Part 8 — The Transition to Quantum Physics
- Black-Body Radiation and Planck's Hypothesis
- The Photon: Photoelectric and Compton Effects
- Atomic Models and Spectra
- Matter Waves
- Experiment: Franck–Hertz experiment
- Experiment: The Blackbody Spectrum Measured experiment
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Experiment: The Photoelectric Effect and Compton Scattering
experiment
- Hertz and Hallwachs: ultraviolet light discharges a metal (1887–1888)
- Lenard: the energy of the electrons ignores the intensity (1902)
- Millikan: the slope of the line is $h/e$ (1916)
- Compton: the wavelength of scattered X-rays changes (1923)
- Bothe and Geiger: the two products appear together (1925)
- Grangier, Roger and Aspect: a single quantum is not split (1986)
- What the measurements settle
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Experiment: Matter Waves Observed
experiment
- Davisson and Germer: electron diffraction by a crystal (1927)
- Thomson and Reid: transmission rings from thin films (1927)
- Estermann and Stern: helium and hydrogen diffracted (1930)
- The electron double slit, one electron at a time (1961–1989)
- Colella, Overhauser and Werner: gravity shifts a phase (1975)
- Molecule interferometry and the edge of coherence (1999–2019)
- What the measurements settle
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Experiment: X-ray Spectra and the Charge of the Nucleus
experiment
- Röntgen: a new kind of rays (1895)
- Barkla: characteristic radiation and the transversality of X-rays (1905–1911)
- Friedrich, Knipping and von Laue: diffraction by a crystal (1912)
- The Braggs: the reflection law and the X-ray spectrometer (1913)
- Moseley: the high-frequency spectra of the elements (1913–1914)
- Siegbahn: precision X-ray spectroscopy (1916–1925)
- What the X-ray spectra established