How Scanning Tunneling Microscopy Reveals Biology's Hidden Landscapes
In the hidden world of the ultra-small, a revolutionary tool allows us to touch the very atoms that compose life's building blocks.
Imagine possessing a microscope so powerful that it could reveal the intricate twists of a DNA strand, not as an artist's interpretation, but as a direct image where individual atoms are discernible. This is not science fiction; it is the reality made possible by the Scanning Tunneling Microscope (STM).
Since its invention in the 1980s, a breakthrough that earned Gerd Binnig and Heinrich Rohrer the Nobel Prize in Physics, STM has allowed scientists to explore the universe at the atomic level 8 . While initially designed for physics, this tool's potential for biology was immediately recognized. It promised a dream: to see biological molecules like proteins, DNA, and lipids in their native state, at a resolution so fine it could distinguish the very atoms that form their structures 1 3 .
This article delves into the journey of STM from studying inert metals to illuminating the dynamic, fragile surfaces of biology, revealing the hidden architecture of life itself.
The magic of STM lies in a quantum mechanical phenomenon called the "tunneling effect." Imagine bringing a super-sharp metallic tip so close to a conductive surface that the electrons, behaving as waves, don't see the gap as a barrier but as a short tunnel they can simply traverse. This creates a tiny tunneling current 8 .
The key is the distance. The tunneling current is exquisitely sensitive, changing by an order of magnitude for every single Ångström (0.1 nanometers) the tip moves toward or away from the surface 8 . By scanning this tip across a surface and meticulously tracking how the current changes, a computer can map out the topography of the surface, atom by atom.
Schematic representation of electron tunneling between tip and sample
STM operates in two primary modes to achieve this:
A feedback system continuously adjusts the tip's height to keep the tunneling current unchanged. The movement of the tip up and down then traces the surface's contours. This mode is safer for rough surfaces and is the most common method for biological samples, preventing the tip from crashing into delicate molecular structures 3 8 .
Applying STM to biology is not straightforward. Biological molecules are the antithesis of ideal STM samples: they are poor electrical conductors, soft and flexible, and often float in an aqueous environment. Early researchers asked a critical question: How can these non-conductive, "squishy" structures be imaged with a tool that requires electrical current and a solid surface? 1 3 The answers emerged through brilliant experimental workarounds.
Biomolecules are deposited on ultra-flat, conductive surfaces like highly oriented pyrolytic graphite (HOPG) or gold 3 .
Inspired by electron microscopy, some methods involve lightly coating the biological sample with a fine layer of metal, making it conductive enough for tunneling 1 .
A fascinating discovery was that STM could image insulating materials in humid air. A thin monolayer of water adsorbed onto the sample can act as a conductive pathway 3 .
To understand how STM biology works in practice, let's examine a pivotal area of research: the imaging of DNA.
A solution containing linearized plasmid DNA is prepared. A small droplet of this solution is placed on a freshly cleaved, atomically flat HOPG surface 3 .
The sample is allowed to dry in a controlled manner, causing the DNA molecules to adsorb onto the graphite surface, held in place by weak molecular forces.
The loaded substrate is transferred to the STM. Using a tungsten tip sharpened to a radius of curvature of less than 50 nm 9 , the scanner begins its painstaking journey back and forth across the surface.
The experiment is often conducted in a humid atmosphere or even a liquid cell to help preserve the biomolecule's structure and enhance conductivity via the water layer 3 . The tunneling parameters, such as bias voltage and set-point current, are carefully optimized to be low enough to avoid damaging the delicate DNA strands.
STM allows visualization of DNA's double helix structure at unprecedented resolution.
Successful experiments have allowed researchers to directly visualize the long, thread-like structure of DNA molecules adsorbed onto graphite. In some studies, researchers have gone a step further, introducing small molecules like ethidium bromide (a fluorescent dye that binds to DNA) and using STM to observe the resulting changes in the DNA's appearance 3 . These images provide direct visual evidence of the drug's binding location and its effect on the DNA's local structure.
The scientific importance of this is profound. It moves beyond theoretical models and offers a direct, real-space observation of genetic material and its interactions with other molecules. This has applications in nanobiotechnology, biosensing, and the development of new therapeutic agents, providing a window into the molecular interactions that are the foundation of life and disease 3 .
Technique | Resolution | Sample Requirements | Key Advantage for Biology |
---|---|---|---|
Scanning Tunneling Microscopy (STM) | Atomic (for conductive surfaces) | Conductive or thin layer on conductive substrate | Can image in liquid/native states; visualizes individual molecules 3 |
Atomic Force Microscopy (AFM) | Nanometer | Any solid surface (conductive or not) | Can measure mechanical properties (elasticity, adhesion) in fluid 3 |
X-ray Crystallography | Atomic | Large, high-quality crystals | Gold standard for 3D atomic structure of proteins in crystals 3 |
Transmission Electron Microscopy (TEM) | Near-atomic | Thin, stained, or frozen samples | Very high resolution for a wide range of biological samples 3 |
Nuclear Magnetic Resonance (NMR) | Atomic (for small proteins) | High concentration in solution | Studies protein dynamics and structure in solution 3 |
Reagent / Material | Function in Biological STM |
---|---|
HOPG (Highly Oriented Pyrolytic Graphite) | An atomically flat, conductive substrate for adsorbing biomolecules 3 . |
STM Buffer | A sterile, pH-stabilized solution to maintain biological samples in native state 2 7 . |
Tungsten Wire (0.25 mm diameter) | Raw material for creating ultra-sharp STM tips via electrochemical etching 9 . |
Sodium Hydroxide (NaOH) Solution (2M) | Etching solution for sharpening tungsten wire into fine tips 9 . |
System Type | Operating Environment | Best Suited For |
---|---|---|
Low Temperature (LT) STM | Ultra-high vacuum (UHV), temperatures below 5 K | Ultimate spectral resolution, studying superconductors 5 |
Electrochemical (EC-) STM | Liquid electrolyte, controlled potential | Real-time electrochemical processes, imaging in fluid 4 |
Ambient/Environmental STM | Air or controlled atmosphere, room temperature | Samples in real-world conditions, biological specimens 3 4 |
The journey of the scanning tunneling microscope from the world of physics to the heart of biology is a testament to scientific ingenuity. While it may not replace techniques like X-ray crystallography for determining the precise 3D atomic structure of proteins, STM has carved out a unique and vital niche 3 . Its power lies in its ability to visualize individual biomolecules and their assemblies without the always-necessary need for crystallization, operating in environments that can mimic the native state of these molecules.
Drug delivery systems at molecular scale
Ultra-sensitive detection of biomolecules
Understanding fundamental life processes
As the technology continues to evolve, with systems capable of operating in liquid cells with exquisite control, the potential for STM in biology is still being unlocked. Researchers believe it holds great promise for nanomedicine, biosensing, and the fundamental understanding of life at the molecular level 3 .
Forty years after its invention, the STM continues to fulfill its early promise, allowing us to see the invisible and better understand the intricate machinery of life, one atom at a time.
The invention of the Scanning Tunneling Microscope earned Gerd Binnig and Heinrich Rohrer the Nobel Prize in Physics in 1986, just five years after their first publication on the technique.