The search for quantum spin liquids (QSLs) introduces some of the most challenging and interesting problems in contemporary physics. The recently discovered iridate Cu2IrO3,which contains a honeycomb lattice of Ir4+ions with effective spin 1/2 coupled by frustrated Ising interactions, presents itself as a promising candidate for a Kitaev QSL. In this study, we use nuclear magnetic resonance (NMR), a spectroscopic technique based on the energy levels of nuclear spin states, to probe the intrinsic spin excitations of Cu2IrO3. By measuring the NMR frequency shift of 63Cu from 4.2 K to 298 K,we demonstrate that its spin susceptibility χ spin behaves nearly identically to its parent compound Na2IrO3, without showing evidence of magnetic ordering at low temperatures. We showed that the upturn of bulk susceptibility χ below T=50 K is due to the contribution of defect spins. The hyperfine coupling constant Ahf between Cu and Ir4+was also estimated by comparing the Knight shift 63K to χ / Thesis / Master of Science (MSc)

In this thesis we investigate the frustrated spin liquid Tb$_2$Ti$_2$O$_7$ theoretically. The low-energy effective Hamiltonian of this compound is derived by integrating out the excited crystal field states. It is shown that the pairwise interaction in the effective Hamiltonian is renormalized by all the other Tb$_2$Ti$_2$O$_7$ ions in the system and dynamically generate frustration. The phase diagram of Tb$_2$Ti$_2$O$_7$ in the single tetrahedron approximation is calculated. It is shown that Tb$_2$Ti$_2$O$_7$ is in a singlet state which is a linear combination of all frustrated two-in/two-out states. Motivated by experimental results, the diffuse neutron scattering of Tb$_2$Ti$_2$O$_7$ is obtained within the single tetrahedron approximation. This diffuse neutron scattering captures semi-quantitatively most of the experimental neutron scattering features. The magnetization of Tb$_2$Ti$_2$O$_7$ in the single tetrahedron approximation is calculated. Two experiments based on diffuse neutron scattering and magnetization in high symmetry directions are proposed to verify the spin ice like ground state of Tb$_2$Ti$_2$O$_7$.

In this thesis we investigate the frustrated spin liquid Tb$_2$Ti$_2$O$_7$ theoretically. The low-energy effective Hamiltonian of this compound is derived by integrating out the excited crystal field states. It is shown that the pairwise interaction in the effective Hamiltonian is renormalized by all the other Tb$_2$Ti$_2$O$_7$ ions in the system and dynamically generate frustration. The phase diagram of Tb$_2$Ti$_2$O$_7$ in the single tetrahedron approximation is calculated. It is shown that Tb$_2$Ti$_2$O$_7$ is in a singlet state which is a linear combination of all frustrated two-in/two-out states. Motivated by experimental results, the diffuse neutron scattering of Tb$_2$Ti$_2$O$_7$ is obtained within the single tetrahedron approximation. This diffuse neutron scattering captures semi-quantitatively most of the experimental neutron scattering features. The magnetization of Tb$_2$Ti$_2$O$_7$ in the single tetrahedron approximation is calculated. Two experiments based on diffuse neutron scattering and magnetization in high symmetry directions are proposed to verify the spin ice like ground state of Tb$_2$Ti$_2$O$_7$.

We investigate the properties of the Kitaev honeycomb model with both site dilution and exchange randomness. Embarking on this work, we review disorder in some strongly correlated electron systems, including spin-½ and spin-1 Heisenberg antiferromagnetic chains, two dimensional Heisenberg antiferromagnets, the cuprates and graphene. We outline some aspects of resonating valence bond phases, valence bond solids, spin liquids and quantum computation that are pertinent to an understanding of the Kitaev model. The properties of the Kitaev model without disorder are discussed and it is found to be a critical spin liquid, with algebraic correlations in two spin operators sigma^{alpha}_{i}sigma^{alpha}_{j}, where i and j,/em> are either end of a link of type alpha = x, y or z on the honeycomb lattice. The Kitaev model is exactly solvable and we show that this remains so in the presence of site dilution and exchange randomness. We find that vacancies bind a flux. In the gapped phase, a vacancy forms an effective paramagnetic moment. With two or more vacancies we describe the interaction of their effective moments and show that a finite density of vacancies leads to a divergent macroscopic susceptibility at small fields. In the gapless phase the effective moment has a susceptibility that is, to leading order at small fields, chi(h)~log(1/h). Interaction between the moments from two vacancies on opposite sublattices cuts off this divergence in susceptibility at a large but finite constant. Two vacancies on the same sublattice behave quite differently and we find the combined susceptibility is parametrically larger than that of an isolated vacancy, chi(h)sim [h(log(1/h))^{3/2}]^{-1}. We also investigate the effects of slowly varying, quenched disorder in exchange coupling. We demonstrate that this does not qualitatively affect the susceptibility but show that the heat capacity C ~ T^{2/z}, where z is a measure of the disorder and increases from one with increasing disorder strength.

The Kitaev model has become a source of much excitement in the field of condensed matter. It is a two dimensional model of spins ½ on a honeycomb lattice with bond-dependent interactions. Its interesting properties include a quantum spin liquid ground state and anyonic excitations. These properties could lead to exciting applications in quantum computing if materials were found to behave similarly to the Kitaev model. Such materials have been found, however the Kitaev model is too simple to describe these materials and additional interactions must be considered. The Heisenberg interaction is one such additional interaction. As such, we can define the Kitaev-Heisenberg model by combining the Kitaev and Heisenberg interactions. We can now ask ourselves if the quantum spin liquid ground state and anyonic excitations still exist in the Kitaev-Heisenberg model. To answer this question, a non-local string order parameter has been defined which is non-zero inside the quantum spin liquid phase and zero outside of it. This string order parameter was shown to exist and survive the Heisenberg interaction on the 2-leg ladder. In this thesis, we look to expand this result to multileg ladders such as the 3-leg, 4-leg, and 5-leg ladders to see if the string order parameter survives in the Kitaev-Heisenberg model in 2 dimensions. Our results show that the string order parameter does exist in multileg ladders, however the phase space window in which it survives the Heisenberg interaction is narrower than in the 2-leg ladder. / Thesis / Master of Science (MSc)

The langasites are a class of geometrically frustrated compounds with the formula A3XY3Z2O14 where A,X,Y,Z are cationic sites and site A is occupied by a magnetic ion. The interactions of the magnetic ions form a star shaped pattern called the Kagomé lattice. The langasites have been widely studied by the solid state community because of their functional properties such as piezoelectricity, multiferroicity, ferroelectricity, dielectricity and for use in the telecommunication industry. It was also realized that some langasite materials exhibit exotic magnetic ground states at low temperatures. A thorough understanding of their ground state is limited by the difficulty in synthesizing new members belonging to this series due to the formation of competing phases such as the garnets. In this study, four new magnetic langasites A3Ga3Ge2BeO14 (A= Pr, Nd, Sm and Eu) and a non-magnetic lattice standard La3Ga3Ge2BeO14 were synthesized. These were further structurally characterized by powder X-ray diffraction, Rietveld refinement and bond valence analysis. Further characterization of the low-temperature magnetism was done by performing magnetization, magnetic susceptibility (field cooled and zero field cooled) and heat capacity measurements. The low temperature spin dynamics were probed using muon spin resonance performed at TRIUMF (Vancouver) and elastic and inelastic neutron scattering measurements performed at the DCS (NIST) and D7 (ILL). From all the above measurements it can be concluded that the new Be langasites exhibit net antiferromagnetic interactions at low-temperatures with clear signs of diffuse scattering for Nd3Ga3Ge2BeO14 using inelastic neutron scattering measurements. There was no evidence of magnetic long-range ordering down to as low as 0.025 K. Based on the obtained measurements these new Be-langasite compounds can be classified as potential spin liquid candidates. / February 2017

This work presents macroscopic and microscopic experiments of the disordered hexagonal double perovskite BaTi1/2Mn1/2O3, in order to characterize its electronic, magnetic and structural properties to support the possibility that this system hosts a spin liquid phase. Such assumption is based on the absence of a transition to a magnetically ordered phase in the magnetic and thermodynamic measurements, which points to a strong magnetic frustration in this material. In addition, it is observed the formation of a correlated spin state. To characterize this correlation, we resorted to Muon Spin Resonance (µSR) experiments to measure the low temperature spin dynamics. The zero field µSR relaxation regime displays dynamic magnetism down to T = 0.019 K and longitudinal field experiments support as well that dynamic magnetism persists at low temperatures, a behavior expected for a spin liquid system. The magnetic behavior of BaTi1/2Mn1/2O3 consists in the high temperature physics being dominated by the presence of magnetic trimers, magnetic dimers, and orphan spins. At lower temperatures, the effective magnetic degrees of freedom, composed by orphan spins and magnetic trimers, are correlated but no phase transition is detected down to T = 0.1 K, despite the effective exchange couplings between magnetic trimers and orphan spins being -8.5 K, resulting in a magnetic frustration parameter of at least 85. The possibility that disorder is responsible for the spin liquid ground state is discussed, however, other scenarios are not totally discarded. For example, the possibility that the measured state is not the true ground state, which could lie at even lowers temperatures or the possible formation of a spin glass state. This work raises questions that are not easy to answer. Ultimately, the growth of a single crystal is necessary to continue the characterization of BaTi1/2Mn1/2O3. Besides, theoretical and experimental developments in this field of research are needed to find a more direct and conclusive way to characterize the magnetic phases in this complex material. / Neste trabalho apresento dados experimentais macroscópicos e microscópicos da peroviskita hexagonal dupla BaTi1/2Mn1/2O3, a fim de caracterizar sua estrutura eletrônica, magnética e cristalina para embasar a possibilidade deste sistema apresentar uma fase de líquido de spin. Esta hipótese está baseada na ausência de transição para uma fase magneticamente ordenada nas medidas magnéticas e termodinâmicas, que apontam para uma forte frustração magnética neste material. Além disso, é observada a formação de um estado de spins correlacionados. Para caracterizar esta correlação, recorremos para experimentos de ressonância de múons (µSR) para medir a dinâmica de spins em baixas temperaturas. Dados de µSR para campo magnético nulo mostram em seu regime de relaxamento um magnetismo dinâmico para temperaturas tão baixas quanto T = 0.019 K, adicionalmente, experimentos com campo magnético longitudinal aplicado apontam também que o magnetismo dinâmico persiste em baixas temperaturas, um comportamento esperado para um sistema de líquido de spin. O comportamento magnético do BaTi1/2Mn1/2O3 consiste na física de altas temperaturas sendo dominada pela presença de trimers magnéticos, dimers magnéticos e spins órfãos. Para temperaturas mais baixas, os graus de liberdade magnéticos são efetivamente compostos por spins órfãos e trimers magnéticos, que estão correlacionados mas nenhuma transição de fase é detectada para temperaturas tão baixas quanto T = 0.1 K, mesmo que a constante de interação efetiva entre os spins órfãos e os trimers magnéticos seja -8.5 K, resultando num fator de frustração magnética de ao menos 85. A possibilidade da desordem ser responsável pelo estado fundamental de líquido de spin é discutida, no entanto, outros cenários não estão totalmente descartados, por exemplo, a possibilidade de que o estado medido não seja o verdadeiro estado fundamental, e que este estaria em temperaturas ainda mais baixas ou a possível formação de um estado de vidro de spin. Este trabalho levanta questões que não são fáceis de responder. Por fim, o crescimento de uma amostra monocristalina é necessário para continuar a caracterização do BaTi1/2Mn1/2O3. Ademais, desenvolvimentos de cunho teórico e experimental neste campo de pesquisa são necessários para encontrar um método mais direto e conclusivo para caracterizar a fase magnética neste material complexo.

Thesis advisor: Ziqiang Wang / Exotic phases and associated phase transitions in low dimensions have been a fascinating frontier and a driving force in modern condensed matter physics since the 80s. Due to strong correlation effect, they are beyond the description of mean-field theory based on a single-particle picture and Landau's symmetry-breaking theory of phase transitions. These new phases of matter require new physical quantities to characterize them and new languages to describe them. This thesis is devoted to the study on exotic phases of correlated electrons in two spatial dimensions. We present the following efforts in understanding two-dimensional exotic phases: (1) Using Zn vertex algebra, we give a complete classification and characterization of different one-component fractional quantum Hall (FQH) states, including their ground state properties and quasiparticles. (2) In terms of a non-unitary transformation, we obtain the exact form of statistical interactions between composite fermions in the lowest Landau level (LLL) with v=1/(2m), m=1,2... By studying the pairing instability of composite fermions we theoretically explains recently observed FQHE in LLL with v=1/2,1/4. (3) We classify different Z2 spin liquids (SLs) on kagome lattice in Schwinger-fermion representation using projective symmetry group (PSG). We propose one most promising candidate for the numerically discovered SL state in nearest-neighbor Heisenberg model on kagome lattice}. (4) By analyzing different Z2 spin liquids on honeycomb lattice within PSG classification, we find out the nature of the gapped SL phase in honeycomb lattice Hubbard model, labeled sublattice pairing state (SPS) in Schwinger-fermion representation. We also identify the neighboring magnetic phase of SPS as a chiral-antiferromagnetic (CAF) phase and analyze the continuous phase transition between SPS and CAF phase. For the first time we identify a SL called 0-flux state in Schwinger-boson representation with one (SPS) in Schwinger-fermion representation by a duality transformation. (5) We show that when certain non-collinear magnetic order coexists in a singlet nodal superconductor, there will be Majorana bound states in vortex cores/on the edges of the superconductor. This proposal opens a window for discovering Majorana fermions in strongly correlated electrons. (6) Motivated by recent numerical discovery of fractionalized phases in topological flat bands, we construct wavefunctions for spin-polarized fractional Chern insulators (FCI) and time reversal symmetric fractional topological insulators (FTI) by parton approach. We show that lattice symmetries give rise to different FCI/FTI states even with the same filling fraction. For the first time we construct FTI wavefunctions in the absence of spin conservation which preserve all lattice symmetries. The constructed wavefunctions also set up the framework for future variational Monte Carlo simulations. / Thesis (PhD) — Boston College, 2011. / Submitted to: Boston College. Graduate School of Arts and Sciences. / Discipline: Physics.

This work presents macroscopic and microscopic experiments of the disordered hexagonal double perovskite BaTi1/2Mn1/2O3, in order to characterize its electronic, magnetic and structural properties to support the possibility that this system hosts a spin liquid phase. Such assumption is based on the absence of a transition to a magnetically ordered phase in the magnetic and thermodynamic measurements, which points to a strong magnetic frustration in this material. In addition, it is observed the formation of a correlated spin state. To characterize this correlation, we resorted to Muon Spin Resonance (µSR) experiments to measure the low temperature spin dynamics. The zero field µSR relaxation regime displays dynamic magnetism down to T = 0.019 K and longitudinal field experiments support as well that dynamic magnetism persists at low temperatures, a behavior expected for a spin liquid system. The magnetic behavior of BaTi1/2Mn1/2O3 consists in the high temperature physics being dominated by the presence of magnetic trimers, magnetic dimers, and orphan spins. At lower temperatures, the effective magnetic degrees of freedom, composed by orphan spins and magnetic trimers, are correlated but no phase transition is detected down to T = 0.1 K, despite the effective exchange couplings between magnetic trimers and orphan spins being -8.5 K, resulting in a magnetic frustration parameter of at least 85. The possibility that disorder is responsible for the spin liquid ground state is discussed, however, other scenarios are not totally discarded. For example, the possibility that the measured state is not the true ground state, which could lie at even lowers temperatures or the possible formation of a spin glass state. This work raises questions that are not easy to answer. Ultimately, the growth of a single crystal is necessary to continue the characterization of BaTi1/2Mn1/2O3. Besides, theoretical and experimental developments in this field of research are needed to find a more direct and conclusive way to characterize the magnetic phases in this complex material. / Neste trabalho apresento dados experimentais macroscópicos e microscópicos da peroviskita hexagonal dupla BaTi1/2Mn1/2O3, a fim de caracterizar sua estrutura eletrônica, magnética e cristalina para embasar a possibilidade deste sistema apresentar uma fase de líquido de spin. Esta hipótese está baseada na ausência de transição para uma fase magneticamente ordenada nas medidas magnéticas e termodinâmicas, que apontam para uma forte frustração magnética neste material. Além disso, é observada a formação de um estado de spins correlacionados. Para caracterizar esta correlação, recorremos para experimentos de ressonância de múons (µSR) para medir a dinâmica de spins em baixas temperaturas. Dados de µSR para campo magnético nulo mostram em seu regime de relaxamento um magnetismo dinâmico para temperaturas tão baixas quanto T = 0.019 K, adicionalmente, experimentos com campo magnético longitudinal aplicado apontam também que o magnetismo dinâmico persiste em baixas temperaturas, um comportamento esperado para um sistema de líquido de spin. O comportamento magnético do BaTi1/2Mn1/2O3 consiste na física de altas temperaturas sendo dominada pela presença de trimers magnéticos, dimers magnéticos e spins órfãos. Para temperaturas mais baixas, os graus de liberdade magnéticos são efetivamente compostos por spins órfãos e trimers magnéticos, que estão correlacionados mas nenhuma transição de fase é detectada para temperaturas tão baixas quanto T = 0.1 K, mesmo que a constante de interação efetiva entre os spins órfãos e os trimers magnéticos seja -8.5 K, resultando num fator de frustração magnética de ao menos 85. A possibilidade da desordem ser responsável pelo estado fundamental de líquido de spin é discutida, no entanto, outros cenários não estão totalmente descartados, por exemplo, a possibilidade de que o estado medido não seja o verdadeiro estado fundamental, e que este estaria em temperaturas ainda mais baixas ou a possível formação de um estado de vidro de spin. Este trabalho levanta questões que não são fáceis de responder. Por fim, o crescimento de uma amostra monocristalina é necessário para continuar a caracterização do BaTi1/2Mn1/2O3. Ademais, desenvolvimentos de cunho teórico e experimental neste campo de pesquisa são necessários para encontrar um método mais direto e conclusivo para caracterizar a fase magnética neste material complexo.

In this thesis we present results from quantum Monte Carlo for the fully-frustrated honeycomb lattice. The XXZ model is of interest in the classical limit, as there is a mapping between the classical fully-frustrated honeycomb Ising model groundstates and the classical hard-core dimer model groundstate. The aim of this work is to explore the effect of quantum fluctuations on the fully-frustrated honeycomb model to see what sort of interesting physics arises. One might expect unusual physics due to the quantum hard-core dimer model, where interesting physics are known to exist. This is because there is a duality mapping between the classical dimer model and the classical fully-frustrated honeycomb Ising model. Indeed, by studying the fully-frustrated honeycomb XXZ model we find that in some cases the system orders into crystal-like structures, a case of order-by-disorder. The most interesting case, when the frustrating bonds are chosen randomly, reveals to us a novel state without any discernible order while at the same time avoiding the freezing one would expect of a glass. This state is a featureless system lacking low temperature magnetic susceptibility---a candidate ``quantum spin liquid''. Future work that might more easily measure quantum spin liquid criteria is suggested.