Interactions and topology in two-dimensional semiconductor and semimetal

dc.contributor.advisorMacDonald, Allan H.
dc.contributor.committeeMemberChelikowsky, James R
dc.contributor.committeeMemberFiete, Gregory A
dc.contributor.committeeMemberRegister, Lenoard F
dc.creatorXue, Fei, 1990-
dc.date.accessioned2018-10-01T20:08:32Z
dc.date.available2018-10-01T20:08:32Z
dc.date.created2018-08
dc.date.issued2018-09-14
dc.date.submittedAugust 2018
dc.date.updated2018-10-01T20:08:33Z
dc.description.abstractThis dissertation presents our study of interaction and topology effects in two-dimensional semiconductor and semimetal. In the first part, we explore the ground state thermodynamic phases in various systems using a mean-field theory including long-range Coulomb interaction. In particular, we have discovered two distinct phases with different number of exciton condensate flavors in a bilayer system of two-dimensional semiconductors with spin/valley degree of freedoms. The exciton condensate phase is characterized by spontaneous inter-layer phase coherence and counterflow superfluidity. We have also studied the phase diagram of a model quantum spin Hall system as a function of band inversion and band-coupling strength, demonstrating that when band hybridization is weak, an interaction-induced nematic insulator state emerges over a wide range of band inversion. We also develop a fully microscopic theory of equilibrium polariton condensates that treats the two-dimensional quantum well band states explicitly and goes beyond the commonly used model in which bare excitons are treated as Bose particles that are coupled via flip-flop interactions with cavity photons. In the second part, we present our study of collective excitations in an exciton condensate using a time-dependent mean-field theory. By constructing a fluctuation Lagrangian based on a variational wave-function capturing exciton density and phase fluctuations, we are able to get the collective mode spectra and demonstrate the stability of exciton condensate phase. Moreover, we apply a linear response theory to identify a number of collective modes with a strong electron-hole pairing amplitude(Higgs-like) component. Next, we generalize our time-dependent mean-field theory to finite temperature to address the long debate question that whether a CDW phase of a semimetal is due to Coulomb interaction or electron-phonon interaction. Our theory includes both intraband and interband excitations and direct and exchange interactions, and allows for the formation of exciton condensates at low temperatures.
dc.description.departmentPhysics
dc.format.mimetypeapplication/pdf
dc.identifierdoi:10.15781/T2SB3XH72
dc.identifier.urihttp://hdl.handle.net/2152/68623
dc.language.isoen
dc.subjectExciton
dc.subjectExciton condensate
dc.subjectQuantum spin Hall insulator
dc.subjectNematic insulator
dc.subjectCharge density wave
dc.subjectCollective excitation
dc.subjectPolariton
dc.subjectHiggs mode
dc.titleInteractions and topology in two-dimensional semiconductor and semimetal
dc.typeThesis
dc.type.materialtext
thesis.degree.departmentPhysics
thesis.degree.disciplinePhysics
thesis.degree.grantorThe University of Texas at Austin
thesis.degree.levelDoctoral
thesis.degree.nameDoctor of Philosophy

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