Thesis (Ph. D.)--University of Glasgow, 1998. / Print version also available.

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Thesis (Ph. D.)--Virginia Polytechnic Institute and State University, 1993. / Vita. Abstract. Includes bibliographical references (leaves 132-134). Also available via the Internet.

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A dissertation submitted in fulfillment of the requirements for the degree of Masters in Science in the, The Structured Light Group Department of Physics, University of the Witwatersrand, Johannesburg, 2018 / At the quantum level, entities and systems often behave counter-intuitively which we have come to describe with wave-particle duality. Accordingly, a particle that moves definitively from one position to another in our classical experience does something completely different on the quantum scale. The particle is not localized at any one position, but spreads out over all the possibilities as it moves. Here the particle can interfere with itself with wave-like propagation and generate, what is known as a Quantum Walk. This is the quantum mechanical analogue of the already well-known and used Random Walk where the particle takes random steps across the available positions, building up a series of random paths. The mechanics behind the random walk has already proved largely useful in many fields, from finance to simulation and computation. Analogously, the quantum walk promises even greater potential for development. Here, with many of the algorithms already developed, it would allow computations to outperform current classical methods on an unprecedented level. Additionally, by implementing these mechanics on various levels, it is possible to simulate and understand various quantum mechanical systems and phenomenon. This phenomenon consequently represents a significant advancement in several fields of study. Although there has been considerable theoretical development of this phenomenon, its potential now lies in implementing these quantum walks physically. Here, a physical system is required such that the quantum walk may be sustainably achieved, easily detected and dynamically altered as needed. Many systems have been subsequently proposed and demonstrated, but the criteria for a useful quantum walk leaves many such avenues lacking with the largest number of steps yet to reach 100 to the best of our knowledge. As a result, we explored a classical take on the quantum walk, utilizing the wave properties of light to achieve analogous mechanics with the advantage of the increased degree of control and robustness. While such an approach is not new, we considered a particular method where the quantum walk could be implemented in the spatial modes of light. By exploiting the non-separability (classical entanglement) of polarization and orbital angular momentum, such a classical quantum walk could be realized with greater intuitive implications and the potential for further study into the quantum mechanical nature of this phenomenon, over and above that of the other schemes, by walking the quantum-classical divide. The work presented here subsequently centres on experimentally achieving a quantum walk with classically entangled light for further development and useful implementation. Moreover, this work focused on demonstrating the sustainability, control and robustness necessary for this scheme to be beneficial for future development. In Chapter 1, an intuitive introduction is presented, highlighting the mechanics of this phenomenon that make it different from the Random walk counterpart. We also explore why this phenomenon is of such great importance with an overview of applications that physical implementation can result in. A more in-depth look into the dynamics and mathematical aspects of this walk is found in Chapter 2. Here a detailed look into the mechanisms behind the walk is taken with mathematical analysis. Furthermore, the subsequent differences and implications associated viii with utilizing classical light is explored, answering the question of what is quantum about the quantum walk. As the focus of this chapter is largely cemented in establishing a solid theoretical background, we also look into the physics behind classical light and develop the theoretical basis in the direction of structured light, with an emphasis on establishing classically entangled beams. Chapters 3 and 4 present the experimental work done throughout the course of this dissertation. With Chapter 3 we establish and characterize the elements necessary for obtaining a quantum walk in the spatial modes of light by utilizing waveplates as coins, q-plates as step operators and entanglement generators as well as mode sorters in a detection system. We also look into the characteristics of the modes that will be produced with these elements, allowing the propagation properties of the beam to be experimentally accounted for. In Chapter 4, we examine the experimental considerations of how to achieve a realistic and sustainable quantum walk. Here, we consider and implement the scheme proposed by Goyal et. al. [] where a light pulse follows a looped path, allowing the physical resources to be constant throughout the walk. We also show the experimental limitations of the equipment being utilized and the various steps needed to compensate. Finally, we not only implement a quantum walk with classically entangled light for the first time, but also demonstrate the flexibility of the system. Here, we achieve a maximum of 8 steps and show 5 different types of walks with varying dynamics and symmetry. The last chapter (Chapter 5) gives a summary of the dissertation in context of the goals and achievements of this work. The outlook and implications of these results are discussed and future steps outlined for extending this scheme into a highly competitive alternative for viable implementation of quantum walks for computing and simulation. / XL2019

In this work, the connection between quantum K-theory and quantum integrable systems is studied. Using quasimap spaces the quantum equivariant K-theory of Naka- jima quiver varieties is defined. For every tautological bundle in the K-theory there exists its one-parametric deformation, referred to as quantum tautological bundle. For specific cases of cotangent bundles to Grassmannians and flag varieties it is proved that the spectrum of operators of quantum multiplication by these quantum classes is governed by the Bethe ansatz equations for the inhomogeneous XXZ spin chain. It is also proved that each such operator corresponds to the universal elements of quantum group U􏰁(sln). In particular, the Baxter operator for the XXZ spin chain is identified with the operator of quantum multiplication by the exterior algebra of the tautological bundle. An explicit universal combinatorial formula for this operator is found in the case of U􏰁(sl2). The relation between quantum line bundles and quantum dynamical Weyl group is shown. This thesis is based on works [37] and [24].

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In this thesis, we study the operator algebraic structure of various classes of unimodular free quantum groups, including thefree orthogonal quantum groups $O_n^+$, free unitary quantum groups $U_n^+$, and trace-preserving quantum automorphism groups associated to finite dimensional C$^\ast$-algebras. The first objective of this thesis to establish certain approximation properties for the reduced operator algebras associated to the quantum groups $\G = O_n^+$ and $U_n^+$, ($n \ge 2$). Here we prove that the reduced von Neumann algebras $L^\infty(\G)$ have the Haagerup approximation property, the reduced C$^\ast$-algebras $C_r(\G)$ have Grothendieck's metric approximation property, and that the quantum convolution algebras $L^1(\G)$ admit multiplier-bounded approximate identities. We then go on to study trace-preserving quantum automorphism groups $\G$ of finite dimensional C$^\ast$-algebras $(B, \psi)$, where $\psi$ is the canonical trace on $B$ induced by the regular representation of $B$. Here, we extend several known results for free orthogonal and free unitary quantum groups to the setting of quantum automorphism groups. We prove that the discrete dual quantum groups $\hG$ have the property of rapid decay, the von Neumann algebras $L^\infty(\G)$ have the Haagerup approximation property, and that $L^\infty(\G)$ is (in most cases) a full type II$_1$-factor. As applications of these and other results, we deduce the metric approximation property, exactness, simplicity and uniqueness of trace for the reduced C$^\ast$-algebras $C_r(\G)$, and the existence of multiplier-bounded approximate identities for the convolution algebras $L^1(\G)$. We also show that when $B$ is a full matrix algebra, $L^\infty(\G)$ is an index $2$ subfactor of $L^\infty(O_n^+)$, and thus solid and prime. Finally, we investigate strong Haagerup inequalities in the context of quantum symmetries arising from actions of free quantum groups on non-commutative random variables. We prove a generalization of the strong Haagerup inequality for $\ast$-free R-diagonal families due to Kemp and Speicher, and apply this result to study strong Haagerup inequalites for the free unitary quantum groups. / Thesis (Ph.D, Mathematics & Statistics) -- Queen's University, 2012-07-31 12:45:57.767

Thesis (Ph. D.)--University of Oregon, 2006. / Typescript. Includes vita and abstract. "In this dissertation I investigate Poisson structures on symmetric and exterior algebras of modules over complex reductive Lie algebras. I use the results to study the braided symmetric and exterior algebras"--P. 1. Includes bibliographical references (leaves 150-152). Also available for download via the World Wide Web; free to University of Oregon users.

This thesis is divided into the following three parts. <b>A categorical reconstruction of crystals and quantum groups at</b> q = 0. The quantum co-ordinate algebra A_q(&gfr;) associated to a KacMoody Lie algebra g forms a Hopf algebra whose comodules are direct sums of finite dimensional irreducible U_q(&gfr;) modules. In Part I we investigate whether an analogous result is true when q = 0. We classify crystal bases as coalgebras over a comonadic functor on the category of pointed sets and encode the monoidal structure of crystals into a bicomonadic structure. In doing this we prove that there is no coalgebra in the category of pointed sets whose comodules are equivalent to crystal bases. We then construct a bialgebra over &Zopf; whose based comodules are equivalent to crystals, which we conjecture is linked to Lusztig's quantum group at v = ∞. <b>A Tannakian Reconstruction Theorem for IndBanach Spaces.</b> Classically, Tannaka-Krein duality allows us to reconstruct a (co)algebra from its category of representation. In Part II we present an approach that allows us to generalise this theory to the setting of Banach spaces. This leads to several interesting applications in the directions of analytic quantum groups, bounded cohomology and Galois descent. A large portion of Part II is dedicated to such examples. <b>On analytic analogues of quantum groups.</b> In Part III we present a new construction of analytic analogues of quantum groups over non-Archimedean fields and construct braided monoidal categories of their representations. We do this by constructing analytic Nichols algebras and use Majid's double-bosonisation construction to glue them together. We then go on to study the rigidity of these analytic quantum groups as algebra deformations of completed enveloping algebras through bounded cohomology. This provides the first steps towards a p-adic Drinfel'd-Kohno Theorem, which should relate this work to Furusho's p-adic Drinfel'd associators. Finally, we adapt these constructions to working over Archimedean fields.