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Title page for ETD etd-03172008-150046


Type of Document Dissertation
Author Doan, Quoc
Author's Email Address qmd2934@fsu.edu
URN etd-03172008-150046
Title Variational Study of the Nematic State of the Two Dimensional Electron Gas in a Magnetic Field
Degree Doctor of Philosophy
Department Physics, Department of
Advisory Committee
Advisor Name Title
Efstratios Manousakis Committee Member
Jorge Piekarewicz Committee Member
Kun Yang Committee Member
Michael Mascagni Committee Member
Peng Xiong Committee Member
Keywords
  • Nematic
  • Quantum Hall Effect
  • Monte Carlo
Date of Defense 2008-02-19
Availability unrestricted
Abstract
We have studied the nematic state of the two dimensional electron gas (2DEG) at halffilled

Landau level (LL). Our motivation comes from experiments in which anisotropic

transport in the 2DEG under high magnetic field and at low temperature was observed.

Based on a model of the nematic state proposed by Oganesyan, Fradkin and Kivelson,

we investigate this state and compare it with other competing states proposed by other

groups. First, we investigate at what LL the nematic state becomes energetically favorable

as compared to the isotropic state. Our studies indicate that this occurs at the second

excited LL. Moreover, we compare the energy of the nematic state with that of the stripe

state obtained within the Hartree-Fock approximation (HF) and we conclude that, for the

samples studied experimentally, the nematic state might be more stable. In our study we

have used two different methods which both have advantages and disadvantages. The first

method used is the Fermi-hyper-netted chain (FHNC) which provides results valid in the

thermodynamic limit (infinite size system), however, it is accurate only for a low density

system. The second method used is the Monte Carlo method (MC) which can be used on

a finite-size system and, thus, the issue arises of how to extrapolate in the thermodynamic

limit (finite-size effect). The results obtained from both methods are in good agreement

and indicate that the nematic state might be a viable candidate to explain the experimental

findings. In order to compare our results for the nematic state to those obtained for the

stripe state, we needed to include the kinetic energy contribution beyond the familiar hw_c/2

term in the case of the nematic state which comes from the deformed geometry of the Fermi

sea. For the stripe state we have carried out a HF calculation for a more realistic potential

for a 2DEG which includes the effects of the finite confinement of the electron wave function

along the z-direction.

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