How Scanning Electron Microscopy Works
Understand the principles behind scanning electron microscopy, from electron sources to image formation.
Scanning electron microscopy (SEM) uses a focused beam of electrons to image sample surfaces with nanometer resolution. Unlike optical microscopes limited by the wavelength of visible light (~400-700nm), SEMs achieve resolution down to 1-5nm by using electrons with wavelengths less than 0.1nm at typical accelerating voltages.
The SEM Column
The electron optical column is the heart of the SEM. It generates, accelerates, and focuses electrons onto the sample surface with precise control.
Electron Sources
Three types of electron sources are commonly used, each with different characteristics:
Tungsten Filament
A heated tungsten wire emits electrons through thermionic emission. Most affordable option with moderate resolution. Filament lifetime: 40-100 hours.
LaB6 (Lanthanum Hexaboride)
Brighter source with longer lifetime than tungsten. Better resolution and signal-to-noise ratio. Requires better vacuum conditions.
Field Emission Gun (FEG)
Highest brightness and resolution. Cold FEG or Schottky emitters. Best for high-resolution and low-voltage imaging. Most expensive option.
Electromagnetic Lenses
Unlike optical lenses made of glass, SEM uses electromagnetic lenses to focus the electron beam. Current flowing through copper coils creates magnetic fields that bend electron paths. The main lenses include:
- Condenser Lenses: Control beam current and initial focusing
- Objective Lens: Final focusing of the beam onto the sample
- Scan Coils: Deflect the beam to raster across the sample surface
Apertures
Small openings in the column limit the beam diameter and reduce spherical aberration. Smaller apertures give better resolution but lower beam current. Selecting the right aperture balances resolution and signal strength.
Electron-Sample Interactions
When the focused electron beam strikes the sample, various signals are generated from different interaction volumes:
Secondary Electrons (SE)
Low-energy electrons (<50eV) ejected from near the surface. Provide excellent topographic contrast showing surface morphology, texture, and edges.
Backscattered Electrons (BSE)
High-energy beam electrons elastically scattered by atomic nuclei. Signal intensity depends on atomic number—heavier elements appear brighter (compositional contrast).
Characteristic X-rays
X-rays emitted when beam electrons eject inner-shell electrons. Each element produces X-rays at specific energies—enables elemental analysis via EDS.
Other Signals
Auger electrons (surface chemistry), cathodoluminescence (optical properties), specimen current (conductivity), and transmitted electrons (thin samples).
Vacuum System
The SEM column requires vacuum for several reasons:
- Electron Path: Gas molecules scatter electrons, degrading beam quality
- Electron Source: Filaments oxidize and fail in air
- Detector Function: Many detectors require vacuum to operate
- Sample Contamination: Hydrocarbons in air deposit on samples under the beam
Modern desktop SEMs achieve operating vacuum in under 90 seconds using turbomolecular or scroll pumps combined with efficient chamber designs.
Operating Parameters
Accelerating Voltage (kV)
The voltage that accelerates electrons from the source. Higher voltage means:
- Better resolution (shorter electron wavelength)
- Deeper beam penetration (larger interaction volume)
- More sample damage potential
- Better X-ray excitation for EDS
Lower voltages (1-5kV) are preferred for surface-sensitive imaging and beam-sensitive samples. Higher voltages (15-30kV) are used for EDS analysis and subsurface information.
Working Distance
The distance from the objective lens to the sample surface. Shorter working distances generally provide better resolution but less depth of field. Longer working distances are needed for large samples, tilted samples, or when using certain detectors.
Beam Current
The number of electrons striking the sample per second. Higher beam current provides stronger signals but larger probe size (reduced resolution). Low beam currents minimize sample damage for sensitive specimens.
Image Formation
The electron beam scans across the sample in a raster pattern (left to right, top to bottom). At each point, detector signals are measured and displayed as pixel brightness on the monitor. The scan is synchronized between beam position and display, creating a magnified image of the surface.
Magnification is simply the ratio of display size to scan area. Scanning a smaller area produces higher magnification. Unlike optical microscopy, SEM magnification is controlled electronically with no lens changes required.
Desktop vs Floor-Model SEMs
Desktop SEMs like the SNE-Alpha achieve performance comparable to floor-model instruments in a compact package:
- Resolution: 5nm or better—sufficient for most applications
- Footprint: Fits on a standard lab bench
- Ease of Use: Simplified operation, faster learning curve
- Cost: Significantly lower acquisition and operating costs
- Maintenance: Less complex, lower maintenance requirements
Recommended Equipment
Related Technology
Resources
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