Show simple item record

dc.contributor.advisorSenthil Todadri.en_US
dc.contributor.authorNikoliÄ , Predrag, 1974-en_US
dc.contributor.otherMassachusetts Institute of Technology. Dept. of Physics.en_US
dc.date.accessioned2005-09-27T17:30:52Z
dc.date.available2005-09-27T17:30:52Z
dc.date.copyright2004en_US
dc.date.issued2004en_US
dc.identifier.urihttp://hdl.handle.net/1721.1/28650
dc.descriptionThesis (Ph. D.)--Massachusetts Institute of Technology, Dept. of Physics, 2004.en_US
dc.descriptionIncludes bibliographical references (p. 215-219).en_US
dc.description.abstract(cont.) more general lessons on frustrated quantum magnetism. At the end, we demonstrate some new mathematical tools on two other frustrated two-dimensional systems, and summarize our conclusions, with an outlook to remaining open problems.en_US
dc.description.abstractIn this thesis we attempt to reach a physical understanding and theoretical description of some of the greatest challenges in the field of frustrated quantum magnetism, mainly the Kagome lattice antiferromagnets. After an introductory review of concepts, we closely examine the Kagome lattice quantum Heisenberg and Ising models. We apply several new techniques based on lattice gauge theories, duality mappings and field theory in order to explore phase diagrams of these models. Our approach provides a microscopic picture of the mysterious phenomena observed numerically and experimentally in the Kagome Heisenberg antiferromagnets. Namely, we argue that the spinless excitations, thought to be gapless in absence of any symmetry breaking in this system, are in fact gapped, but at an extremely small emergent energy scale. This scenario is realized in an unconventional valence-bond ordered phase, with a very large unit-cell and complex structure. We also discuss properties of a spin liquid that could be realized in the Kagome antiferromagnet, and argue that its elementary excitations are clearly gapped and extremely massive or even localized. We demonstrate that the Kagome lattice quantum Ising models are an excellent platform for learning about effects of quantum fluctuations on classically degenerate ground-states. We consider several ways in which spins can acquire quantum dynamics, including transverse field, XXZ exchange and ring-exchange perturbations. Using two different setups of compact U(1) gauge theory we find circumstances in which many characteristic quantum phases occur: disordered phase, topologically ordered spin liquid, valence-bond crystal, and a phase with coexistence of magnetic and valence-bond order. From this variety of results we attempten_US
dc.description.statementofresponsibilityby Predrag Nikolić.en_US
dc.format.extent219 p.en_US
dc.format.extent12568812 bytes
dc.format.extent12597086 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypeapplication/pdf
dc.language.isoen_US
dc.publisherMassachusetts Institute of Technologyen_US
dc.rightsM.I.T. theses are protected by copyright. They may be viewed from this source for any purpose, but reproduction or distribution in any format is prohibited without written permission. See provided URL for inquiries about permission.en_US
dc.rights.urihttp://dspace.mit.edu/handle/1721.1/7582
dc.subjectPhysics.en_US
dc.titleGeometrically frustrated quantum magnetsen_US
dc.typeThesisen_US
dc.description.degreePh.D.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Physics
dc.identifier.oclc58965632en_US


Files in this item

Thumbnail

This item appears in the following Collection(s)

Show simple item record