The open spin-1/2 XXZ quantum spin chain with general integrable boundary terms is a fundamental integrable model. Finding a Bethe Ansatz solution for this model has been a subject of intensive research for many years. Such solutions for other simpler spin chain models have been shown to be essential for calculating various physical quantities, e.g., spectrum, scattering amplitudes, finite size corrections, anomalous dimensions of certain field operators in gauge field theories, etc. The first part of this dissertation focuses on Bethe Ansatz solutions for open spin chains with nondiagonal boundary terms. We present such solutions for some special cases where the Hamiltonians contain two free boundary parameters. The functional relation approach is utilized to solve the models at roots of unity, i.e., for bulk anisotropy values eta = i pi/(p+1) where p is a positive integer. This approach is then used to solve open spin chain with the most general integrable boundary terms with six boundary parameters, also at roots of unity, with no constraint among the boundary parameters. The second part of the dissertation is entirely on applications of the newly obtained Bethe Ansatz solutions. We first analyze the ground state and compute the boundary energy (order 1 correction) for all the cases mentioned above. We extend the analysis to study certain excited states for the two-parameter case. We investigate low-lying excited states with one hole and compute the corresponding Casimir energy (order 1/N correction) and conformal dimensions for these states. These results are later generalized to many-hole states. Finally, we compute the boundary S-matrix for one-hole excitations and show that the scattering amplitudes found correspond to the well known results of Ghoshal and Zamolodchikov for the boundary sine-Gordon model provided certain identifications between the lattice parameters (from the spin chain Hamiltonian) and infrared (IR) parameters (from the boundary sine-Gordon S-matrix) are made.

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No. of bitstreams: 2 Dissertação - Andesson Brito Nascimento - 2015.pdf: 4640566 bytes, checksum: dbcca8bfca43a95c51641cfa230b0285 (MD5) license_rdf: 23148 bytes, checksum: 9da0b6dfac957114c6a7714714b86306 (MD5) Previous issue date: 2015-07-24 / Coordenação de Aperfeiçoamento de Pessoal de Nível Superior - CAPES / Correlations are ubiquitous in nature and have played an extremely important role in human life for a long time. For example, in economy, correlations between price and demand are extremely important for a businessman (or even a government) to make decisions regarding their investment policy. In the field of biology, genetic correlations are central to follow individual characteristics. The relationship between income distribution and crime rate is just one example coming from the social sciences. Mathematically, correlation is a number that describes the degree of relationship between two variables. In the classical domain, this number can be computed in the context of information theory, developed by Shannon in 1948. Focusing on the subject of the present work, the discussion regarding the quantum nature of the correlations permeates physics since Einstein, Podolski and Rosen published their famous article criticizing quantum mechanics. Since then, the so-called quantum correlations have been shown to be a very important tool in the study of many-bodies physics. Another feature of many-body physics is that certain systems, under certain conditions, exhibit what we call quantum phase transition. Such transitions are analogous to the classical transitions, but being governed by purely quantum fluctuations and, as such, may occur at zero temperature, unlike the former, which are guided by thermal fluctuations. One of the main phenomenon that characterizes these transitions is the fact that the correlation length (defined between two subsystems of the global system) highly increases at the transition point. This means that such subsystems can be strongly correlated even if they are separated by a large distance. The main goal of the present work is the study of quantum correlations, specifically the entanglement and the local quantum uncertainty (LQU), in systems presenting one or more quantum phase transitions. Specifically, we consider three models of spin chains: 1) The XY and the XY T, which describes chains of spins- 1=2 —the second considering three spins interaction while the first one takes into account only pairwise interactions; 2) A model describing a chain formed by bosonic spins, i.e. particles with spin-1. As a general conclusion, quantum correlation provides a very powerful tool for the study of critical phenomena, providing, among other things, a means to identify a quantum phase transition. / As correlações são onipresentes na natureza e têm desempenhado um papel extremamente importante na vida humana por um longo tempo. Por exemplo, na economia correlações entre oferta e demanda são extremamente importantes para um homem de negócios (ou mesmo para um governo) tomar decisões à respeito de sua política de investimento. No campo da biologia, correlações genéticas são fundamentais para seguirmos características individuais. A relação entre distribuição de renda e taxa de criminalidade é apenas um dos exemplo vindos das Ciências Sociais. De um modo geral, a correlação é uma quantidade que descreve o grau de relação entre duas variáveis. No domínio clássico, essa quantidade pode ser medida no âmbito da teoria da informação, desenvolvida por Shannon em 1948. Focando no assunto do presente trabalho, a discussão sobre a natureza quântica das correlações permeia a física desde que Einstein, Podolski e Rosen publicaram seu famoso artigo criticando a mecânica quântica. Desde então, as chamadas correlações quânticas têm se mostrado uma ferramenta muito importante no estudo da Física de muitos corpos. Outra característica da Física de muitos corpos é que certos sistemas, em certas condições, exibem o que chamamos de transição de fase quântica. Tais transições são análogas às transições clássicas, mas sendo governadas por flutuações de natureza puramente quântica, podendo ocorrer à temperatura zero, ao contrário das primeiras, que são guiadas por flutuações térmicas. Um dos principais fenômenos que caracterizam estas transições é o fato de que o comprimento de correlação (definido entre dois subsistemas do sistema global) torna-se de longo alcance no ponto de transição. Isso significa que tais subsistemas podem estar fortemente correlacionados mesmo estando separados por uma grande distância. O objetivo deste trabalho é o estudo de correlações quânticas, mais especificamente do emaranhamento e da incerteza local quântica (LQU), em cadeias de spin que apresentem uma ou mais transições quânticas de fase. Especificamente, estudamos três modelos de cadeias de spin: Os modelos XY e XY T, que são cadeias formadas por spins-1=2, sendo que o segundo considera interação entre três spins enquanto o primeiro somente entre pares; um modelo formado por partículas bosônicas de spin-1. Como conclusão geral, temos que as correlações quânticas fornecem uma ferramenta muito boa para o estudo de fenômenos críticos, oferecendo, entre outros, um meio de identificarmos uma transição quântica de fase.

Indiana University-Purdue University Indianapolis (IUPUI) / We describe a reproduction procedure which, given a solution of the gl(m|n) Gaudin Bethe ansatz equation associated to a tensor product of polynomial modules, produces a family P of other solutions called the population. To a population we associate a rational pseudodifferential operator R and a superspace W of rational functions. We show that if at least one module is typical then the population P is canonically identified with the set of minimal factorizations of R and with the space of full superflags in W. We conjecture that the singular eigenvectors (up to rescaling) of all gl(m|n) Gaudin Hamiltonians are in a bijective correspondence with certain superspaces of rational functions. We establish a duality of the non-periodic Gaudin model associated with superalgebra gl(m|n) and the non-periodic Gaudin model associated with algebra gl(k). The Hamiltonians of the Gaudin models are given by expansions of a Berezinian of an (m+n) by (m+n) matrix in the case of gl(m|n) and of a column determinant of a k by k matrix in the case of gl(k). We obtain our results by proving Capelli type identities for both cases and comparing the results. We study solutions of the Bethe ansatz equations of the non-homogeneous periodic XXX model associated to super Yangian Y(gl(m|n)). To a solution we associate a rational difference operator D and a superspace of rational functions W. We show that the set of complete factorizations of D is in canonical bijection with the variety of superflags in W and that each generic superflag defines a solution of the Bethe ansatz equation. We also give the analogous statements for the quasi-periodic supersymmetric spin chains.

The intention with this thesis is to investigate a dimer in a spin chain. Inorder to do that, a model from Z2-gauge theory is taken as the theoretical motivation to construct a discrete lattice with Ising spin properties. A dimer is then allowed to exist indirectly in the empty space between sites. We choose to tackle the problem through a quantum mechanical approach in 1+1-dimensions, distancing ourselves from the original description in quantum field theory. The exposition begins by reviewing the spatial construction of the entire chain as well as its components, and ends with a discussion of time development where the main concern is dispersion in addition to reflection against a static charge.

京都大学 / 新制・課程博士 / 博士(理学) / 甲第23731号 / 理博第4821号 / 新制||理||1689(附属図書館) / 京都大学大学院理学研究科化学専攻 / (主査)教授 谷村 吉隆, 教授 林 重彦, 教授 渡邊 一也 / 学位規則第4条第1項該当 / Doctor of Science / Kyoto University / DGAM

Quantum simulations, where controllable quantum systems are used to simulate other quantum systems, originally proposed by Richard Feynman, are one of the most remarkable applications of quantum information science. Compared to computation, quantum simulations require much less number of qubits for the m to be practical. In the work described in this thesis, we have performed a few quantum simulations of small quantum systems using Nuclear Magnetic Resonance(NMR) techniques. These simulations have been used to experimentally demonstrate the underlying interesting quantum protocols. All the experiments presented have been carried out using liquid-state or liquid crystal NMR. Numerical pulse optimization techniques have been utilized in some of the experiments, to achieve better control over the spin systems. The first chapter contains “Introduction” to quantum information processing, NMR, and numerical pulse optimization techniques. In chapter 2, we describe quantum simulation of a 3-spin Heisenberg-XY spin chain having only nearest neighbour interactions. Recently, spin chains having pre-engineered short-range interactions have been proposed to efficiently transfer quantum information between different parts of a quantum information processor. Other important proposals involving these spin chains include generating entangled states and universal quantum computation. However, such engineered interactions do not occur naturally in any system. In such a scenario, the experimental viability of these proposals can be tested by simulating the spin chains in other controllable quantum systems. In this work, we first theoretically study the time evolution of bipartite and tripartite entanglement measures for a 3-spin open ended XY spin chain. Then, by simulating the XY interactions in a 3-spin nuclear spin system, we experimentally generate, (i)a bipartite maximally(pseudo-)entangled state(Bell state) between end qubits, and(ii) multipartite(pseudo-)entangled states(Wand GHZ states),starting from separable pseudo-pure states. Bell state has been generated by using only the natural unitary evolution of the XY spin chain. W-state and GHZ-state have been generated by applying a single-qubit rotation to the second qubit, and a global rotation of all the three qubits respectively after the unitary evolution of the spin chain. In chapter 3, we simulate a 3-spin quantum transverse Ising spin system in a triangular configuration, and show that multipartite quantum correlations can be used to distinguish between the frustrated and non-frustrated regimes in the ground state of this spin system. The ground state of the spin system has been prepared by using adiabatic state preparation method. Gradient ascent pulse engineering technique has been utilized to efficiently realize the adiabatic evolution of the spin system. To analyse the experimental ground state of the system, we employ two different multipartite quantum correlation measures, generated from monogamy studies of bipartite quantum correlations. Chapter 4 contains a digital quantum simulation of the mirror inversion propagator corresponding to the time evolution of an XY spin chain. This simulation has been used to experimentally demonstrate the mirror inversion of quantum states, proposed by Albanese et al.[Phys.Rev.Lett.93,230502(2004)], by which entangled states can be transferred from one end of the chain to the other end. The experiments have been performed in a 5-qubit dipolar coupled nuclear spin system. For simulation, we make use of the recently proposed unitary operator decomposition algorithm along with the numerical pulse optimization techniques, which assisted in achieving high experimental fidelities. Chapter 5 contains a digital quantum simulation of the unitary propagator of a transverse Ising spin chain, which has been used to experimentally demonstrate the perfect state transfer protocol of Di Franco et al. [Phys.Rev.Lett.101,230502(2008)]. The importance of this protocol arises due to the fact that it achieves perfect state transfer from one end of the chain to the other end without the necessity of initializing the intermediate spins of the chain, whereas most of the previously proposed protocols require initialization. The experiments have been performed in a 3-spin nuclear spin system. The simulation has also been used to demonstrate the generation of a GHZ state.

This thesis is concerned with the collective dynamics in different spin chains and spin ensembles in solid-state materials. The focus is on the manipulation of electron spins, through spin-spin and spin-photon couplings controlled by voltage potentials or electromagnetic fields. A brief review of various systems is provided to describe the possible physical implementation of the ideas, and also outlines the basis of the adopted effective interaction models. The first two ideas presented explore the collective behaviour of non-interacting spin chains with external couplings. One focuses on mapping the identical state of spin-singlet pairs in two currents onto two distant, static spins downstream, creating distributed entanglement that may be accessed. The other studies a quantum memory consisting of an array of non-interacting, static spins, which may encode and decode multiple flying spins. Both chains could effectively `enhance' weak couplings in a cumulative fashion, and neither scheme requires active quantum control. Moreover, the distributed entanglement generated can offer larger separation between the qubits than more conventional protocols that only exploit the tunnelling effects between quantum dots. The quantum memory can also `smooth' the statistical fluctuations in the effects of local errors when the stored information is spread. Next, an interacting chain of static spins with nearest-neighbour interactions is introduced to connect distant end spins. Previously, it has been shown that this approach provides a cubic speed-up when compared with the direct coupling between the target spins. The practicality of this scheme is investigated by analysing realistic error effects via numerical simulations, and from that perspective relaxation of the nearest-neighbour assumption is proposed. Finally, a non-interacting electron spin ensemble is reviewed as a quantum memory to store single photons from an on-chip stripline cavity. It is then promoted to a full quantum processor, with major error effects analysed.

This thesis explores connections between the Gaudin Hamiltonians in type A and the combinatorics of tableaux. The cactus group acts on standard tableaux via the Schützenberger involution. We show in this thesis that the action of the cactus group on standard tableaux can be recovered as a monodromy action of the cactus group on the simultaneous spectrum of the Gaudin Hamiltonians. More precisely, we consider the action of the Bethe algebra, which contains the Gaudin Hamiltonians, on the multiplicity space of a tensor product of irreducible glr-modules. The spectrum of this algebra forms a flat and finite family over M0,n+1(C). We use work of Mukhin, Tarasov and Varchenko, who link this spectrum to certain Schubert intersections, and work of Speyer, who extends these Schubert intersections to a flat and finite map over the entire moduli space of stable curves M0,n+1(C). We show the monodromy over the real points M0,n+1(R) can be identified with the action of the cactus group on a tensor product of irreducible glr-crystals. Furthermore we show this identification is canonical with respect to natural labelling sets on both sides.