2008 APS March Meeting
Volume 53, Number 2
Monday–Friday, March 10–14, 2008;
New Orleans, Louisiana
Session Y3: Novel Physics and Quantum Interference in Weakly Disordered Graphene Devices
11:15 AM–2:15 PM,
Friday, March 14, 2008
Morial Convention Center
Room: RO2 - RO3
Sponsoring
Unit:
DCMP
Chair: Alberto Morpurgo, Technical Univerisity of Delft
Abstract ID: BAPS.2008.MAR.Y3.3
Abstract: Y3.00003 : Quantum Interference in Single and Bilayer Graphene
12:27 PM–1:03 PM
Preview Abstract
Abstract
Author:
Alexander Savchenko
(School of Physics, University of Exeter, Exeter EX4 4QL, Uk)
It is known that interference of charge carriers scattered by
impurities
results in a quantum correction to the conductivity of a
two-dimensional
(2D) system. This phenomenon of weak localisation (WL) is usually
seen as
magnetoconductivity, as magnetic field changes the phase of
interfering
waves. Here we show that quantum interference in graphene -- a
single layer
of carbon atoms [1] -- is very different from that in
conventional 2D
systems. Due to the \textit{chiral} nature of carriers, it
becomes sensitive to different
\textit{elastic} scattering mechanisms. By changing the geometry
and quality of samples we
show that quantum interference in graphene can take a variety of
forms, and
that WL is a sensitive tool to detect defects in graphene
crystals [2].
We perform a comparative study of WL in single-layers and
bilayers. Although
the two systems are different in their spectrum (massless and
massive
fermions, respectively), the carriers in both are chiral. As a
result WL in
a bilayer is also affected by elastic scattering [3].
Analysis of the magnetoresistance using theories [4] allows us to
determine
the phase-breaking time as well as times of inter- and intra-valley
scattering, which together control WL. They are found at
different carrier
densities, including the electro-neutrality point where the
nominal carrier
density is zero. We show that in all cases WL is not suppressed,
and that
the reason for this is strong inter-valley scattering. The study
of WL is
complemented by AFM imaging of the surface which provides
information about
the nature of the defects responsible for the different
manifestations of WL
in graphene systems.
In addition to the studies of WL, we perform analysis of universal
conductance fluctuations (UCF) in both systems. They have the
same physical
origin as WL -- quantum interference -- and are controlled by the
same
characteristic times. We compare the times found from analysis of
WL and
UCF.
\newline
[1] K.S. Novoselov \textit{et al}., Science \textbf{306}, 666 (2004)
\newline
[2] F.V.Tikhonenko \textit{et al.}, arXiv: 0708.1700 (to be
published in Phys. Rev. Lett.)
\newline
[3] R.V. Gorbachev \textit{et al.}, Phys. Rev. Lett. \textbf{98},
176805 (2007).
\newline
[4] E. McCann et al., Phys. Rev. Lett. \textbf{97}, 146805
(2006); K. Kechedzhi \textit{et al}., Phys. Rev. Lett.
\textbf{98}, 176806 (2007).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2008.MAR.Y3.3