By Walther Gerlach and Otto Stern. Zeitschrift für Physik 9, 349–352 (1922), received 1 March. English translation by Martin Bauer, arXiv:2301.11343v1, 26 January 2023.
Cited passages: Experimental setup; Results, Figures 1–5; closing measurement caveat.
In 1922, Otto Stern and Walther Gerlach used an electrically heated oven to emit neutral silver chemical atoms. Two platinum apertures, a pinhole and a slit – wide, supplied collimation. The beam passed along a knife-edge pole in a nonuniform magnetic field. At its end, a glass plate collected the condensed silver. Continuous pumping maintained vacuum; the thin deposit required development even after eight hours.[ref]
The field-off image established the undeflected slit width. A comparison put field-on and field-off deposits on the same plate. Microscopy revealed two deflected bands, no detectable central component, and broadening attributed to the velocity distribution. Alignment and distance from the knife-edge affected the pattern; precise magnetic field gradient measurements were still pending.[ref]
The apertures act as a collimator: they constrain the initial transverse positions and velocities, so a magnetic displacement can be distinguished from an initially broad beam. Vacuum reduces collisions that would destroy this preparation. Deposition integrates arrivals over the exposure; a darkened band is not a time-resolved record of individual chemical atoms. The field-off comparison tests whether the magnet changes the spatial distribution, while alignment checks address a geometric source of apparent asymmetry. Finite sensitivity qualifies the absence of a central deposit: it is an experimental upper limit, not a proof that exactly zero atoms landed there.
Figure 1.
From an oven to a silver deposit, and a separate ideal flight model
. The upper schematic shows the historical sequence without reproducing the original image. The lower diagram introduces the hypothetical constant-gradient magnet length and additional drift distance used below. The historical plate was at the magnet exit; the extra drift is a modeling choice. Details.