Thesis (MSc)--Stellenbosch University, 2004. / ENGLISH ABSTRACT: In this thesis, generalized Dyson boson-fermion mappings are considered. These are techniques used in the analysis of the quantum many-body problem, and are instances of so-called boson expansion methods. A generalized Dyson boson-fermion mapping, or a Dyson mapping for short, is a one-to-one linear but non-unitary operator that can be applied to vectors representing the states of a many-fermion system. A vector representing a fermion system maps onto a vector that is most naturally interpreted as representing a state of a many-body system that contains both bosons and fermions. The motivation for doing such a mapping is the hope that the mapping will reveal some property of the system that simplifies its analysis and that was hidden in the original form. The aims of this thesis are 1. to review the theory of generalized Dyson boson-fermion mappings, 2. by considering a tutorial example, to demonstrate that it is feasible to implement the theory and 3. to find a useful application for a generalized Dyson boson-fermion mapping, by considering a non-trivial model, namely the Richardson model for superconductivity. The realization of the first two aims mainly involve the collecting together of ideas that have already appeared in the literature, into one coherent text. Some subtle points that were treated only briefly due to space restrictions in the journal publications where the theory was first expounded, are elaborated on in the present work. On the other hand, the analysis of the Richardson Hamiltonian that uses a Dyson mapping, goes beyond what has already appeared in the literature. It is the first time that a boson expansion technique is implemented for a system where the roles of both collective and non-collective fermion pairs are important. (The Dyson mapping associates bosons with Cooper pairs, while the fermions not bound in Cooper pairs result in fermions being present in the mapped system as well.) What is found is that the Dyson mapping uncovers non-trivial properties of the system. These properties aid the construction of time-independent perturbation expansions for the stationary states of the system, as well as time-dependent expansions for transition amplitudes between states. The time-independent expansions agree with results that other authors obtained through methods other than boson expansions. The time-dependent expansions, that one would be hard-pressed to develop without a Dyson mapping, might in future prove useful in understanding aspects of the dynamics of ultracold fermi gases, when time-dependent magnetic fields are used to vary the atom-atom interaction strenght. / AFRIKAANSE OPSOMMING: In hierdie tesis word veralgemeende Dyson boson-fermion-afbeeldings ondersoek. Hierdie afbeeldings word gebruik in die analise van die kwantum veeldeeltjie probleem, en is voorbeelde van sogenaamde boson-uitbreidingstegnieke. 'n Veralgemeende Dyson bosonfermion- afbeelding, of kortweg 'n Dyson afbeelding, is 'n een-tot-een, lineêre maar nie-unitêre operator wat inwerk op vektore wat toestande verteenwoordig van 'n veel-fermion sisteem. 'n Vektor wat 'n fermionsisteem verteenwoordig word so afgebeeld op 'n vektor waarvoor die mees natuurlike interpretasie is dat dit 'n toestand verteenwoordig van 'n sisteem waarin beide bosone en fermione aanwesig is. So 'n afbeelding word gewoonlik gemaak in die hoop dat eienskappe van die sisteem, wat versteek was in die oorspronklike weergawe, voor-die-hand-liggend is na die afbeelding. Hierdie tesis het ten doel 1. om die teorie van veralgemeende Dyson boson-fermion-afbeeldings te hersien, 2. om 'n eenvoudige voorbeeld deur te werk, en so te demonstreer dat die teorie sonder moeite geïmplimenteer kan word en 3. om 'n nuttige toepassing te vind vir 'n veralgemeende Dyson boson-fermion-afbeelding deur 'n nie-triviale model, naamlik die Richardson model vir supergeleiding, te ondersoek. Die eerste twee van hierdie doelwitte behels hoofsaaklik dat idees wat reeds in die literatuur verskyn het, saamgevat word in een koherente teks. Sommige subtiele punte wat, vanwee beperkte ruimte, slegs kortliks bespreek is in die joernaalartikels waarin die teorie oorspronklik verskyn het, word in hierdie tesis meer breedvoering bespreek. Daarteenoor verteenwoordig die analise van die Richardson model met behulp van 'n Dyson afbeelding 'n nuwe bydra. Dit is naamlik die eerste keer dat 'n bosonuitbreiding ingespan word vir 'n sisteem waar sowel kollektiewe as nie-kollektiewe fermionpare 'n belangrike rol speel. (Die Dyson afbeelding assosieer bosone met die oorspronklike sisteem se Cooper pare, terwyl die fermione wat in die oorspronklike sisteem nie tot Cooper pare gebind is nie, sorg dat daar ook fermione teenwoordig is in die afgebeelde sisteem.) Ons vind dat die Dyson afbeelding nie-triviale eienskappe van die sisteem aan die lig bring. Hierdie eienskappe is nuttig vir die konstruksie van beide tyd-onafhanklike steuringsreekse vir die stasionêre toestande van die sisteem en vir tyd-afhanklike steuringsreekse vir oorgangsamplitudes tussen toestande. Die tyd-onafhanklike uitbreidings stem ooreen met resultate wat ander outeurs afgelei het sonder die gebruik van 'n Dyson afbeelding. Die tyd-afhanklike uitbreidings, wat kwalik afgelei kan word sonder 'n Dyson afbeelding, mag vorentoe nuttig wees om aspekte van die dinamika van baie koue Fermi gasse te verstaan, wanneer tydafhanklike magneetvelde gebruik word om die inter-atoomwisselwerking te manipuleer.

This thesis presents a study of two-dimensional electron systems in GaAs-(Al,Ga)As heterojunctions and quasi-two-dimensional electron and hole systems in graphite within the quantum Hall effect regime of low temperature and high magnetic field. This thesis covers three main sets of experimental work as well as details of the experimental methods (chapter 2) used and the background theory behind the observed results (chapter 1). The first experimental results presented in this thesis in chapter 3 focus on contactless measurement of the equilibrium magnetisation of sample A2268, a ten layer multiple quantum well sample. Fitting the shape of dHvA oscillations at various temperatures to different models for the density of states, various properties of the system can be estimated, such as the shape of the disorder-broadened density of states and the presence of a background density of states between the Landau levels. Chapter 4 focuses on measurements of the decay of induced circulating currents in the quasi-dissipationless quantum Hall regime in two samples, V0049 and T73. The induced current is measured via contactless measurement of the associated magnetic moment. The magnitude of the induced current is found to be affected by the sweep rate of the magnetic field and also the distance of approach. The decay of the induced currents is observed at several temperatures and for different magnetic field sweep rates and distances of approach. Decays are observed for up to several days at time, far longer than previously possible. Information about the rate of decay can be used to build a picture of the decay mechanisms present in the quantum Hall regime. The presence of a power-law decay regime indicates many decay mechanisms contribute to the decay of a circulating current in the quasi-dissipationless quantum Hall regime. Chapter 5 focuses on both contactless magnetometry and transport experiments carried out on a graphite sample. The experiments aim to confirm or dispute recent claims of Dirac fermions in graphite. Experiments are carried out at temperatures in the range 30 mK to ~4 K and at two different angles to the applied magnetic field. Phase analysis of both Shubnikov de Haas and de Haas van Alphen oscillations is used to distinguish between normal and Dirac fermions. Observation of quantum Hall effect displays the presence of a half-integer quantum Hall staircase similar to that observed in graphene.

There is now convincing evidence that the Standard Model of electroweak and strong interactions is not the end of the story but only a low energy effective theory. In particular, new flavour physics is required to explain the fermion mass spectrum. Most of the proposed extensions of the Standard Model fail to meet this criterion. We may hope that the LHC or some future colliders could help to clarify the situation by discovering new particles or spotting some unexpected events. In the meantime, more precise measurements of masses and mixing parameters could also play an important role. In this work, we do not aim at finding a new mechanism that could explain this spectrum, but we rather assume that fermion masses and mixings are calculable in a yet-to-be-found more fundamental theory. Our goal is to glean as much information as possible from the observed fermion masses and mixings in order to find some hidden structures that could significantly lower the number of free parameters and help us to get some clues about what could be this fundamental theory. We analyse first the various parametrizations of the flavour mixing and single out a specific decomposition. The parameters of this decomposition can be independently and accurately computed if we impose some simple textures to the Yukawa couplings. We propose then a straightforward combination of these interesting textures which reproduces quite well the observed quark flavour mixing. We study then the properties of a successful mass relation for the charged leptons. We propose some generalizations of this relation in order to be valid also for the neutrinos and the quarks. One of them successfully combines the masses and mixings while another one describes the lepton masses via an accurate geometric description. Hopefully, these two studies lead to similar conclusions and allow us to speculate on some interesting properties for new flavour physics.

PrOs₄Sb₁₂ is the first known heavy fermion superconductor containing Pr. Many experiments show results indicating unconventional superconductivity in this system. Most notably, PrOs₄Sb₁₂ exhibits two superconducting transitions. The upper transition occurs at Tc₁ ≈ 1.89 K and the lower transition occurs at Tc₂ ≈ 1.72 K. There are many features of this system that are not understood and do not have a unifi ed consensus among researchers. Many issues remain unanswered, such as the origin of superconductivity, symmetry of the superconducting energy gap, and the nature of the two superconducting transitions. We present specific heat data for a single PrOs₄Sb₁₂ crystal. The data show two superconducting transitions. Variance in the lower superconducting transition (among various samples) suggests multiple superconducting phases. Power law dependence of the low temperature specific heat is indicative of asymmetric energy gap. Cuprates are unconventional high temperature superconductors. The theory on origin and characteristics of superconductivity in these systems is still a debated issue. Experiments indicate presence of a phase in these systems that occurs above the superconducting transition temperature which exhibits some common characteristics with the superconducting state. An important issue is the nature of this so-called "pseudogap" phase and its relationship to the superconducting state. We have developed an experimental apparatus and procedure for measuring the specific heat of a high temperature superconductor and demonstrated it by measuring the heat capacity of a YBCO high-Tc superconductor sample.

PrOs₄Sb₁₂ is the first known heavy fermion superconductor containing Pr. Many experiments show results indicating unconventional superconductivity in this system. Most notably, PrOs₄Sb₁₂ exhibits two superconducting transitions. The upper transition occurs at Tc₁ ≈ 1.89 K and the lower transition occurs at Tc₂ ≈ 1.72 K. There are many features of this system that are not understood and do not have a unifi ed consensus among researchers. Many issues remain unanswered, such as the origin of superconductivity, symmetry of the superconducting energy gap, and the nature of the two superconducting transitions. We present specific heat data for a single PrOs₄Sb₁₂ crystal. The data show two superconducting transitions. Variance in the lower superconducting transition (among various samples) suggests multiple superconducting phases. Power law dependence of the low temperature specific heat is indicative of asymmetric energy gap. Cuprates are unconventional high temperature superconductors. The theory on origin and characteristics of superconductivity in these systems is still a debated issue. Experiments indicate presence of a phase in these systems that occurs above the superconducting transition temperature which exhibits some common characteristics with the superconducting state. An important issue is the nature of this so-called "pseudogap" phase and its relationship to the superconducting state. We have developed an experimental apparatus and procedure for measuring the specific heat of a high temperature superconductor and demonstrated it by measuring the heat capacity of a YBCO high-Tc superconductor sample.

Zugl.: Karlsruhe, Univ., Diss., 2005

Thesis (Ph. D.)--Virginia Polytechnic Institute and State University, 1992. / Vita. Abstract. Includes bibliographical references (leaves 115-118). Also available via the Internet.

Thesis--Max-Planck-Institut fur Stromungsforschung, 1997.

DANTAS, Davi Monteiro. Localização de modos fermiônicos em uma geometria de seis dimensões do tipo Conifold. 2012. 83 f. Dissertação (Mestrado em Física) - Programa de Pós-Graduação em Física, Departamento de Física, Centro de Ciências, Universidade Federal do Ceará, Fortaleza, 2012. / Submitted by Edvander Pires (edvanderpires@gmail.com) on 2015-10-21T21:39:04Z No. of bitstreams: 1 2012_dis_dmdantas.pdf: 4713678 bytes, checksum: f91a14fbcd068cfe00c42afc012b1a22 (MD5) / Approved for entry into archive by Edvander Pires(edvanderpires@gmail.com) on 2015-10-22T21:32:16Z (GMT) No. of bitstreams: 1 2012_dis_dmdantas.pdf: 4713678 bytes, checksum: f91a14fbcd068cfe00c42afc012b1a22 (MD5) / Made available in DSpace on 2015-10-22T21:32:16Z (GMT). No. of bitstreams: 1 2012_dis_dmdantas.pdf: 4713678 bytes, checksum: f91a14fbcd068cfe00c42afc012b1a22 (MD5) Previous issue date: 2012 / One way to solve the hierarchy problem and therefore unify the fundamental forces is to assume, under the theoretical point of view, that our four-dimensional space (Brane) is housed in a space of higher dimensionality (Bulk). We call all that extra dimension which is not present in our Brana. The idea of extra dimensions to include unification of fundamental forces date from the 30s of last century, with the innovative proposal of Kaluza and Klein, and has been evolving ever since its formulation. Thus, other innovative proposals like that of the work of Randall and Sundrum have created new possibilities for the study, although it is curious that cite not have any experimental evidence to date that these dimensions exist. Fundamental fermionic particles have as one of its interesting properties the existence of left and right chiral modes, this information widely studied in the Standard Model and Supersymmetry in the call. In this article we treat on the location of the chiral modes, massless and massive, the fermionic fields of spin 1/2 in a six-dimensional space of type Conifold solved. This space has an adjustable parameter which allows to recover the geometry of other works of literature. Beyond this generalization was possible to find other interesting results as the thickening of the Brana and smoothing the model studied in 6D. Looking at work that the ratio of chiral modes is strictly dependent on the choice of coupling fields used. For free fermions chiral modes are identical. Regarding the location of Massive modes, we find that by rewriting the Dirac equation, obtained from our action, in a way kind of Schrödinger equation, we find a term potential. We found that when using the factors derived from the sixth dimension as a term coupling, we obtain results similar to a Yukawa coupling in five dimensions. / Uma das formas de resolver o Problema de Hierarquia e por consequência unificar as forças fundamentais da natureza é assumir, sob o ponto de vista teórico, que nosso espaço quadrimensional (brana) está inserido em um espaço de dimensionalidade maior (bulk). Chamamos de dimensão extra toda aquela que não está presente em nossa brana. A idéia de incluir dimensões extras para unificação de forças fundamentais data dos anos 30 do século passado, com a inovadora proposta de Kaluza e Klein, e vem evoluindo sua formulação desde então. Assim, outras propostas inovadoras como aquela do trabalho de Randall e Sundrum, criaram novas possibilidades para o estudo, embora seja interessante citar que não possuímos nenhuma evidência experimental até o presente momento de que tais dimensões existam. Partículas fundamentais fermiônicas têm como uma de suas propriedades interessantes a existência dos modos quirais direito e esquerdo, informação esta bastante estudada no Modelo Padrão assim como em Supersimetria. Nesse trabalho tratamos sobre a localização dos modos quirais, sem massa e massivo, de campos fermiônicos de spin 1/2 em uma espaço de seis dimensões do tipo Conifold Resolvido. Este espaço possui um parâmetro regulável, o qual permite obter geometrias de outros trabalhos da literatura como casos particulares. Além desta generalização, foi possível encontrar outros resultados interessantes como o espessamento da brana e suavização do modelo estudado em 6D. Observaremos também que a relação dos modos quirais é estritamente dependente da escolha do acoplamento de campos utilizado. Para férmions livres, os modos quirais serão idênticos. Quanto à localização de Modos Massivos, verificaremos que ao reescrever a equação de Dirac, obtida a partir de nossa ação, em uma forma do tipo equação de Schrödinger, encontraremos um termo de potencial. Estudaremos que ao se utilizar os fatores derivados da sexta dimensão como um termo de acoplamento, obteremos resultado semelhante ao de um acoplamento Yukawa em cinco dimensões.

京都大学 / 0048 / 新制・課程博士 / 博士(理学) / 甲第20889号 / 理博第4341号 / 新制||理||1623(附属図書館) / 京都大学大学院理学研究科物理学・宇宙物理学専攻 / (主査)准教授 戸塚 圭介, 教授 川上 則雄, 教授 佐藤 昌利 / 学位規則第4条第1項該当 / Doctor of Science / Kyoto University / DFAM