
Microscopy
Today - September 2010
AFM Measurements of DNA Molecule
Electron Transport Properties
Jim McMahon
Nanotechnology writer for Zebra Communications, P.O. Box 940968,
Simi Valley, CA 93094
jim.mcmahon@zebracom.net
Introduction
Deoxyribonucleic acid (DNA) has been considered as a possibility
for molecular electronics. Because DNA is able to recognize
other molecules-other strands of DNA-and because it binds
together with similar DNA strands in a very unique way, scientists
have suggested the possibility of using DNA as an electronic
circuit without having to build in any other circuitry. The
DNA would bind with other similar DNA strands that it recognizes
and then use the connecting properties of the DNA to create
a self-assembled biological wire for electrical conduction.
Until recently, uncertainty existed about whether DNA could
conduct at all, and if it could, how well it could conduct.
Scientific speculations ranged from DNA being a superconductor
to a complete insulator. Recent research, however, by Dr.
Sidney R. Cohen in collaboration with Dr. Ron Naaman and Dr.
Claude Nogues of the Weizmann Institute of Science, Scanned
Probe Microscopy Unit, in Rehovot, Israel, aided by the enabling
technologies of ultra-high-resolution microscopy and negative-stiffness
vibration isolation, has shed new light on the electrical
transport properties of DNA, focusing on the capacity of single
molecules of DNA to transport current along individual strands.
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DNA Measurement Challenges
DNA is a nucleic acid that contains the genetic instructions
used in the development and functioning of all known
living organisms and some viruses. The main role of
DNA molecules is the long-term storage of information.
DNA nanotechnology uses the unique molecular-recognition
properties of DNA to create self-assembling branched
DNA complexes with useful properties.
To measure the electronic properties of DNA, Dr. Cohen
and his staff needed to connect an electrode to the
end of a DNA molecule, which is only a few nanometers
in length, using an AFM (atomic force microscope) [1,
2], One difficulty in measuring something this small
is ensuring that a good electrical contact is made to
the molecule-the researcher wants to measure the electrical
properties of the molecule, not the quality of the connection.
To facilitate this bio-molecular connection, the lab
attached a bio-link, a gold electrode, to a single strand
of DNA, and then attached a very small gold ball (10
to 20 nanometers in size) to a complementary DNA strand,
after which these two strands were hybridized {linking
of the two single strands, aided by genetic similarity
between corresponding DNA sequences) as shown in Figure
1, If the strands are complementary, their matching
cousin on the other strand will form a double-strand.
Single strands of DNA do not conduct electricity. The
double-strand does conduct for certain configurations.
DNA molecules are very easily destroyed. Hooking up these gold
connectors and balls at the nano level without tearing
them off or burning them out is quite challenging (Figure
2). This preparation method, developed by Dr. Nogues,
is critical and somewhat time-consuming but is a fundamental
aspect of this research model. Using an AFM, with the
DNA double-strand displayed on a flat surface, the researchers
could then locate the gold ball, put the AFM tip on top
of the ball, flow a current through the double-strand,
and view the current voltage characteristics (Figure 3).
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Figure 1: Schematic of the measuring system. DNA
oligomer is attached to a gold electrode below and hybridizes
with a DMA attached to a gold nanoparticle, which then
forms the upper electrode for the double-stranded DNA.
Current is measured by applying a bias between upper
and lower electrodes with placement controlled by the
AFM tip. Modified from a figure in [1].
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Electron Transport Properties of DNA
Dr. Cohen explains, "There are two possibilities when
we talk about electrons flowing through a DNA molecule. We
can break it down into two different kinds of electron transport.
One is called a 'tunneling process,' where the electron effectively
shoots through the molecule without caring too much about
the internal structure of the molecule. The other is called
a 'hopping process,' where the electron actually resides for
small periods of time in certain positions along the molecule.
In this case the electron will be affected by temperature.
DNA consists of a sequence of base pairs. We found that variations
in both the sequence and the composition of a strand's base
pairs can also affect the progress of electron transport through
the strand. Similarly, bases which are electron-rich have
better electron conductivity than those which have fewer available
electrons [Figure 3]. This is not solely academic; electronic
behavior of DNA is very closely related to function. There
are electrochemical processes, which are mediated by these
DNA biological molecules. For instance, radiation damage,
and mutation-how does the DNA deal with an extra electron
or an absence of an electron located somewhere along its chain?"
[3]
The characteristics of electron conductivity in DNA also
have implications in molecular electronics, which is trying
to achieve devices that, instead of working on the standard
silicon circuitry, function through innocuous molecules. Because
of DNA's facility to bind with similar types of DNA molecules,
it is not necessary to physically place each molecule in a
set location. DNA put into solution can be expected to organize
itself in the right way and become a predictable medium for
electrons.
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Figure 2: AFM image of gold nanoparticles bound from
below to the double-stranded DNA[1].
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Figure 3: Current versus voltage curves for DNA strands
with different concentrations of the guanine-cytosine
(GC} base pair, which releases electrons more readily
than the thymine-adenine (AT) base pairs. Higher numbers
of GC pairs are increasingly electron rich.
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Vibration Isolation Critical to DNA Research
The Weizmann Institute is one of the few research groups in
the world that has actually managed to measure the electrical
transport properties of a single molecule of DNA. One of the
challenges that presents itself in nanoscale research is vibration
isolation. Every laboratory measuring and imaging at the nano-level
is dealing with problems of site vibration, which compromises
to a greater or lesser degree the imaging quality and data
sets that are acquired through ultra-high-resolution microscopy.
A critical factor in the Weizmann Institute's ability to consistently
measure DNA electron structures at such extreme nano-level
resolutions is the lab's use of negative-stiffness vibration
isolation systems (Minus K Technology) which produced the
ultra-stable environment that the AFMs needed to execute this
research [4, 5]
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"Any lab site is subject to vibrations from machines,
vibrations of the building itself, and even from people
walking around, in the range from less than 10 hertz
to about 30 hertz," says Cohen. "The lab has
three separate AFM systems, each with several different
modules that require very precise vibration isolation
for all of our research, including our DNA electron
transport studies. We have opted for negative-stiffness
vibration isolation to provide the necessary low-noise
environment." [3]
Negative-stiffness mechanism (NSM) isolators have the
flexibility of custom tailoring resonant frequencies
vertically and horizontally. They employ a completely
mechanical concept in low-frequency vibration isolation.
Vertical-motion isolation is provided by a stiff spring
that supports a weight load, combined with an NSM. The
net vertical stiffness is made very low without affecting
the static load-supporting capability of the spring.
Beam-columns connected in series with the vertical-motion
isolator provide horizontal-motion isolation. The horizontal
stiffness of the beam-columns is reduced by the "beam-column"
effect. A beam-column behaves as a spring combined with
an NSM. The result is a compact passive isolator capable
of very low vertical and horizontal natural frequencies
and very high internal structural frequencies (Figure
4).
"We tried air tables, but they did not do very
well for us with the horizontal vibrations," continues
Cohen. "Then we compared active systems to the
negative-stiffness isolator, measuring the frequency
spectrum up to about 100 hertz, and the active systems
did not perform as well as the negative-stiffness isolator."
[3]
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Figure 1: Schematic of a negative-stiffness vibration
isolator.
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Negative-stiffness mechanism (NSM) isolators have the flexibility
of custom tailoring resonant frequencies vertically and horizontally.
They employ a completely mechanical concept in low-frequency
vibration isolation. Vertical-motion isolation is provided
by a stiff spring that supports a weight load, combined with
an NSM. The net vertical stiffness is made very low without
affecting the static load-supporting capability of the spring.
Beam-columns connected in series with the vertical-motion
isolator provide horizontal-motion isolation. The horizontal
stiffness of the beam-columns is reduced by the "beam-column"
effect. A beam-column behaves as a spring combined with an
NSM. The result is a compact passive isolator capable of very
low vertical and horizontal natural frequencies and very high
internal structural frequencies (Figure 4).
"We tried air tables, but they did not do very well
for us with the horizontal vibrations," continues Cohen.
"Then we compared active systems to the negative-stiffness
isolator, measuring the frequency spectrum up to about 100
hertz, and the active systems did not perform as well as the
negative-stiffness isolator." [3]
Transmissibility with negative-stiffness is substantially
improved over air systems, which can make vibration isolation
problems worse since they have a resonant frequency that can
match that of floor vibrations. Transmissibility is a measure
of the vibrations that transmit through the isolator relative
to the input vibrations. The NSM isolators, when adjusted
to 0.5 Hz, achieve 93 percent isolation efficiency at 2 Hz,
99 percent at 5 Hz, and 99.7 percent at 10 Hz. NSM transmissibility
is also improved over active systems.
Conclusion
The measurement of electron transport through DNA molecules
by AFM is one more step toward DNA-related electronic devices.
Negative-stiffness vibration isolation was an essential component
of the AFM system.
References
[1] C Nogues et al, Phys Chem Chem Phys 6 (2004) 4459-66.
[2] SR Cohen and A Hitler, Curr Opin Colloid In 13 (2008)
316-25. [3] SR Cohen, interviewed by lim McMahon, tape recording,
May 16, 2007.
[4] DK Ferry, Laser Focus World 43(10) (2007) 107-10. [5]
DL Flatus, Proc SP1E 3786 (2009) 98-105.

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