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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 halffilledLandau 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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