• Pixel-art sticker of Comptessa, personifying Compton Scattering, with the caption “Bounced And Stretched.”

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Comptessa

Compton Scattering Physics

\[\Delta\lambda = \frac{h}{m_e c}(1-\cos\theta)\]
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Meet Comptessa, an X-ray photon bounced and stretched: bouncing off an electron, she hands over some energy and comes out with a longer wavelength. Her shift depends only on the scattering angle, in units of h/mec, about 2.426 pm. Pixel-art kiss-cut sticker in 2, 3, 4 and 6 inches; equation, symbols and sources in the physics panel below.

Size
Surface

Flat $6 shipping worldwideMade to order, ships in 2–5 business days

Details

Size3″ × 3″

3″ × 3″ kiss-cut sticker.

Shipping

Flat $6 shipping on every order, worldwide, whatever's in it.

Delivery times & where we ship

Returns & replacements21 days

Every item is printed to order, so we can’t accept returns or exchanges for change of mind, or if you ordered the wrong size or colour.

Print defect, misprint, damage or the wrong item? We’ll send a free replacement, or a refund if you prefer. Report it within 21 days of delivery with a photo; no need to send it back.

Full refund & replacement policy

The physics

Meet Comptessa, an X-ray photon who bounces off an electron and comes away a little redder.

In 1923 Arthur Compton fired X-rays at a target and found that scattered X-rays had longer wavelengths than the incoming ones. Classical waves could not explain this. Treat the X-ray as a particle carrying momentum h/λ, though, and it becomes a billiard-ball collision: the photon gives some energy and momentum to an electron, and its wavelength grows by an amount that depends only on the scattering angle θ.

The scale is the Compton wavelength of the electron, h/(m_e c) ≈ 2.426 picometres. A photon scattered at 90° gains exactly that much wavelength; one bounced straight back gains twice that. For visible light, with wavelengths around 500 nanometres, the shift is far too small to notice, which is why X-rays were needed.

The result was strong evidence that light carries momentum in quanta. Compton shared the 1927 Nobel Prize in Physics for it.

The formula assumes a free electron at rest. Electrons bound in atoms add a spread to the measured shifts.

Equations

\[\Delta\lambda = \frac{h}{m_e c}(1-\cos\theta)\]
Symbols
SymbolMeaningUnit
\(\Delta\lambda\) increase in wavelength \(\mathrm{m}\)
\(h\) Planck constant \(\mathrm{J·s}\)
\(m_e\) electron mass \(\mathrm{kg}\)
\(c\) speed of light in vacuum \(\mathrm{m/s}\)
\(\theta\) photon scattering angle \(\mathrm{rad}\)