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