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The Bethe formula tracks radiation through matter

In 1930 Hans Bethe derived a formula for how fast charged particles lose energy passing through matter, still used across physics today.

Hans Bethe
Hans Bethe · 1906–2005
Person
Hans Bethe
Lived
1906–2005
Field
Theoretical physics
From
German-born American

The story

Hans Bethe earned his doctorate under Arnold Sommerfeld in Munich in 1928. In 1929 he moved to the Technische Hochschule in Stuttgart to work with Paul Ewald, and there he tackled a basic question: when a fast charged particle, such as a proton or an alpha particle, travels through a material, how quickly does it lose its energy?

Starting from Max Born's interpretation of quantum mechanics, Bethe produced a compact formula for these collisions. His paper, "On the Theory of the Passage of Fast Corpuscular Rays Through Matter", served as his habilitation thesis in 1930, the qualification for teaching at a German university. Bethe himself considered it his greatest paper. In 1930 he went to the Cavendish Laboratory in Cambridge on a Rockefeller fellowship, and at the request of Patrick Blackett, who was studying particle tracks in cloud chambers, he extended the formula to particles moving close to the speed of light. The relativistic version appeared in 1932.

The result, known as the Bethe formula, gives the average energy a charged particle loses per unit of distance as it passes through matter, a quantity called stopping power. In Bethe's theory the material is described by a single number, its mean excitation energy. In 1933 Felix Bloch showed how to estimate that number, so the result is often called the Bethe–Bloch formula. Later physicists added corrections for slower particles, and they are built into widely used programs that calculate the stopping power of protons and alpha particles.

The Nobel Foundation described Bethe's collision theory as simple and powerful, and noted that it gave nuclear physicists a tool for determining the stopping power of matter for fast charged particles. Physicists use it to work out how far radiation penetrates a material, which matters for designing particle detectors and shielding.

The same physics underlies proton therapy for cancer. Because a proton loses energy faster as it slows down, it deposits most of its energy near the end of its path, in a sharp maximum known as the Bragg peak. Doctors exploit this to concentrate the dose on a tumour while sparing healthy tissue around it.

Why it matters

A calculation made in 1930 remains part of the everyday toolkit of nuclear, particle and medical physicists nearly a century later.

About Hans Bethe

Refugee physicist who explained how the stars shine, led theory at Los Alamos, cracked the Lamb shift and spent half a century campaigning against the nuclear arms race; Nobel Prize 1967.

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Hans Bethe
1906–2005 · Theoretical physics
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