It is pointed out that the hypothesis that the electron has a diameter comparable with the wave-length of the hard ??-rays will account qualitatively for these differences, in virtue of the phase difference between rays scattered by different parts of the electron. The scattering coefficient for different wave-lengths is calculated on the basis of three types of electron: (1) A rigid spherical shell of electricity, incapable of rotation; (2) a flexible spherical shell of electricity; (3) a thin flexible ring of electricity. All three types are found to account satisfactorily for the meager available data on the magnitude of the scattering coefficient for various wave-lengths. The rigid spherical electron is incapable of accounting for the difference between the emergent and the incident scattered radiation, while the flexible ring electron accounts more accurately for this difference than does the flexible spherical shell electron.
It is concluded that the diameter of the electron is comparable in magnitude with the wave-length of the shortest ??-rays. Using the best available values for the wave-length and the scattering by matter of hard X-rays and ??-rays, the radius of the electron is estimated as about 2 ?? 10-10 cm. Evidence is also found that the radius of the electron is the same in the different elements. In order to explain the fact that the incident scattered radiation is less intense than the emergent radiation, the electron must be subject to rotations as well as translations.