2008 APS March Meeting
Volume 53, Number 2
Monday–Friday, March 10–14, 2008;
New Orleans, Louisiana
Session Q1: Ballistic Charge and Spin Transport in Graphene
11:15 AM–1:39 PM,
Wednesday, March 12, 2008
Morial Convention Center
Room: LaLouisiane AB
Sponsoring
Unit:
DCMP
Chair: Shan-Wen Tsai, University of California, Riverside
Abstract ID: BAPS.2008.MAR.Q1.1
Abstract: Q1.00001 : Electronic spin transport and spin precession in single graphene layers at room temperature.
11:15 AM–11:51 AM
Preview Abstract
Abstract
Author:
Bart Van Wees
(University of Groningen)
I will give a review of our experiments on spin injection, spin
transport
and spin precession in field effect transistors based on single
graphene
layers. We have employed a four terminal non-local measurement
technique
which allows us to fully separate the electronic charge and spin
circuits.
One pair of ferromagnetic electrodes is used as spin injectors,
the other
pair as spin detectors. By using different widths for the
ferromagnetic
electrodes we are able to control the coercive fields and prepare
the
magnetization direction of each with an applied magnetic field
(in positive
or negative x-direction). We observe clear signals due to spin
diffusion
from injector to detector electrodes. From the dependence of the
spin
signals on electrode spacing we obtain a spin relaxation length
of 1.5 to 2
micrometer, and a corresponding spin relaxation time of about 100
ps [1].
These measurements are confirmed by Hanle-type spin precession
measurements
where the injected spins precess around a magnetic field applied
perpendicular to the graphene plane. The spin signals only weakly
depend on
temperature (between 4.2 K and 300K), and also change little when
the gate
voltage is tuned from the metallic electron/hole regimes to the
Dirac
neutrality point. Recent experiments show that the spin relaxation
times/lengths are similar for spin directions pointing in the
graphene plane
and perpendicular to the graphene plane [2]. Also the presence of
an Al$_2$O$_3$
layer on top of the graphene does not significantly change the spin
relaxation length and time. I will discuss these results in the
light of
existing theories for spin-orbit interaction in graphene. The
implications
for graphene spintronics and graphene qubits will be discussed.
\newline
\newline
[1] N. Tombros, C. Jozsa, M. Popinciuc, H.T. Jonkman, and B.J.
van Wees,
Nature 448, 571 (2007)
\newline
[2] N. Tombros et al.,submitted to Phys. Rev. lett.
\newline
[3] M. Popinciuc et al., submitted to Phys. Rev. B.
\newline
[4] C. Jozs et al., submitted to Phys. Rev. Lett.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2008.MAR.Q1.1