Physics/Option Modules/Turning Points in Physics/Advantages Over Optical Microscopes
Physics · Turning Points in Physics · A2 Level

Advantages Over Optical Microscopes

The TEM and STM reach atomic-scale detail by two completely different mechanisms, but they solve exactly the same underlying problem: visible light simply cannot see anything as small as an atom, no matter how good the lenses are. This lesson ties the two instruments together and shows precisely why an electron beam can succeed where a light beam never could.

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Resolution is fundamentally limited by wavelength

Any imaging system — an eye, an optical microscope, a telescope, a camera — has a fundamental resolution limit set by the wavelength of the radiation it uses to form an image. Two points closer together than roughly one wavelength apart cannot be distinguished as separate objects, however precisely the lenses are ground or however much the image is magnified afterwards. This isn't an engineering shortfall that better manufacturing could eventually fix; it's a consequence of the wave nature of the illuminating radiation itself, and no amount of money spent on glass or polishing can get around it.

Visible light spans roughly $400$–$700\,\text{nm}$. That range sets a hard floor on what any light-based instrument can ever resolve. Individual atoms are typically spaced around $0.1$–$0.3\,\text{nm}$ apart — a distance around three thousand times smaller than the shortest visible wavelength. An optical microscope aimed at a single atom isn't looking at a slightly blurry dot; it's looking at nothing resolvable at all, because the wavelength doing the "looking" is thousands of times too coarse for a feature that small ever to register as a distinct point.

Why a better lens can't fix this

It's tempting to think resolution is just a matter of manufacturing quality — a sufficiently well-ground lens, polished to a sufficiently fine tolerance, should eventually resolve anything. It can't. The wavelength limit comes from diffraction: light spreads out slightly whenever it passes any aperture or lens, and that spreading sets a minimum size for the smallest resolvable feature, regardless of how perfectly the optics are made. The only way past the limit is to use radiation with a fundamentally shorter wavelength than visible light.

The electron's short wavelength as a way around the limit

The de Broglie relationship gives exactly that route around the limit. An electron accelerated through a potential difference $V$ behaves as a wave with wavelength

$\lambda = \dfrac{h}{\sqrt{2meV}}$
Because the electron's mass $m$ is so small, even a modest accelerating voltage produces a wavelength far shorter than any visible light — potentially short enough, in principle, to resolve individual atoms. This is the whole reason electron microscopy exists: swap the illuminating wave from a photon with a wavelength fixed by its colour, to an electron whose wavelength can be dialled down simply by increasing the accelerating voltage.

Worked exampleEstimating the voltage needed to resolve atomic-scale detail
1
Estimate the accelerating voltage needed to give electrons a de Broglie wavelength of the same order as the size of an atom, taking a typical atomic diameter as $\lambda \approx 1\times10^{-10}\,\text{m}$.
2
Start from $\lambda = \dfrac{h}{\sqrt{2meV}}$ and rearrange for $V$: squaring both sides, $\lambda^2 = \dfrac{h^2}{2meV}$, so
$V = \dfrac{h^2}{2me\lambda^2}$
3
Substitute $h=6.63\times10^{-34}\,\text{J s}$, $m=9.11\times10^{-31}\,\text{kg}$, $e=1.60\times10^{-19}\,\text{C}$, $\lambda=1\times10^{-10}\,\text{m}$:
$V = \dfrac{(6.63\times10^{-34})^2}{2\times9.11\times10^{-31}\times1.60\times10^{-19}\times(1\times10^{-10})^2}$
4
$V = \dfrac{4.396\times10^{-67}}{2.915\times10^{-59}} \approx 1.5\times10^{2}\,\text{V}$, of the order of a few hundred volts.
This is a remarkably small voltage — easily achievable with simple laboratory apparatus — for a wavelength short enough, in principle, to probe atomic-scale structure.
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Wavelength sets the limit, other factors set the reality

This calculation shows the de Broglie wavelength can reach atomic scale at readily achievable voltages — but in practice, the actual resolution of a real instrument falls well short of the electron wavelength itself, limited by lens aberrations, mechanical stability and sample preparation. Real electron microscopes typically use accelerating voltages from a few kV up to several hundred kV, both to shorten the wavelength further (for better resolution than this rough estimate suggests) and to give the beam enough energy to penetrate a sample. Even so, electron microscopes still resolve detail many thousands of times finer than any optical microscope, simply because their starting wavelength is so much shorter to begin with.

TEM and STM: two very different routes to the same scale

The transmission electron microscope and the scanning tunnelling microscope, covered in the previous two lessons, reach atomic-scale imaging by entirely different physical mechanisms, even though both end up competing with — and vastly outperforming — the optical microscope.

The TEM exploits exactly the short-wavelength argument above: a beam of electrons, accelerated to a short de Broglie wavelength, is fired through an ultra-thin sample and focused by magnetic lenses into a transmission image, in a direct (if much more capable) analogue of how an optical microscope shines light through a specimen. Its resolution is fundamentally tied to that electron wavelength, in the same way an optical microscope's resolution is tied to the wavelength of light.

The STM works completely differently, and doesn't rely on any beam or wavelength-based imaging at all. It brings a sharp conducting tip to within about a nanometre of a conducting surface and measures the quantum-mechanical tunnelling current that flows across the gap, scanning the tip while a feedback loop holds that current constant to trace out the surface's atomic-scale topography. No wavelength argument features anywhere in how an STM works — its resolution comes instead from how sensitively the tunnelling current depends on the tip-to-surface distance.

Two side-by-side schematic panels comparing a transmission electron microscope and a scanning tunnelling microscope. Left panel, labelled TEM: an electron gun at the top emits a downward beam, passing through two magnetic lens symbols, then through a thin flat sample, then continuing down to a screen at the bottom. Right panel, labelled STM: a sharp pointed tip is positioned just above a flat sample surface with a small gap between them, a curved arrow indicates the tip scanning left to right, and a dashed line represents the tunnelling current path across the gap.
TEM (left): an accelerated electron beam is focused by magnetic lenses and transmitted through a thin sample onto a screen. STM (right): a sharp tip scans just above a conducting surface, using the tunnelling current across the gap to map atomic-scale height.
Two very different routes to the same scale

The TEM and STM reach atomic-scale imaging by entirely different physical mechanisms: the TEM exploits the short de Broglie wavelength of a fast-moving electron beam to form a transmission image, much like an extreme version of an optical microscope; the STM exploits quantum tunnelling of electrons across a vacuum gap, with no beam or wavelength-based imaging involved at all. Both, though, only became possible once quantum mechanics — wave-particle duality on one hand, tunnelling on the other — was well enough understood to be engineered into working instruments, decades after the underlying theory was first developed.

Key takeaways

  • Any imaging system's resolution is fundamentally limited by wavelength: two points closer together than roughly one wavelength cannot be distinguished, regardless of lens quality.
  • Visible light's wavelength range ($400$–$700\,\text{nm}$) is thousands of times too coarse to resolve individual atoms (spaced $\sim0.1$–$0.3\,\text{nm}$ apart), so no optical microscope can ever image them.
  • An accelerated electron's de Broglie wavelength, $\lambda = h/\sqrt{2meV}$, can reach atomic scale ($\sim10^{-10}\,\text{m}$) at accelerating voltages of only a few hundred volts, in principle.
  • Real instruments use much higher voltages (kV to hundreds of kV) than this estimate, both for better resolution and to give the beam enough energy to penetrate a sample; real resolution still falls short of the wavelength itself due to lens aberrations and mechanical stability.
  • The TEM reaches atomic scale via a short-wavelength transmitted beam; the STM reaches atomic scale via quantum tunnelling current, with no beam or wavelength involved at all.
  • Both instruments only became possible once quantum mechanics was well enough understood to be engineered into working apparatus.