APS March Meeting 2013
Volume 58, Number 1
Monday–Friday, March 18–22, 2013;
Baltimore, Maryland
Session Y3: Invited Session: New Directions in Fractional Quantum Hall Phenomena
8:00 AM–11:00 AM,
Friday, March 22, 2013
Room: Ballroom III
Sponsoring
Units:
DCMP DCOMP
Chair: Mansour Shayegan, Princeton University
Abstract ID: BAPS.2013.MAR.Y3.5
Abstract: Y3.00005 : Fractional quantum Hall effect in AlAs quantum wells: Role of valley degree of freedom
10:24 AM–11:00 AM
Preview Abstract
Abstract
Author:
Tayfun Gokmen
(IBM T.J. Watson Research Center)
When interacting two-dimensional electrons are placed in a large
perpendicular magnetic field, to minimize their energy, they capture an even
number of flux quanta and create new particles called composite fermions
(CFs). These complex electron-flux-bound states offer an elegant explanation
for the fractional quantum Hall effect. Thanks to the flux attachment, the
effective field vanishes at half-filled Landau levels ($\nu =$ 1/2 and
3/2) and CFs exhibit Fermi-liquid-like properties, similar to their
zero-field electron counterparts. Here, we study a two-dimensional electron
system in AlAs quantum wells where the electrons occupy two conduction band
valleys with anisotropic Fermi contours and strain-tunable occupation. We
address a fundamental question whether the anisotropy of the electron
effective mass and Fermi surface is transferred to the CFs formed around
filling factors $\nu =$ 1/2 and 3/2. Similar to their electron counter
parts, CFs also exhibit anisotropic transport, suggesting an anisotropy of
CF effective mass and Fermi surface. We also study quantum Hall
ferromagnetism for fractional quantum Hall states formed at $\nu =$ 1/3
and 5/3 as a function of valley splitting. Within the framework of the CF
theory, electronic fractional filling factors $\nu =$ 1/3 and 5/3 are
equivalent to the integer filling factor $p=$ 1 of CFs. Reminiscent of the
quantum Hall ferromagnetism observed at $\nu =$ 1, we report persistent
fractional quantum Hall states at filling factors $\nu =$ 1/3 and 5/3 when
the two valleys are degenerate. However, the comparison of the energy gaps
measured at $\nu =$ 1/3 and 5/3 to the available theory developed for
single-valley, two-spin systems reveals that the gaps and their rates of
rise with strain are much smaller than predicted.\\[4pt]
[1] ``Transference of Transport Anisotropy to Composite Fermions,'' T. Gokmen, M. Padmanabhan, and M. Shayegan, \textit{Nature Physics }\textbf{6}, 621-624 (2010).\\[4pt]
[2] `Ferromagnetic Fractional Quantum Hall States in a Valley-Degenerate Two-Dimensional Electron System,'' M. Padmanabhan, T. Gokmen, and M. Shayegan, \textit{Phys. Rev. Lett.} \textbf{104}, 016805 (2010).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2013.MAR.Y3.5