SPIN & STERN–GERLACH

In 1922 Stern and Gerlach sent a beam of silver atoms through a non-uniform magnetic field. Classical physics predicted one continuous smear; the plate showed exactly two spots. The awkward part comes with three analyzers in a row: measure along z, then along x, then along z again, and the last one still splits 50/50, because the x measurement erased everything known about z. In a uniform field the spin no longer splits but precesses about the axis at the Larmor frequency, proportional to the field strength.

▸ Heating the source oven · emitting a silver (Ag) atom beam…
▸ Building wedge-shaped N/S poles (non-uniform field)
▸ Quantizing the spin projection mₛ = ±½
▸ Chaining sequential SG analyzers (z · x · z)…
▸ Calibrating Larmor precession ω = γ·B…
▸ Ready — Online. ✅
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⌂ Particle physics & quantum

Simulation room Spin & Stern–Gerlach

Spin & Stern–Gerlach
Online
spin ½ · 2 spots · sequential SG · Larmor
Running configuration
🧲 1 máy SG trục z
Last measurement axis—
↑ spin up fraction—
↓ spin down fraction—
Atoms through—
Number of SG analyzers—
Quantum note
—
Pick a configuration on the right · adjust speed & field B · press 🔬 Diagram to see how spin splits into 2 spots
Result distribution over time (↑ / ↓ %) ↑ up↓ down
About Spin

In 1922 Stern and Gerlach sent a beam of silver atoms through a non-uniform magnetic field. Classical physics predicted one continuous smear; the plate showed exactly two spots. The awkward part comes with three analyzers in a row: measure along z, then along x, then along z again, and the last one still splits 50/50, because the x measurement erased everything known about z. In a uniform field the spin no longer splits but precesses about the axis at the Larmor frequency, proportional to the field strength.

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