By Arthur Holly Compton, printed as Arthur H. Compton. Published in Physical Review 21, 483–502, May 1923. The Norwegian University of Science and Technology hosts this copy of the original paper.
Compton scattering experiment of 1923 2026-10-18
In Arthur Holly Compton's A Quantum Theory of the Scattering of X-rays by Light Elements (1923), pp. 494–495 and Figure 4 compare X-rays from a molybdenum target with rays scattered by graphite at right angles. Slits select the rays; a calcite crystal analyzes their wavelengths by Bragg's law. The plotted readout is scattered wave intensity against the crystal's glancing angle, distinct from the fixed photon deflection. The primary-beam comparison uses the same slits, crystal, and tube potential. First-order diffraction lines on both sides establish angular zero. The displaced spectral line supports a longer outgoing wavelength and hence photon energy transfer. The two curves use different vertical scales, so their heights cannot directly compare absolute wave intensities. The paper postpones a fuller apparatus description; it also states on p. 496 that recoil Electrons from ordinary X-rays had not been observed. Thus this spectral test infers recoil through the conservation model rather than directly tracking an Electron.[ref]
A Quantum Theory of the Scattering of X-rays by Light Elements by Arthur Holly Compton. Compton, Physical Review 21 (1923), pp. 494–496, Experimental Test, Figure 4 and opening of Velocity of recoil of the scattering electrons
Nobel Prize in Physics in 1927 2026-10-18
Awarded in equal shares to Arthur Holly Compton for the Compton effect and Charles Thomson Rees Wilson for making charged-particle paths visible by condensation. The Compton scattering experiment of 1923 and Wilson cloud-chamber experiment explain the two experimental methods.[ref]
The Nobel Prize in Physics 1927 by Nobel Prize Outreach. Official award record: Compton and Wilson, half shares and their distinct experimental subjects