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Compton Effect

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The Compton effect is the increase in wavelength of X-rays or gamma rays when they are scattered by electrons. Discovered by Arthur Holly Compton and published in 1923, it is conventionally regarded as the decisive evidence that light carries momentum in discrete amounts, and therefore as the strongest of the three classic arguments for the photon.

The standard account

Compton directed molybdenum K-alpha X-rays at a graphite target and measured the wavelength of the scattered radiation as a function of scattering angle. Classical Thomson scattering predicts that the scattered wave has the same frequency as the incident one. Compton found instead a shifted component, with

Δλ = (h/mec) (1 − cos θ)

where θ is the scattering angle. The constant h/mec is the Compton wavelength of the electron, 2.426 × 10−12 m. The shift depends only on angle — not on wavelength, not on the target material, not on intensity. Compton derived it by treating the collision as an elastic two-body encounter between a particle of energy hf and momentum hf/c and a free electron at rest, and applying conservation of energy and momentum. He shared the 1927 Nobel Prize in Physics with C. T. R. Wilson.

Two points of precision are worth keeping. First, the shift is an additive constant in wavelength, not a multiplicative one: for visible light it is utterly negligible, for hard X-rays it dominates. Second, the same kinematic formula can be obtained by treating the process as a double Doppler shift from a recoiling electron, a wave-mechanical derivation given by Schrödinger in 1927; what the photon picture adds is not the shift but the coincidence between individual scattered quanta and individual recoil electrons, which Bothe and Geiger demonstrated in 1925 and which is much harder to reproduce without quantization.

On this wiki

Two distinct interests run through the Compton material catalogued here.

Compton scattering as a redshift mechanism

The larger group treats the Compton shift as a candidate mechanism for cosmological redshift — a tired-light proposal in which light loses energy to scattering on its way to us rather than to the recession of its source. John W Kierein is the principal advocate here, in "Implications of the Compton Effect Interpretation of Red Shift", "The Compton Effect Interpretation of Solar Red Shift" and "Gravitation as a Compton Effect Redshift of Long Wavelength Background Radiation", the last extending the idea to gravitation itself. Related papers include "Cosmological Redshift, Compton Effect and Age of the Stars" and Biagio Buonaura's "Electromagnetic Waves, Inertial Transformations and Compton Effect".

The standard objection should be stated, because it is a real one and readers deserve it: Compton scattering redirects the photon as well as reddening it, so a scattering-based redshift would blur distant images and broaden spectral lines, and the sharpness of quasar images and of absorption lines at high redshift constrains such mechanisms severely. The wavelength dependence is also wrong — the Compton shift is additive in λ, whereas cosmological redshift is proportional to λ. Proponents here respond by invoking variant or forward-scattering mechanisms rather than ordinary Compton scattering; whether that rescue works is the substance of the dispute, and it is not settled by assertion on either side. See also the wider Tired Light and Redshift articles.

Compton scattering without the photon

The smaller group disputes the quantum reading of the effect itself.

The Compton effect belongs with the Photoelectric Effect and Blackbody Radiation as the standard trio of quantization arguments, and this wiki holds classical alternatives to all three; the Compton case is the hardest of the three for a classical account, because of the Bothe–Geiger coincidences rather than because of the wavelength shift.

See also