Manipulating Nanoparticles in Solution with Electrically
Contacted Nanotubes Using Dielectrophoresis
Lifeng Zheng,
†
Shengdong Li,
†
James P. Brody,
†,‡
and Peter J. Burke*
,†,‡
Department of Electrical Engineering and Computer Science and Biomedical Engineering,
University of California, Irvine, California 92697
Received February 4, 2004. In Final Form: July 13, 2004
Dielectrophoresis is an electronic analogue
1,2
of optical tweezers
3
based on the same physical principle:
an ac electric field induces a dipole moment on an object in solution, which then experiences a force
proportional to the gradient of the field intensity. For both types of tweezers, this force must compete with
thermal Brownian
4
motion to be effective, which becomes increasingly difficult as the particle size approaches
the nanometer scale. Here we show that this restriction can be overcome by using the large electric field
gradient in the vicinity of a carbon nanotube to electronically manipulate nanoparticles down to 2 nm in
diameter.
I. Introduction
The physical principles of self-assembly that give rise
to complicated three-dimensional structures on the na-
nometer scale in both biological and synthetic systems
have been studied extensively.
5,6
The forces at work include
noncovalent inter- and intramolecular interactions, i.e.,
hydrogen bonding, van der Waals, metal-ligand interac-
tions, π-π stacking, and hydrophobic vs hydrophilic
interactions. These bottom-up principles of self-assembly,
while efficient and economical, generally are passive; i.e.,
they are controlled only by macroscopic quantities such
as temperature, pH, and solvent concentration. It would
be a distinct advantage if this assembly process could be
actively, electronically controlled, especially with nano-
meter spatial resolution. In this regard, top-down ap-
proaches to the manipulation of matter have been suc-
cessful at the nanometer scale only with atomic force
microscopy (AFM)/scanned probed technologies, which are
difficult to scale to a massively parallel environment, such
as that envisioned in the nascent field of molecular
electronics.
In a separate, related research theme, the use of electric
fields generated by an external voltage source to actively
manipulate the locations of nanometer scale objects and
large molecules such as DNA and proteins is well-known
from conventional, established techniques such as gel
electrophoresis. Here, the electrodes used are typically
macroscopic in size, i.e., many centimeters. A recent
variant on this research theme is the integration of
microelectronic fabrication techniques such as photo-
lithography to fabricate electrodes with dimensions on
the order of millimeters or hundreds of micrometers.
7,8
In
these electrophoresis techniques, charged species respond
via the Coulomb force to dc electric fields. As a result, a
limitation of the technique is that neutral species are
unaffected and hence cannot be manipulated.
One available technique to electronically manipulate
the position of both neutral and charged species in solution
is to use ac electric fields, a technique called dielectro-
phoresis.
1
The physical principles of dielectrophoresis are
well-established. If a polarizable object is placed in an
electric field, there will be an induced positive charge on
one side of the object and an induced negative charge (of
the same magnitude as the induced positive charge) on
the other side of the object. The positive charge will
experience a pulling force; the negative charge will
experience a pushing force. However, in a nonuniform
field, the electric field will be stronger on one side of the
object and weaker on the other side of the object. Hence,
the pulling and pushing forces will not cancel, and there
will be a net force on the object. This is the dielectrophoresis
(DEP) force.
The key physical insight in this paper is that we use
carbon nanotubes as the electrode to generate the electric
field gradient; the nanotubes are electrically contacted by
lithographically defined metal electrodes, which are far
away from the region of interest, so that the fields from
the metal electrodes are numerically insignificant com-
pared to the fields generated by the nanotube itself. Since
the electric field gradient in the vicinity of a nanotube is
large, nanoparticles as small as 2 nm in diameter can be
manipulated despite the large tendency for random,
thermal Brownian motion important for such small
particles. This is an order of magnitude smaller than
previous nanoparticles that were manipulated with
lithographically defined electrodes, and represents the
first use of nanotube electrodes in dielectrophoresis.
Because this allows an electronic link to the nanometer
world, this technology may find applications as a com-
ponent of massively parallel, actively controlled na-
nomanufacturing platforms and, generally speaking, may
provide a bridge between top-down and bottom-up
approaches to nanotechnology.
* To whom correspondence may be addressed. E-mail:
pburke@uci.edu.
†
Department of Electrical Engineering and Computer Science.
‡
Biomedical Engineering.
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8612 Langmuir 2004, 20, 8612-8619
10.1021/la049687h CCC: $27.50 © 2004 American Chemical Society
Published on Web 08/24/2004