object

electron beam

A stream of electrons used as a projectile in scattering experiments.
12 related articles

Description

An electron beam is a stream of electrons moving in a common direction, typically at high speed. In physics, it is a versatile tool for probing matter: when electrons strike a target, their scattering patterns reveal the internal structure of atoms, nuclei, and even nucleons. Because electrons are charged and light, they can be focused and steered with electric and magnetic fields, making them precise probes. The beam's energy, intensity, and focus determine what it can resolve — from the arrangement of atoms on a surface to the distribution of quarks inside a proton.

History

The concept emerged in the late 19th century with the discovery of the electron by J.J. Thomson in 1897, who used a beam of electrons to measure their charge-to-mass ratio. The first practical electron microscope was built by Ernst Ruska in 1931.

How it works

Electrons are emitted from a source (e.g., a heated filament) and accelerated by an electric field. Magnetic lenses and steering coils shape the beam into a narrow, controlled stream. When the beam hits a target, electrons scatter off the electric fields of the target's constituents; detectors record the scattered electrons' angles and energies. By comparing the scattering pattern to theoretical models, physicists infer the target's structure. In accelerators, the beam can be stored in a ring or delivered in pulses, with its properties tuned for specific experiments.

In practice

Electron beams are used in electron microscopes, semiconductor lithography, and in particle accelerators for scattering experiments that probe nuclear and particle physics, such as the SoLID spectrometer project.

Fun fact

In a storage ring, an electron beam can be kept circulating for hours, traveling a distance equivalent to several trips to the Sun.

Concept graph →

Related articles · 12

Electron Microscope Leaves the Vacuum: Seeing Hot and Wet
The electron beam of a microscope usually flies through emptiness, like a courier on an empty highway. Any air molecule is a bump that makes it bounce and lose direction. So before, to examine a sample, you had to freeze it, dry it, or coat it with metal—and still you could only look in a vacuum.
A Chorus of Electrons in Helium: Next-Generation Cherenkov Light
The blue glow in water around a nuclear reactor is light born when a charged particle outruns light in that medium. The effect was discovered by Pavel Cherenkov in 1934, with the theory provided by Igor Tamm and Ilya Frank.
Plasma waveguide for twisted electrons
A laser pulse slams into a gas cloud and knocks electrons out of it, leaving behind a bubble: a cavity almost devoid of particles. This bubble races through the plasma at nearly the speed of light, and its walls drag along the electrons trapped inside, much like a speedboat tows a water skier.
Optics2026-08-112 minarXiv:2608.10582express
Weighing an Electron Beam
An electron beam is a stream of tiny particles carrying an electric charge. When such a beam hits a material, it doesn't just heat it or knock out atoms: it also gives the surface a slight push, like a jet of water pushing against your palm.
Plasma Physics2026-08-021 minarXiv:2608.01323express
How the Electron's Shape Controls Gamma Light
An electron is not just a point. It is a probability cloud, smeared out in space. When such a cloud collides with a powerful laser pulse, it can emit a high-energy photon — a gamma quantum. And this photon can be not just ordinary but twisted, like a corkscrew, carrying orbital angular momentum.
physics.acc-ph2026-03-291 minarXiv:2603.27692express
The beam squeezes itself
An electron beam in an accelerator is like a flock of birds: it flies in a tight group, but over time it spreads out. To keep particles together, heavy magnets are usually used. Here they did without them — the beam squeezed itself.
Space Physics2026-03-111 minarXiv:2603.10760express
Beams from Jupiter's Poles
Above Jupiter's poles, auroras blaze as electrons are accelerated by electric fields and slam into the upper atmosphere, making the gas glow. But not all electrons head downward. Some, it turns out, get a kick in the opposite direction — away from the planet, into deep space.
physics.acc-ph2026-02-221 minarXiv:2602.19081express
Light from a Perfectly Even Stream
Modern X-ray light sources are like an orchestra without a conductor: electrons in the beam fly every which way, and the radiation comes out blurry. The new idea is to make electrons line up in neat rows with a spacing of a few nanometers. Then the light they emit becomes coherent, like a laser beam.
physics.acc-ph2026-02-131 minarXiv:2602.12765express
An Electron Beam as Fine as a Pencil
An electron beam can be compared to the light from a laser pointer: if it diverges, the spot on the wall quickly spreads out. In the lab, physicists created such a narrow beam that it remained thin over a long distance, like the beam of a good pointer.
physics.acc-ph2026-02-021 minarXiv:2602.01504express
Electron beam trapped in a ring the size of a dinner plate
A ring the size of a dinner plate made an electron beam run in circles. Its diameter is 22 centimeters, and a full turn takes just 4.7 nanoseconds. To put that in perspective: in one second, such an electron would complete more than two hundred million laps.
Instrumentation2026-01-261 minarXiv:2601.18311express
X-ray Light from the Lab
An X-ray telescope captures light from hot gas around stars, but that light arrives 'blurred'—like a voice over a bad phone line. To make out the words, you need a dictionary of the exact frequencies at which atoms glow. Such a dictionary is written not only with calculations but also with direct experiments.
A Wide-Angle Lens for the Subatomic World
At Jefferson Lab, electrons are accelerated to 12 GeV and smash into protons to pry out their secrets. But existing detectors are like cameras with a narrow field of view: you either see a lot but dimly, or brightly but only a tiny patch. Electron scattering is the main tool, but statistics are insufficient for subtle effects.