É descrito um sistema automatizado para a realização de medidas elétricas em materiais dielétricos. Um microcomputador é responsável pelo controle e programação da temperatura da amostra, aquisição dos dados experimentais e apresentação e armazenamento dos resultados. O controle de temperatura permite aquecer e resfriar amostras a taxas constantes, manter a temperatura constante, superpor a esses processos uma variação senoidal de temperatura e ainda programar aquecimentos com taxas não lineares. Por esta versatilidade, o sistema permite realizar vários tipos de medidas elétricas tais como; corrente termo estimuladas em circuito fechado e aberto, correntes de absorção e correntes piroelétricas. Mostra-se o desempenho do sistema e alguns resultados de medidas elétricas em polímeros. / We describe an automatic system for electrical measurements in dielectric samples. The system is based on an Apple-like microcomputer, responsible for controlling and programming the sample temperature, data acquisition, display and storage. The temperature control allows heating and cooling samples at fixed rates, over which a superimposed sinusoidal perturbation may be applied, and also, non linear heating rates can be generated. Because of this versatility, the system allows many types of electrical measurements, just like thermal stimulated currents, thermal stimulated discharges, absorption currents and pyroelectric currents. We show the performance of the system and some results of practical measurements in polymers.

A irradiação de dielétricos sólidos com feixes eletrônicos tem-se revelado uma poderosa ferramenta na investigação das características de armazenamento e condução de carga elétrica nesses materiais. O presente trabalho faz urna revisão dos resultados que se tem obtido no campo, discute uma equação de transporte para carga em excesso em isolantes amorfos e aplica-la a particulares montagens experimentais. Encontra-se que os efeitos de carga espacial não são em geral importantes para pequenas penetrações do feixe na amostra, mas desempenham papel essencial no caso de elétrons quase-trespassantes. Em particular, obtém-se satisfatória concordância com os resultados experimentais de Spear (1955). / Irradiation of solid dielectric with electron beams has been used as a powerful tool in investigations of charge storage and transport in such materials. The present work reviews some of the results that have been obtained in this area and discusses the formulation of a transport equation for excess charge in irradiated insulators. This equation is subsequently applied to various experimental set-ups . It is found that space charge effects p1ay an essential role in the establishment of stationary currents in samples subject to quasi- -penetrating electron beams. Such effects may, however, be neglected for low electron ranges. Theoretical results are in good agreement with experimental findings by Spear (1955).

The propagation of waves through nonlinear media is of interest here, namely as it pertains to two specific examples, a nonlinear dielectric and a hyperelastic solid. In both cases, we examine the propagation of two-dimensional, weakly nonlinear, quasi-planar waves. It is found that such systems will have a nonlinearity that is intrinsically cubic, and therefore, a classical Zabolotskaya-Khokhlov equation cannot give an accurate description of the wave evolution. To determine the general evolution equation in such systems, a multi-timing technique developed by Kluwick and Cox (1998) and Cramer and Webb (1998) will be employed. The resultant evolution equations are seen to involve only one new nonlinearity coefficient rather than the three coefficients found in other studies of cubically nonlinear systems. After determining the general evolution equation, inclusion of relaxation, dispersion and dissipation effects can be easily incorporated. / Master of Science

Aerogels are highly porous, low dielectric constant (low k) materials being considered by the semiconductor industry as an interlayer dielectric. Low k materials are needed to overcome capacitance problems that limit device feature sizes. Precursors triethoxyfluorosilane (TEFS) and tetraethoxysilane (TEOS) were used to prepare bulk aerogels. Samples were prepared by sol-gel methods, and then carbon dioxide supercritically-dried. Effects of varying the water to precursor ratio were studied with respect to aerogel properties and microstructure. Methods of analysis for this study include FTIR-ATR, TEM, RBS, EDS, SEM, dielectric constant determination by impedance and surface area by gas adsorption. Si-F bonds were determined to be present in both acid- and base-catalyzed TEFS as well as HF-catalyzed TEOS. Fluorine promotes a fractal network microstructure as opposed to a particle-like microstructure. Surface area and dielectric constant were determined to increase slightly with increases in the water to precursor ratio.

Integrating nanometer-sized pores into low-k ILD films is one of the approaches to lower the RC signal delay and thus help sustain the continued scaling of microelectronic devices. While increasing porosity of porous dielectrics lowers the dielectric constant (k), it also creates many reliability and implementation issues. One of the problems is the little understood metal ion diffusion and drift in porous media. Here, we present a rigorous simulation method of Cu diffusion based on Master equation with elementary jump probabilities within the contiguous dielectric film, along the pore boundary, from the dielectric matrix to the pore boundary, and from the pore boundary to the matrix material. In view of the diffusional jump distance being as large as 2 nm, the nano-pores being on a similar length scale, and the film thickness being only a few tens of nanometers, the conventional diffusion equation in differential equation form is grossly inadequate and elementary jump frequencies are required for a proper description of the Cu diffusion in porous dielectric. The present atomistic approach allows a consistent implementation of Cu ion drift in electric field by lowering and raising of the diffusion barriers along the field direction. This will help understand the behavior of Cu interconnects under thermal or electric stress at an atomistic level. Another approach to lower the increasing RC delays is to bring memory and logic closer by integrating memory in the BEOL. Resistive RAM is one such memory is not transistor based and thus, does not require a silicon substrate. Thus, it offers the possibility of integration directly into the back-end reducing memory to logic distance from 1000s of µm to a 10s of nm. This 3D integration also allows for increased density as well. However, one barrier in the implementation of RRAM in the back end is the use of expensive as well as non-BEOL native material in conventional Cu/TaOx/Pt resistive devices. In this thesis, we present our research about functionality of RRAM with porous low-k dielectrics (which are a candidate for CMOS ILD), and through the similar elementary jump simulations, discuss the impact of porosity in dielectrics on the functionality of RRAM. Lastly, we present a cheaper replacement for Pt as the counter electrode in RRAM and show that it functions as good as Pt. This work addresses following three areas: 1. Modeling of diffusion in porous dielectrics through elementary jump based simulation. The model is based on random walk theory of elementary particle jumps. Initially, qualitative simulations are conducted without actual parameters. It is shown that Cu diffusion in porous dielectrics decreases quasi-linearly with porosity. Furthermore, it is shown that morphology of the pores may have a greater effect on diffusivity compared to porosity. The simulations are then calibrated with parameters, and the result is shown to yield a similar diffusivity times as actual process time. 2. Modeling of Cu ions drift in porous dielectrics under electric stress. First, the model is explained, and then qualitative simulation results are presented for porous dielectrics with varied porosities and morphologies. 3. Research to find a suitable replacement for Pt as the counter electrode in RRAM devices. The research methodology is discussed and a much cheaper Rh is selected as the potential replacement for Pt. Successful functionality of Rh based resistive devices is presented. / Master of Science

Active colloids are small particles that can convert external energy supply into self-propulsion. Because of the existence of the energy current inside and across the system, active colloids exhibit behaviors that are far away from thermodynamic equilibrium. During the past decades, active colloids have been used to provide models for many different non-equilibrium system studies and have been designed to complete tasks on small scale. By tuning the particle size, shape, etc, or changing the actuation methods of the active colloid systems, people have developed a large number of different active colloid systems. Among all active colloid systems, the Quincke rotation system can effectively propel particles with rapid speed. This phenomenon refers to the spontaneous rolling of a dielectric sphere in a weakly conducting liquid under a DC electric field. Although the basic mechanism of a single Quincke roller has been well explained, some behaviors that occur in complex environments or with multiple Quincke particles are still mysteries. For example, one particle will move back and forth on the bottom electrode under a high electric DC field. This so-called Quincke Oscillation motion cannot be explained by the previous models well. So a new model is required. In this dissertation, we will focus on explaining this newly-discovered dynamic in the Quincke system. Then we will study the collective dynamics of multiple Quincke oscillators with designed experiments and models. In Chapter 1, the background and different actuation methods of active colloid systems are first introduced. Then the Quincke rotation system and its field-dependent dynamics are explained with a classic leaky dielectric model. The recent research results with Quincke systems are shortly reviewed afterward. In Chapter 2, we introduce the experimentally discovered Quincke Oscillation phenomenon. Then we reveal its dependency on liquid conductivity and particle size. This dynamic is finally explained by the asymmetric charging of the particle surface in the field-induced boundary layer near the electrode. This work opens the door to the study of the collective dynamics of Quincke oscillators. In Chapter 3, we first introduce a dynamical model considering the charge, dipole, and quadrupole moments of the sphere and predict its oscillatory motion under a non-uniform liquid conductivity environment. Then we study the behavior of two coupled Quincke oscillators with far-field hydrodynamic and electrostatic interactions. The numerical simulations predict the synchronization and alignment of two oscillators with fixed positions. We further develop a model based on weakly coupled oscillator assumptions by considering the relative phase and oscillating orientations of two oscillators. The model successfully explains the numerical simulation results and can be applied to other active colloid systems with multiple mobile oscillators. In Chapter 4, we show that the Quincke oscillators can assemble into a cluster and oscillate with high synchronization and alignment. This formation of the cluster can also increase the oscillation frequency of the oscillators. By considering the perfect contact rolling of the oscillators on the electrode, we develop a weakly coupled oscillator theory model. This model explains the tendency of particles to synchronize and align in a cluster and predicts the increase of the oscillation frequency when particles are in synchronized phases. The cluster is stabilized due to the existing phase waves observed in experiments and simulations. In Chapter 5, we introduce two other studies on Quincke rollers with different experimental designs. Particles of helical shape exhibit self-propulsion in the liquid bulk and highlight the role of shape in controlling particle dynamics. For multiple spheres in a height-confined system, the particles display a transition from a fluctuating state to an absorbing stable state depending on their density and the applied field strength. This work provides an experimental model for studying absorbing state. In Chapter 6, the development of the Quincke system study is reviewed and some future directions are suggested.

Bound electromagnetic surface waves can be excited by free-space waves on a corrugated conduction surface. These electromagnetic surface waves, called surface plasmon polaritons (SPPs), are coupled to a plasma of free charges, which travel together with the wave. We investigated the effect of separating metal corrugations from the smooth metal ground plane with a thin dielectric layer and show that SPPs can be excited via displacement currents. However, the SPP excitation resonances broaden and disappear as the dielectric thickness approaches 1% of the wavelength.

No description available.

No description available.

The dielectric dispersion of poly(vinyl acetate) solutions was studied in an attempt to relate this behavior to the chemical nature of the material. The bridge method was employed in which capacitance measurement of solutions were made over a frequency range of 400 cycles to 500 kilocycles. The results of these experiments indicate that a vinyl type material possesses greater flexibility than cellulose derivatives in solution and, thus, the magnitude of capacitance changes over a frequency range is considerably reduced. Because of the very small changes in capacitance, reproducible results are difficult to obtain and definite conclusions as to the relation of dispersion to molecular weight are impossible. Dielectric dispersion studies were made on solutions of poly(vinyl acetate) in dioxane, ethylene chloride and acetone. / Master of Science