Condensed Matter Seminar Series
Composite Fermions and Broken Symmetries in Graphene
Francois Amet
Stanford University
Thursday April 24, 11:30 am, Room 298, Physics Building
Abstract: The
electronic properties of graphene are well described by a
non-interacting Dirac Hamiltonian with a fourfold symmetry associated
with spin and valley, an additional degree of freedom due to the
hexagonal crystal lattice of graphene. As a result, graphene exhibits a
variety of peculiar phenomena such as an anomalous quantum Hall effect.
At high magnetic fields, the electron kinetic energy is quenched by the
Landau quantization, and Coulomb interactions become the dominant
energy scale of the system. This results in a variety of new electronic
phases, whose ground states depend on the competition between symmetry
breaking interactions.
Observing these so-called fractional
quantum Hall (FQH) phases is challenging in graphene because potential
fluctuations induced by disorder blur out transport signatures of FQH
states. I will describe fabrication techniques to overcome these
difficulties and obtain devices with carrier mobility exceeding one
million cm2/Vs in FET or bipolar geometries. This quality allows for
the observation of a plethora of fractional quantum Hall phases at
filling factors following the composite fermion theory. The sequence of
fractions, as well as the magnetic field dependence of their activation
gaps, informs us about the spin and valley polarization of the ground
state in each phase.
Host: Gleb Finkelstein