In 1927, C.J. Davisson and L.H. Germer performed an experiment known as the Davisson Germer experiment to explain the wave nature of electrons through electron diffraction.
A low voltage power supply was used to heat an electron gun with a tungsten filament F coated with barium oxide.
When a suitable potential difference is applied from a high voltage power supply, the electron gun emits electrons that are then accelerated to a specific velocity.
These emitted electrons were made to pass through a cylinder perforated with fine holes along its axis, producing a finely collimated beam.
The cylinder's beam is once more directed toward the surface of a nickel crystal. As a result, electrons scatter in various directions.
The intensity of the electron beam produced is measured by the electron detector after it is connected to a sensitive galvanometer (to measure voltage).
An illustrative setup of the experiment is shown below.