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Physicists
Show Electrons Can Travel More Than 100 Times Faster in Graphene
Monday, March 24, 2008
Michael
S. Fuhrer
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Credit:
University of Maryland
University of Maryland
physicists have shown that in graphene the intrinsic limit to the
mobility, a measure of how well a material conducts electricity,
is higher than any other known material at room temperature.
Graphene, a single-atom-thick sheet of graphite, is a new
material which combines aspects of semiconductors and metals.
Their results, published online
in the journal Nature
Nanotechnology,
indicate that graphene holds great promise for replacing
conventional semiconductor materials such as silicon in
applications ranging from high-speed computer chips to
biochemical sensors.
A team of researchers led by
physics professor Michael S. Fuhrer of the university's Center
for Nanophysics and Advanced Materials, and the Maryland
NanoCenter said the findings are the first measurement of the
effect of thermal vibrations on the conduction of electrons in
graphene, and show that thermal vibrations have an
extraordinarily small effect on the electrons in graphene.
In any material, the energy
associated with the temperature of the material causes the atoms
of the material to vibrate in place. As electrons travel through
the material, they can bounce off these vibrating atoms, giving
rise to electrical resistance. This electrical resistance is
'intrinsic' to the material: it cannot be eliminated unless the
material is cooled to absolute zero temperature, and hence sets
the upper limit to how well a material can conduct electricity.
In graphene, the vibrating
atoms at room temperature produce a resistivity of about 1.0
microOhm-cm (resistivity is a specific measure of resistance; the
resistance of a piece material is its resistivity times its
length and divided by its cross-sectional area). This is about 35
percent less than the resistivity of copper, the lowest
resistivity material known at room temperature.
"Other extrinsic sources
in today's fairly dirty graphene samples add some extra
resistivity to graphene," explained Fuhrer, "so the
overall resistivity isn't quite as low as copper's at room
temperature - yet. However, graphene has far fewer electrons than
copper, so in graphene the electrical current is carried by only
a few electrons moving much faster than the electrons in copper."
In semiconductors, a different
measure, mobility, is used to quantify how fast electrons move.
The limit to mobility of electrons in graphene is set by thermal
vibration of the atoms and is about 200,000 cm2/Vs at room
temperature, compared to about 1,400 cm2/Vs in silicon, and
77,000 cm2/Vs in indium antimonide, the highest mobility
conventional semiconductor known.
"Interestingly, in
semiconducting carbon nanotubes, which may be thought of as
graphene rolled into a cylinder, we've shown that the mobility at
room temperature is over 100,000 cm2/Vs," said Fuhrer.
Mobility Mobility
determines the speed at which an electronic device (for instance,
a field-effect transistor, which forms the basis of modern
computer chips) can turn on and off. The very high mobility makes
graphene promising for applications in which transistors much
switch extremely fast, such as in processing extremely high
frequency signals.
Mobility can also be expressed
as the conductivity of a material per electronic charge carrier,
and so high mobility is also advantageous for chemical or
bio-chemical sensing applications in which a charge signal from,
for instance, a molecule adsorbed on the device, is translated
into an electrical signal by changing the conductivity of the
device.
Graphene is therefore a very
promising material for chemical and bio-chemical sensing
applications. The low resistivity and extremely thin nature of
graphene also promises applications in thin, mechanically tough,
electrically conducting, transparent films. Such films are sorely
needed in a variety of electronics applications from touch
screens to photovoltaic cells.
Fuhrer and co-workers showed
that although the room temperature limit of mobility in graphene
is as high as 200,000 cm2/Vs, in present-day samples the actual
mobility is lower, around 10,000 cm2/Vs, leaving significant room
for improvement. Because graphene is only one atom thick, current
samples must sit on a substrate, in this case silicon dioxide.
Trapped electrical charges in the silicon dioxide (a sort of
atomic-scale dirt) can affect the electrons in graphene and
reduce the mobility.
Also, vibrations of the silicon
dioxide atoms themselves can also have an effect on the graphene
which is stronger than the effect of graphene's own atomic
vibrations. This so-called 'remote interfacial phonon scattering'
effect is only a small correction to the mobility in a silicon
transistor, but because the phonons in graphene itself are so
ineffective at scattering electrons, this effect becomes very
important in graphene.
"We believe that this work
points out the importance of these extrinsic effects, and creates
a roadmap for finding better substrates for future graphene
devices in order to reduce the effects of charged impurity
scattering and remote interfacial phonon scattering." Fuhrer
said.
Source:
University of Maryland

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