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Bifurcor

Stern–Gerlach Experiment / Spin Quantization Physics

\[F_z = \mu_z\,\frac{\partial B_z}{\partial z}\]
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Bifurcor is a Pixelated Physics law character, one of our quantum designs. Stern–Gerlach: silver atoms in a steep magnetic gradient split into exactly two beams, spin up or down, never a smear. This is a 3" × 3" pixel-art sticker. The physics panel below gives the equation, what each symbol means and the sources.

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Size3″ × 3″

3″ × 3″ kiss-cut sticker.

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The physics

A magnetic field that changes with height pushes on an atom's magnetic moment. Because an electron's spin can only point up or down, silver atoms in the Stern–Gerlach magnet split into exactly two beams instead of smearing out.

Bifurcor runs a toll booth with two lanes, and he does not take requests.

His booth is a magnet built lopsided on purpose: a knife-edge pole above, a grooved pole below, so the field changes steeply with height. A small magnet driving through a field like that feels a force set by its magnetic moment along the field, the first line on this page. Classically, silver atoms with randomly tilted moments should smear into one broad band.

In Frankfurt in 1922 Walther Gerlach and Otto Stern sent a beam of silver atoms from an oven through such a magnet and onto a glass plate. The deposit was too thin to see at first; as Friedrich and Herschbach recount, the sulphurous smoke of a cheap cigar helped turn the silver black. The trace was not a band. It split in two, with nothing in the middle.

They called it Richtungsquantelung, space quantisation, and read it as support for the Bohr–Sommerfeld atom. Nobody had proposed spin yet. In 1925 George Uhlenbeck and Samuel Goudsmit suggested that the electron carries its own intrinsic angular momentum, and only later was the Frankfurt split reinterpreted as the spin of silver’s single outer electron: two values, plus or minus one half, the second line. Stern received the 1943 Nobel Prize for the molecular-ray method.

So Bifurcor never discovered spin. He asks one question about one axis, and the answer has only two values: plus a half goes up, minus a half goes down. A second booth turned sideways would split each lane fifty-fifty all over again, because a definite answer about one axis leaves the other undecided.

Two lanes. No middle lane.

Equations

\[F_z = \mu_z\,\frac{\partial B_z}{\partial z}\]
\[\begin{gathered} \mu_z = -g_s\,\mu_B\,m_s \\ m_s = \pm\tfrac{1}{2} \end{gathered}\]
Symbols
SymbolMeaningUnit
\(F_z\) force on the atom along the field gradient \(\mathrm{N}\)
\(\mu_z\) z-component of the atom's magnetic moment (for silver, set by its one outer electron) \(\mathrm{J/T}\)
\(B_z\) z-component of the magnetic field \(\mathrm{T}\)
\(z\) position along the gradient, up the page \(\mathrm{m}\)
\(g_s\) electron spin g-factor, about 2.0023 \(\mathrm{1}\)
\(\mu_B\) Bohr magneton \(\mathrm{J/T}\)
\(m_s\) spin projection quantum number: only +1/2 or −1/2 \(\mathrm{1}\)

Source Gerlach, W.; Stern, O. (1922). Der experimentelle Nachweis der Richtungsquantelung im Magnetfeld. Zeitschrift für Physik 9, 349–352.doi.org/10.1007/BF01326983 (opens in a new tab)