Plate I
On the Correlation of Divided Pairs
being the apparatus of Bell, drawn to the life, with its readings taken under two suppositions
the supposition under which the pairs are decided
turn to set the oven's pace
turn to rotate the magnet
turn to rotate the magnet
0 above · 0 below
0 above · 0 below
The Ledger of Coincidences
| both above | 0 |
| A above, B below | 0 |
| A below, B above | 0 |
| both below | 0 |
| pairs | 0 |
—of pairs answered alike, the magnets 45° apart
the classical supposition expects 25% divergence from it — the quantum supposition expects 15% divergence from it —
classical: a hidden directionquantum: one wave functionas measured
Of the apparatus. The oven divides an atom into two and sends one each way. Each magnet sorts its atom to the upper pole or the lower, along the magnet's own axis, and the atom leaves its grain on the plate behind. Turn a dial and the magnet turns in its ring. The ledger counts how often the two plates agree, and the chart sets down that agreement as a dot for every angle the reader has tried.
The classical supposition. Each pair leaves the oven with one hidden direction, drawn by lot. Each atom answers with the pole nearest that direction. Nothing about Magnet A can reach Magnet B. This is the best any local story can do, and it draws the straight dashed line: the agreement changes evenly with the angle.
The quantum supposition. The pair is one wave function. Whichever atom is measured first collapses it, and the other then answers with odds that follow the cosine of the angle between the magnets. That is the solid curve. At 45° apart it parts from the straight line by a fifth, and no hidden direction can be drawn that lands there.
The proof. Set the magnets 45° apart and move the slider. Let the plates fill. The dot settles on one curve or the other, and in the laboratory it settles on the cosine. Bell showed that no story in which each atom carries its own answer from the oven can bend the line so far. Something of the pair is shared at the moment of measurement, however far apart the magnets stand.
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