtige Methoden, um lokalisierte Niveaus in organischen und anorganischen Materialien zu erforschen. Themisch-Stimulierte Lumineszenz (TSL), Thermisch-Stimulierte Ströme (TSC) und Thermisch-Stimulierte Depolarisierte Ströme (TSDC) ermöglichen die Untersuchung flacher und tiefer traps; in Verbindung mit DiElektrischer Spektroskopie (DES) können außerdem Polarisations- und Depolarisationseffekte studiert werden.<br /> Mit Hilfe numerischer Simulationen haben wir die kinetischen Gleichungen erster und zweiter Ordnung untersucht, die sich durch schwaches bzw. starkes Wieder-Fangen beschreiben lassen. In diesen Gleichungen haben wir Gaussian-, exponentielle und quasi-kontinuierliche Verteilungen von lokalisierten Zustände berücksichtigt. Durch Veränderung der beiden wichtigsten Parameter (Tiefe der traps E und Häufigkeit) konnte die Form der thermischen Maxima untersucht werden. Auch die die Gaussian-Verteilung bestimmenden Faktoren wurden verändert. <br /> Diese theoretischen Ergebnisse wurden auf die experimentellen Glow-Kurven angewandt. Dünne Filme aus polymeren und niedermolekularen Verbindungen (Polyphenylquinoxaline, Trisphenylquinoxaline und Oxadiazole), die wegen ihrer technologischen Bedeutung ausgewählt wurden, zeigen komplexes thermisches Verhalten.<br /> Insbesondere hoch geordnete Filme eines amphiphil substituierten 2-(p-nitrophenyl)-5-(p-undecylamidophenyl)-1,3,4-oxadiazols (NADPO) zeichnen sich durch komplexe TSL-Diagramme aus. Im Bereich von Em = 4 meV wurde eine Region flacher traps gefunden. Zwei weitere TSL-Maxima treten bei Tm = 221.5 K bzw. Tm = 254.2 K auf. Sie besitzen Aktivierungsenergien von Em= 0.63 eV bzw. Em = 0.66 eV, ihre Frequenzfaktoren betragen s = 2.4x1012 s-1 bzw. s = 1.85x1011 s-1, sie zeigen Breiten der Verteilung von s = 0.045 eV bzw. s = 0.088 eV. <br /> Des weiteren zeigt diese Arbeit, daß die Form der Glow-Kurven stark von der Anregungstemperatur und vom thermischen Kreislauf beeinflußt wird. / New polymers and low molecular compounds, suitable for organic light emitting devices and organic electronic applications, have been synthesised in this years in order to obtain electron transport characteristics compatible with requirements for applications in real plastic devices. However, despite of the technological importance and of the relevant progress in devices manufacture, fundamental physical properties of such class of materials are still not enough studied. In particular extensive presence of distributions of localised states inside the band gap has a deep impact on their electronic properties. Such presence of shallow traps as well as the influence of the sample preparation conditions on deep and shallow localised states have not been, until now, systematically explored.<br /> The thermal techniques are powerful tools in order to study localised levels in inorganic and organic materials. Thermally stimulated luminescence (TSL), thermally stimulated currents (TSC) and thermally stimulated depolarisation currents (TSDC) allow to deeply look to shallow and deep trap levels as well as they permit to study, in synergy with dielectric spectroscopy (DES), polarisation and depolarisation effects. <br /> We studied, by means of numerical simulations, the first and the second order kinetic equations characterised by negligible and strong re-trapping respectively. We included in the equations Gaussian, exponential and quasi-continuous distributions of localised states. The shapes of the theoretical peaks have been investigated by means of systematic variation of the two main parameters of the equations, i. e. the energy trap depth E and the frequency factor a and of the parameters regulating the distributions, in particular for a Gaussian distribution the distribution width s and the integration limits. <br /> The theoretical findings have been applied to experimental glow curves. Thin films of polymers and low molecular compounds. Polyphenylquinoxalines, trisphenylquinoxalines and oxadiazoles, studied because of their technological relevance, show complex thermograms, having several levels of localised states and depolarisation peaks. <br /> In particular well ordered films of an amphiphilic substituted 2-(p-nitrophenyl)-5-(p-undecylamidophenyl)-1,3,4-oxadiazole (NADPO) are characterised by rich TSL thermograms. A wide region of shallow traps, localised at Em = 4 meV, has been successfully fit by means of a first order kinetic equation having a Gaussian distribution of localised states. <br /> Two further peaks, having a different origin, have been characterised. The peaks at Tm = 221.5 K and Tm = 254.2 have activation energy of Em= 0.63 eV and Em = 0.66 eV, frequency factor s = 2.4x1012 s-1 and s = 1.85x1011 s-1, distribution width s = 0.045 eV and s = 0.088 eV respectively. <br /> Increasing the number of thermal cycle, a peak, probably connected with structural defects, appears at Tm = 197.7 K. The numerical analysis of this peak was performed by means of a first order equation containing a Gaussian distribution of traps. The activation energy of the trap level is centred at Em = 0.55 eV. The distribution is perfectly symmetric with a quite small width s = 0.028 eV. The frequency factor is s = 1.15 x 1012 s-1, resulting of the same order of magnitude of its neighbour peak at Tm = 221.5 K, having both, probably, the same origin.<br /> Furthermore the work demonstrates that the shape of the glow curves is strongly influenced by the excitation temperature and by the thermal cycles. For that reason Gaussian distributions of localised states can be confused with exponential distributions if the previous thermal history of the samples is not adequately considered.

In this thesis, in order to study the structural, optical and electrical transport properties of Tl2In2S3Se, TlInSeS and Tl2In2SSe3 crystals, X-ray diffraction (XRD), energy dispersive spectroscopic analysis (EDSA), transmission, reflection, photoluminescence (PL), thermally stimulated current (TSC) and photoconductivity decay (PC) measurements were carried out. Lattice parameters and atomic composition of these crystals were determined from XRD and EDSA experiments, respectively. By the help of transmission and reflection experiments, the room temperature absorption data were analyzed and it was revealed the coexistence of indirect and direct band gap energies of the studied crystals. Moreover, the refractive index dispersion parameters - oscillator energies, dispersion energies, oscillator strengths, oscillator wavelengths and zero-frequency refractive indexes were determined. Temperature-dependent transmission measurements made it possible to find the rate of change of indirect band gaps with temperature, absolute zero values of the band gap energies and Debye temperatures of these crystals. From the analysis of the transmission and reflection measurements, it was established that, there is a decrease in the values of indirect and direct band gaps energies and an increase in zero-frequency refractive indexes with increasing of selenium content. PL measurements were carried out to obtain the detailed information about recombination levels in crystals studied. The behavior of PL spectra were investigated as a function of laser excitation intensity and temperature. The variation of the spectra with laser excitation intensity and temperature suggested that the observed emission bands in these crystals were due to the donor-acceptor pair recombination. TSC measurements were carried out with various heating rates at different illumination temperatures to obtain information about trap levels in these crystals. The mean activation energies, attempt-to-escape frequencies, concentrations and capture cross sections of the traps were determined as a result of TSC spectra analysis. The analysis of experimental TSC curves registered at different light illumination temperatures revealed the exponential trap distribution in the studied crystals. From the analysis of PC measurements, carrier lifetimes were obtained.

A thorough study on the distribution of defect-related active energy levels has been performed on nanocrystalline TiO2. Films have been deposited on thick-alumina printed circuit boards equipped with electrical contacts, heater and temperature sensors, to carry out a detailed thermally stimulated currents analysis on a wide temperature range (5-630 K), in view to evidence contributions from shallow to deep energy levels within the gap. Data have been processed by numerically modelling electrical transport. The model considers both free and hopping contribution to conduction, a density of states characterized by an exponential tail of localized states below the conduction band and the convolution of standard Thermally Stimulated Currents (TSC) emissions with gaussian distributions to take into account the variability in energy due to local perturbations in the highly disordered network. Results show that in the low temperature range, up to 200 K, hopping within the exponential band tail represents the main contribution to electrical conduction. Above room temperature, electrical conduction is dominated by free carriers contribution and by emissions from deep energy levels, with a defect density ranging within 10(14)-10(18) cm(-3), associated with physio- and chemi-sorbed water vapour, OH groups and to oxygen vacancies.

Ametistas naturais brasileiras foram estudadas através das técnicas de Absorção Óptica (AO), Ressonância Paramagnética Eletrônica (RPE) e Corrente de Despolarização Termicamente Estimulada (CDTE).O espectro de AO apresentou três picos principais na região espectral do visível (10500, 18600 e 28200cm POT.-1) e um enorme pico na região do ultravioleta (45000cm POT.-1) atribuídos ao ferro em diferentes estados de valência. A presença de centros OH POT.- foi observada na região do infravermelho através das bandas em 3440 e 3580cm POT.-1. O espectro de RPE, operando na banda X, exibe um conjunto de linhas centrado em 2000G, um pico intenso em 3000G e quatro picos pequenos em 4000, 5000, 6000 e 7000G, quando o campo magnético encontra-se paralelo a um dos eixos cristalograficamente equivalentes. Quando o campo magnético encontra-se paralelo ao eixo c do cristal, o espectro de RPE revela um conjunto de linhas centrado em 2000G, dois picos intensos próximos a 5000G e um pico pequeno em 6800G. Amostras em pó apresentam uma banda larga centrada em 3400G. Tratamentos térmicos mostram uma redução gradativa desta banda com o aumento do tempo de tratamento térmico e uma redução mais rápida para temperaturas maiores. Sabe-se que os centros de cor nas ametistas são produzidos pela ação de radiação ionizante natural sobre os centros precursores que surgem da substituição do Si POT.4+ pelo Fe POT.3+ na estrutura do quartzo-alfa. Esses centros de Fe POT.3+ não se distribuem igualmente entre os sítios equivalentes no cristal natural e são responsáveis pelas características dominantes do espectro de RPE. O espectro de CDTE obtido da polarização de uma amostra em 1000V apresenta uma banda em 215K, que vem a ser a composição de três bandas de menor intensidade (185, 200 e 214K) e uma banda única em 260K. Foi confirmado o caráter dipolar dessas bandas. Tratamentos térmicos efetuados a diferentes temperaturas mostram ) um decaimento de área total e uma redução da intensidade das bandas mais acentuadas para temperaturas maiores. Iluminação ultravioleta restaura parcialmente o espectro de CDTE e demonstra o crescimento de uma banda na região da temperatura ambiente. Devido ao comportamento semelhante dos espectros de CDTE e de RPE, o sendo Fe POT.3+ um elemento presente em grande quantidade nas amostras estudadas, acredita-se que o centro de dipolo responsável pelas bandas de CDTE observadas, seja do Fe POT.3+ substituindo um Si POT.4+ próximo a um O POT.- ou a um OH POT.-, e que as diferentes posições dos picos devem-se à população desigual do Fe POT.3+ substitucional nos sítios cristalograficamente equivalentes do cristal. / Brazilian natural amethyst samples have been studied through Optical Absorption (AO), Electron Paramagnetic Resonance (EPR) and Thermally Stimulated Depolarization Current (TSDC) Techniques.The AO spectrum shows three main peaks in the visible region (10500, 18600 e 28200cm POT.-1) and a huge peak in the ultraviolet region (45000cm POT.-1). All these peaks were attributed to iron in different valence states. The presence of centros OH POT.- centres have been observed through the bands at 3440 e 3580cm POT.-1in the infrared.The EPR spectrum shows a set of lines centered at 2000G, an intense peak at 3000G and four small peaks at 4000, 5000, 6000 and 7000G, when the magnetic field is parallel to one of crystallographically equivalents sites. When the magnetic field is parallel to the crystal c-axis, the EPR spectrum shows a set of lines centered at 2000G, two high peaks near 5000G and a small peak at 6800G. Powder samples presents a broad band centered in 3400G. Thermal treatments reduce this band for increasing thermal treatments time intervals. The reduction increases for high temperatures. It is well known that colour centres in amethysts are produced after natural ionizing radiation and that the centres are provided with the substitution of Fe POT.3+ for Si POT.4+ in quartzo-alfa structure. The Fe POT.3+ centres are not equally distributed among the equivalent sites of the natural crystal and are responsible for the dominant features of the EPR spectra. The obtained TSDC spectrum for polarization at 1000V shows a broad band at 215K, resulting from the superposition of three bands at 185, 200 and 214k and another band at 260K. The dipole origin of these bands has been confirmed. Thermal treatments at different temperatures produce a decay of the total area and a reduction of the bands intensities. Thermal reduction increases for higher temperatures. Ultraviolet illumination partially restores the TSDC spectrum. A new band appears at room temperature. Due to the similar behavior of the TSDC and EPR spectra and taking into account that the Fe POT.3+ is the most prominent impurity in the studied samples, we believe that the dipoles are substitutional Fe POT.3+ near O POT.- or an OH POT.- and that the different position of the peaks, very near, but not the same, are in crystallographically equivalent sites.

No description available.