Analysis of the Kondo effect in ferromagnetic atomic-sized contacts

Atomic contacts made of ferromagnetic metals present zero-bias anomalies in the differential conductance due to the Kondo effect. These systems provide a unique opportunity to perform a statistical analysis of the Kondo parameters in nanostructures since a large number of contacts can be easily fabricated using break-junction techniques. The details of the atomic structure differ from one contact to another so a large number of different configurations can be statistically analyzed. Here we present such a statistical analysis of the Kondo effect in atomic contacts made from the ferromagnetic transition metals Ni, Co, and Fe. Our analysis shows clear differences between materials that can be understood by fundamental theoretical considerations. This combination of experiments and theory allows us to extract information about the origin and nature of the Kondo effect in these systems and to explore the influence of geometry and valence in the Kondo screening of atomic-sized nanostructures.

Onset of energy dissipation in ballistic atomic wires

Electronic transport at finite voltages in free-standing gold atomic chains of up to seven atoms in length is studied at low temperatures using a scanning tunneling microscope. The conductance vs voltage curves show that transport in these single-mode ballistic atomic wires is nondissipative up to a finite voltage threshold of the order of several mV. The onset of dissipation and resistance within the wire corresponds to the excitation of the atomic vibrations by the electrons traversing the wire and is very sensitive to strain.

Cotunneling theory of atomic spin inelastic electron tunneling spectroscopy

We propose cotunneling as the microscopic mechanism that makes possible inelastic electron tunneling spectroscopy of magnetic atoms in surfaces for a wide range of systems, including single magnetic adatoms, molecules, and molecular stacks. We describe electronic transport between the scanning tip and the conducting surface through the magnetic system (MS) with a generalized Anderson model, without making use of effective spin models. Transport and spin dynamics are described with an effective cotunneling Hamiltonian in which the correlations in the magnetic system are calculated exactly and the coupling to the electrodes is included up to second order in the tip MS and MS substrate. In the adequate limit our approach is equivalent to the phenomenological Kondo exchange model that successfully describes the experiments. We apply our method to study in detail inelastic transport in two systems, stacks of cobalt phthalocyanines and a single Mn atom on Cu2N. Our method accounts for both the large contribution of the inelastic spin exchange events to the conductance and the observed conductance asymmetry.

Giant magnetoresistance in ultrasmall graphene based devices

By computing spin-polarized electronic transport across a finite zigzag graphene ribbon bridging two metallic graphene electrodes, we demonstrate, as a proof of principle, that devices featuring 100% magnetoresistance can be built entirely out of carbon. In the ground state a short zigzag ribbon is an antiferromagnetic insulator which, when connecting two metallic electrodes, acts as a tunnel barrier that suppresses the conductance. The application of a magnetic field makes the ribbon ferromagnetic and conductive, increasing dramatically the current between electrodes. We predict large magnetoresistance in this system at liquid nitrogen temperature and 10 T or at liquid helium temperature and 300 G.

Spin-filtered edge states in graphene

Spin–orbit coupling changes graphene, in principle, into a two-dimensional topological insulator, also known as quantum spin Hall insulator. One of the expected consequences is the existence of spin-filtered edge states that carry dissipationless spin currents and undergo no backscattering in the presence of non-magnetic disorder, leading to quantization of conductance. Whereas, due to the small size of spin–orbit coupling in graphene, the experimental observation of these remarkable predictions is unlikely, the theoretical understanding of these spin-filtered states is shedding light on the electronic properties of edge states in other two-dimensional quantum spin Hall insulators. Here we review the effect of a variety of perturbations, like curvature, disorder, edge reconstruction, edge crystallographic orientation, and Coulomb interactions on the electronic properties of these spin filtered states.

Understanding the structure of the first atomic contact in gold

We have studied experimentally jump-to-contact (JC) and jump-out-of-contact (JOC) phenomena in gold electrodes. JC can be observed at first contact when two metals approach each other, while JOC occurs in the last contact before breaking. When the indentation depth between the electrodes is limited to a certain value of conductance, a highly reproducible behaviour in the evolution of the conductance can be obtained for hundreds of cycles of formation and rupture. Molecular dynamics simulations of this process show how the two metallic electrodes are shaped into tips of a well-defined crystallographic structure formed through a mechanical annealing mechanism. We report a detailed analysis of the atomic configurations obtained before contact and rupture of these stable structures and obtained their conductance using first-principles quantum transport calculations. These results help us understand the values of conductance obtained experimentally in the JC and JOC phenomena and improve our understanding of atomic-sized contacts and the evolution of their structural characteristics.

Modeling contact formation between atomic-sized gold tips via molecular dynamics

The formation and rupture of atomic-sized contacts is modelled by means of molecular dynamics simulations. Such nano-contacts are realized in scanning tunnelling microscope and mechanically controlled break junction experiments. These instruments routinely measure the conductance across the nano-sized electrodes as they are brought into contact and separated, permitting conductance traces to be recorded that are plots of conductance versus the distance between the electrodes. One interesting feature of the conductance traces is that for some metals and geometric configurations a jump in the value of the conductance is observed right before contact between the electrodes, a phenomenon known as jump-to-contact. This paper considers, from a computational point of view, the dynamics of contact between two gold nano-electrodes. Repeated indentation of the two surfaces on each other is performed in two crystallographic orientations of face-centred cubic gold, namely (001) and (111). Ultimately, the intention is to identify the structures at the atomic level at the moment of first contact between the surfaces, since the value of the conductance is related to the minimum cross-section in the contact region. Conductance values obtained in this way are determined using first principles electronic transport calculations, with atomic configurations taken from the molecular dynamics simulations serving as input structures.

Rashba spin precession in a magnetic field

Spin precession due to Rashba spin-orbit coupling in a two-dimension electron gas is the basis for the spin field effect transistor, in which the overall perfect spin-polarized current modulation could be acquired. There is a prerequisite, however, that a strong transverse confinement potential should be imposed on the electron gas or the width of the confined quantum well must be narrow. We propose relieving this rather strict limitation by applying an external magnetic field perpendicular to the plane of the electron gas because the effect of the magnetic field on the conductance of the system is equivalent to the enhancement of the lateral confining potential. Our results show that the applied magnetic field has little effect on the spin precession length or period although in this case Rashba spin-orbit coupling could lead to a Zeeman-type spin splitting of the energy band.

Duality of weak and strong scatterer in a Luttinger liquid coupled to massless bosons

We study electronic transport in a Luttinger liquid with an embedded impurity, which is either a weak scatterer (WS) or a weak link (WL), when interacting electrons are coupled to one-dimensional massless bosons (e.g., acoustic phonons). We find that the duality relation, ?WS?WL=1, between scaling dimensions of the electron backscattering in the WS and WL limits, established for the standard Luttinger liquid, holds in the presence of the additional coupling for an arbitrary fixed strength of boson scattering from the impurity. This means that at low temperatures such a system remains either an ideal insulator or an ideal metal, regardless of the scattering strength. On the other hand, when fermion and boson scattering from the impurity are correlated, the system has a rich phase diagram that includes a metal-insulator transition at some intermediate values of the scattering.

First-principles calculation of carrier-phonon scattering in n-type Si1−xGex alloys

First-principles electronic structure methods are used to find the rates of inelastic intravalley and intervalley n-type carrier scattering in Si1-xGex alloys. Scattering parameters for all relevant Delta and L intra- and intervalley scattering are calculated. The short-wavelength acoustic and the optical phonon modes in the alloy are computed using the random mass approximation, with interatomic forces calculated in the virtual crystal approximation using density functional perturbation theory. Optical phonon and intervalley scattering matrix elements are calculated from these modes of the disordered alloy. It is found that alloy disorder has only a small effect on the overall inelastic intervalley scattering rate at room temperature. Intravalley acoustic scattering rates are calculated within the deformation potential approximation. The acoustic deformation potentials are found directly and the range of validity of the deformation potential approximation verified in long-wavelength frozen phonon calculations. Details of the calculation of elastic alloy scattering rates presented in an earlier paper are also given. Elastic alloy disorder scattering is found to dominate over inelastic scattering, except for almost pure silicon (x approximate to 0) or almost pure germanium (x approximate to 1), where acoustic phonon scattering is predominant. The n-type carrier mobility, calculated from the total (elastic plus inelastic) scattering rate, using the Boltzmann transport equation in the relaxation time approximation, is in excellent agreement with experiments on bulk, unstrained alloys..

First-principles calculation of P-type alloy scattering in Si1-xGex

The p-type carrier scattering rate due to alloy disorder in Si1-xGex alloys is obtained from first principles. The required alloy scattering matrix elements are calculated from the energy splitting of the valence bands, which arise when one average host atom is replaced by a Ge or Si atom in supercells containing up to 128 atoms. Alloy scattering within the valence bands is found to be characterized by a single scattering parameter. The hole mobility is calculated from the scattering rate using the Boltzmann transport equation in the relaxation time approximation. The results are in good agreement with experiments on bulk, unstrained alloys..

Application of Numerical Methods to Study Arrangement and Fracture of Lithium-Ion Microstructure

The focus of this work is to develop and employ numerical methods that provide characterization of granular microstructures, dynamic fragmentation of brittle materials, and dynamic fracture of three-dimensional bodies.

We first propose the fabric tensor formalism to describe the structure and evolution of lithium-ion electrode microstructure during the calendaring process. Fabric tensors are directional measures of particulate assemblies based on inter-particle connectivity, relating to the structural and transport properties of the electrode. Applying this technique to X-ray computed tomography of cathode microstructure, we show that fabric tensors capture the evolution of the inter-particle contact distribution and are therefore good measures for the internal state of and electronic transport within the electrode.

We then shift focus to the development and analysis of fracture models within finite element simulations. A difficult problem to characterize in the realm of fracture modeling is that of fragmentation, wherein brittle materials subjected to a uniform tensile loading break apart into a large number of smaller pieces. We explore the effect of numerical precision in the results of dynamic fragmentation simulations using the cohesive element approach on a one-dimensional domain. By introducing random and non-random field variations, we discern that round-off error plays a significant role in establishing a mesh-convergent solution for uniform fragmentation problems. Further, by using differing magnitudes of randomized material properties and mesh discretizations, we find that employing randomness can improve convergence behavior and provide a computational savings.

The Thick Level-Set model is implemented to describe brittle media undergoing dynamic fragmentation as an alternative to the cohesive element approach. This non-local damage model features a level-set function that defines the extent and severity of degradation and uses a length scale to limit the damage gradient. In terms of energy dissipated by fracture and mean fragment size, we find that the proposed model reproduces the rate-dependent observations of analytical approaches, cohesive element simulations, and experimental studies.

Lastly, the Thick Level-Set model is implemented in three dimensions to describe the dynamic failure of brittle media, such as the active material particles in the battery cathode during manufacturing. The proposed model matches expected behavior from physical experiments, analytical approaches, and numerical models, and mesh convergence is established. We find that the use of an asymmetrical damage model to represent tensile damage is important to producing the expected results for brittle fracture problems.

The impact of this work is that designers of lithium-ion battery components can employ the numerical methods presented herein to analyze the evolving electrode microstructure during manufacturing, operational, and extraordinary loadings. This allows for enhanced designs and manufacturing methods that advance the state of battery technology. Further, these numerical tools have applicability in a broad range of fields, from geotechnical analysis to ice-sheet modeling to armor design to hydraulic fracturing.

Trasporte eléctrico y magnetismo en sistemas electrodo - aislante - electrodo: hacia el desarrollo de dispositivos del tipo juntura tunel.

La presente tesis es un estudio dedicado a la optimización y desarrollo de sistemas del tipo juntura túnel. La metodología utilizada para la realización de la tesis consistió, en primer lugar, en la optimización de las componentes independientes de la juntura túnel: electrodo y barrera aislante. Posteriormente se optimizaron los procesos de fabricación para el desarrollo y caracterización de dispositivos del tipo juntura túnel en su forma final. En la primera parte de la tesis se analizan detalladamente los resultados obtenidos de la caracterización eléctrica y topografica de barreras aislantes en sistemas electrodo - barrera. Los sistemas bicapas estudiados, GdBa_2Cu_3_7/SrTiO_3, Nb/Ba_0,05Sr_0,95TiO_3 y YBa_2Cu_3O_7/SrTiO_3, fueron caracterizados utilizando un microscopio de fuerza atómica en modo conductor. Se propuso un modelo fenomenológico basado en los resultados experimentales, que permitió la obtención de parámetros críticos para el desarrollo de dispositivos del tipo juntura túnel con nuevas funcionalidades. La información obtenida de la caracterización de los sistemas bicapas (homogeneidad de crecimiento, baja densidad de defectos y de pinholes) indican un muy buen control de los parámetros de crecimiento de las barreras. Por otro lado, se obtuvo un buen comportamiento aislante para espesores mayores a 2 nm sin la presencia de pinholes en la barrera. La similitud en la estequiometría de las barreras (SrTiO_3) permitió comparar los distintos sistemas estudiados en términos de conductividad eléctrica. Se verificó que el modelo fenomenológico permite comparar la conductividad eléctrica de los sistemas mediante uno de los parámetros definidos en el modelo fenomenológico (obtenido de los ajustes lineales de las curvas I(V)). De los 3 sistemas estudiados, las bicapas GdBa_2Cu_3O_7/SrTiO_3 presentaron un mayor valor de longitud de atenuación de los portadores de carga a través de la barrera y una muy baja densidad de defectos superficiales. Las bicapas YBa_2Cu_3O_7/SrTiO_3 y Nb/Ba_0,05Sr_0,95TiO_3 permitieron validar el modelo fenomenológico propuesto para el análisis de la respuesta corriente - voltaje obtenida con el microscopio de fuerza atómica en modo conductor. La segunda parte de la tesis abarca conceptos de magnetismo y microfabricación para el desarrollo de junturas túnel magnéticas. Durante la caracterización de las películas ferromagnéticas individuales de Co_90Fe_10 (CoFe) se logró aumentar valor del campo coercitivo de films de 10 nm de espesor al incrementar la temperatura de depósito. Esto se debe a un aumento del tamaño de grano de los films. El aumento de la temperatura del sustrato durante el crecimiento influye en la morfología y las propiedades magnéticas de los films de CoFe favoreciendo la formación de granos y la pérdida del eje preferencial de magnetización. Estos resultados permitieron la fabricación de sistemas Co_90Fe_10/M_gO/Co_90Fe_10 con distintas orientaciones relativas accesibles con campo magnético para el estudio del acople magnético entre los films de CoFe. La caracterización eléctrica de estos sistemas, particularmente la respuesta corriente - voltaje obtenida con el microscopio de fuerza atómica en modo conductor, indicó que las propiedades de transporte eléctrico de las junturas presentan un alto grado de reproducibilidad. Se analizó además la inuencia del sustrato utilizado en la corriente túnel que atraviesa la barrera aislante. Por otro lado, se discuten los fenómenos relacionados a la optimización de las propiedades magnéticas de electrodos ferromagnéticos para la fabricación de junturas túnel Co_90Fe_10/MgO/Co_90Fe_10 y Co_90Fe_10/MgO /Fe_20Ni_80. En particular, se estudió el acople magnético entre capas ferromagnéticas y la inuencia del sustrato utilizado para el crecimiento de las tricapas. La optimización de los electrodos magnéticos involucró el análisis de la inuencia de la presencia de un aislante entre dos capas magnéticas en el acople de los electrodos. Se logró el desacople de films de 10 nm de Co_90Fe_10 y Fe_20Ni_80 separados por un espaciador de MgO de 2 nm. Finalmente se detallan los pasos para la fabricación de una red de junturas túnel magnéticas y su caracterización eléctrica a bajas temperaturas. El sistema estudiado fue la tricapa Co_90Fe_10 (10 nm)/M_gO (8 nm)/ Fe_20Ni_80 (10 nm) crecido sobre un sustrato de M_gO. La caracterización eléctrica confirmó la buena calidad de la junturas fabricadas. Las junturas obtenidas presentaron un comportamiento altamente resistivo (~ MΩ). Las mediciones de la corriente túnel en función de la temperatura permitieron descartar la presencia de pinholes en la barrera. El transporte de los portadores de carga es por efecto túnel a través de la barrera aislante. Las curvas de conductancia diferencial permitieron calcular el valor medio de la altura de la barrera de potencial (φ = 3.1 eV) a partir del modelo de Brinkman. Los resultados obtenidos en cada uno de los capítulos se complementan y son relevantes para la optimización de junturas túnel, debido a que brindan información crítica para su correcto funcionamiento. En la presente tesis se lograron obtener los primeros avances para la fabricación de arreglos de junturas túnel que permitan el desarrollo de dispositivos.

Trasporte eléctrico y magnetismo en sistemas electrodo - aislante - electrodo: hacia el desarrollo de dispositivos del tipo juntura tunel.

La presente tesis es un estudio dedicado a la optimización y desarrollo de sistemas del tipo juntura túnel. La metodología utilizada para la realización de la tesis consistió, en primer lugar, en la optimización de las componentes independientes de la juntura túnel: electrodo y barrera aislante. Posteriormente se optimizaron los procesos de fabricación para el desarrollo y caracterización de dispositivos del tipo juntura túnel en su forma final. En la primera parte de la tesis se analizan detalladamente los resultados obtenidos de la caracterización eléctrica y topografica de barreras aislantes en sistemas electrodo - barrera. Los sistemas bicapas estudiados, GdBa_2Cu_3_7/SrTiO_3, Nb/Ba_0,05Sr_0,95TiO_3 y YBa_2Cu_3O_7/SrTiO_3, fueron caracterizados utilizando un microscopio de fuerza atómica en modo conductor. Se propuso un modelo fenomenológico basado en los resultados experimentales, que permitió la obtención de parámetros críticos para el desarrollo de dispositivos del tipo juntura túnel con nuevas funcionalidades. La información obtenida de la caracterización de los sistemas bicapas (homogeneidad de crecimiento, baja densidad de defectos y de pinholes) indican un muy buen control de los parámetros de crecimiento de las barreras. Por otro lado, se obtuvo un buen comportamiento aislante para espesores mayores a 2 nm sin la presencia de pinholes en la barrera. La similitud en la estequiometría de las barreras (SrTiO_3) permitió comparar los distintos sistemas estudiados en términos de conductividad eléctrica. Se verificó que el modelo fenomenológico permite comparar la conductividad eléctrica de los sistemas mediante uno de los parámetros definidos en el modelo fenomenológico (obtenido de los ajustes lineales de las curvas I(V)). De los 3 sistemas estudiados, las bicapas GdBa_2Cu_3O_7/SrTiO_3 presentaron un mayor valor de longitud de atenuación de los portadores de carga a través de la barrera y una muy baja densidad de defectos superficiales. Las bicapas YBa_2Cu_3O_7/SrTiO_3 y Nb/Ba_0,05Sr_0,95TiO_3 permitieron validar el modelo fenomenológico propuesto para el análisis de la respuesta corriente - voltaje obtenida con el microscopio de fuerza atómica en modo conductor. La segunda parte de la tesis abarca conceptos de magnetismo y microfabricación para el desarrollo de junturas túnel magnéticas. Durante la caracterización de las películas ferromagnéticas individuales de Co_90Fe_10 (CoFe) se logró aumentar valor del campo coercitivo de films de 10 nm de espesor al incrementar la temperatura de depósito. Esto se debe a un aumento del tamaño de grano de los films. El aumento de la temperatura del sustrato durante el crecimiento influye en la morfología y las propiedades magnéticas de los films de CoFe favoreciendo la formación de granos y la pérdida del eje preferencial de magnetización. Estos resultados permitieron la fabricación de sistemas Co_90Fe_10/M_gO/Co_90Fe_10 con distintas orientaciones relativas accesibles con campo magnético para el estudio del acople magnético entre los films de CoFe. La caracterización eléctrica de estos sistemas, particularmente la respuesta corriente - voltaje obtenida con el microscopio de fuerza atómica en modo conductor, indicó que las propiedades de transporte eléctrico de las junturas presentan un alto grado de reproducibilidad. Se analizó además la inuencia del sustrato utilizado en la corriente túnel que atraviesa la barrera aislante. Por otro lado, se discuten los fenómenos relacionados a la optimización de las propiedades magnéticas de electrodos ferromagnéticos para la fabricación de junturas túnel Co_90Fe_10/MgO/Co_90Fe_10 y Co_90Fe_10/MgO /Fe_20Ni_80. En particular, se estudió el acople magnético entre capas ferromagnéticas y la inuencia del sustrato utilizado para el crecimiento de las tricapas. La optimización de los electrodos magnéticos involucró el análisis de la inuencia de la presencia de un aislante entre dos capas magnéticas en el acople de los electrodos. Se logró el desacople de films de 10 nm de Co_90Fe_10 y Fe_20Ni_80 separados por un espaciador de MgO de 2 nm. Finalmente se detallan los pasos para la fabricación de una red de junturas túnel magnéticas y su caracterización eléctrica a bajas temperaturas. El sistema estudiado fue la tricapa Co_90Fe_10 (10 nm)/M_gO (8 nm)/ Fe_20Ni_80 (10 nm) crecido sobre un sustrato de M_gO. La caracterización eléctrica confirmó la buena calidad de la junturas fabricadas. Las junturas obtenidas presentaron un comportamiento altamente resistivo (~ MΩ). Las mediciones de la corriente túnel en función de la temperatura permitieron descartar la presencia de pinholes en la barrera. El transporte de los portadores de carga es por efecto túnel a través de la barrera aislante. Las curvas de conductancia diferencial permitieron calcular el valor medio de la altura de la barrera de potencial (φ = 3.1 eV) a partir del modelo de Brinkman. Los resultados obtenidos en cada uno de los capítulos se complementan y son relevantes para la optimización de junturas túnel, debido a que brindan información crítica para su correcto funcionamiento. En la presente tesis se lograron obtener los primeros avances para la fabricación de arreglos de junturas túnel que permitan el desarrollo de dispositivos.

Electrical and optical studies on carbon nanotube arrays

Single-walled carbon nanotubes (SWNTs) have been studied as a prominent class of high performance electronic materials for next generation electronics. Their geometry dependent electronic structure, ballistic transport and low power dissipation due to quasi one dimensional transport, and their capability of carrying high current densities are some of the main reasons for the optimistic expectations on SWNTs. However, device applications of individual SWNTs have been hindered by uncontrolled variations in characteristics and lack of scalable methods to integrate SWNTs into electronic devices. One relatively new direction in SWNT electronics, which avoids these issues, is using arrays of SWNTs, where the ensemble average may provide uniformity from device to device, and this new breed of electronic material can be integrated into electronic devices in a scalable fashion. This dissertation describes (1) methods for characterization of SWNT arrays, (2) how the electrical transport in these two-dimensional arrays depend on length scales and spatial anisotropy, (3) the interaction of aligned SWNTs with the underlying substrate, and (4) methods for scalable integration of SWNT arrays into electronic devices. The electrical characterization of SWNT arrays have been realized by polymer electrolyte-gated SWNT thin film transistors (TFTs). Polymer electrolyte-gating addresses many technical difficulties inherent to electrical characterization by gating through oxide-dielectrics. Having shown polymer electrolyte-gating can be successfully applied on SWNT arrays, we have studied the length scaling dependence of electrical transport in SWNT arrays. Ultrathin films formed by sub-monolayer surface coverage of SWNT arrays are very interesting systems in terms of the physics of two-dimensional electronic transport. We have observed that they behave qualitatively different than the classical conducting films, which obey the Ohm’s law. The resistance of an ultrathin film of SWNT arrays is indeed non-linear with the length of the film, across which the transport occurs. More interestingly, a transition between conducting and insulating states is observed at a critical surface coverage, which is called percolation limit. The surface coverage of conducting SWNTs can be manipulated by turning on and off the semiconductors in the SWNT array, leading to the operation principle of SWNT TFTs. The percolation limit depends also on the length and the spatial orientation of SWNTs. We have also observed that the percolation limit increases abruptly for aligned arrays of SWNTs, which are grown on single crystal quartz substrates. In this dissertation, we also compare our experimental results with a two-dimensional stick network model, which gives a good qualitative picture of the electrical transport in SWNT arrays in terms of surface coverage, length scaling, and spatial orientation, and briefly discuss the validity of this model. However, the electronic properties of SWNT arrays are not only determined by geometrical arguments. The contact resistances at the nanotube-nanotube and nanotube-electrode (bulk metal) interfaces, and interactions with the local chemical groups and the underlying substrates are among other issues related to the electronic transport in SWNT arrays. Different aspects of these factors have been studied in detail by many groups. In fact, I have also included a brief discussion about electron injection onto semiconducting SWNTs by polymer dopants. On the other hand, we have compared the substrate-SWNT interactions for isotropic (in two dimensions) arrays of SWNTs grown on Si/SiO2 substrates and horizontally (on substrate) aligned arrays of SWNTs grown on single crystal quartz substrates. The anisotropic interactions associated with the quartz lattice between quartz and SWNTs that allow near perfect horizontal alignment on substrate along a particular crystallographic direction is examined by Raman spectroscopy, and shown to lead to uniaxial compressive strain in as-grown SWNTs on single crystal quartz. This is the first experimental demonstration of the hard-to-achieve uniaxial compression of SWNTs. Temperature dependence of Raman G-band spectra along the length of individual nanotubes reveals that the compressive strain is non-uniform and can be larger than 1% locally at room temperature. Effects of device fabrication steps on the non-uniform strain are also examined and implications on electrical performance are discussed. Based on our findings, there are discussions about device performances and designs included in this dissertation. The channel length dependences of device mobilities and on/off ratios are included for SWNT TFTs. Time response of polymer-electrolyte gated SWNT TFTs has been measured to be ~300 Hz, and a proof-of-concept logic inverter has been fabricated by using polymer electrolyte gated SWNT TFTs for macroelectronic applications. Finally, I dedicated a chapter on scalable device designs based on aligned arrays of SWNTs, including a design for SWNT memory devices.