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The experiment room

Wave function evolution

What does the equation do between measurements?

Fig. 07 — Wave function evolution
A single probability packet over a baseline, with dashed ghost outlines marking its shape at the start and end of the run. Controls play, pause and reverse the packet, which spreads as it drifts, and an arrow shows which way time is running. Measuring freezes the run and marks one position with a detection ring.t₀t₁FORWARDSMOOTH · REVERSIBLE · DETERMINISTICt = 0.00
The experiment never changes. What Copenhagen says about it does.

Unitary — information preserved

forward in time

Paused, pointing forward in time at t equals 0.00, packet width 0.06 of the baseline. The evolution is smooth, deterministic and reversible — running the same interval backwards returns the state exactly to where it began. Measuring is where the interpretations part ways: some add a genuinely irreversible step, others keep the dynamics unitary throughout and call the loss practical rather than fundamental.

t = 0.00

Explained by

Copenhagen

The orthodox view

Between measurements the equation runs the state forward smoothly and reversibly, and Copenhagen uses it without reservation. What it will not say is that the state is a thing evolving out in the world — it is the bookkeeping that yields probabilities when a measurement finally happens.

The orthodox account has two rules: unitary evolution between measurements, and collapse at measurement. Only the first is deterministic and reversible; the second is neither, and the theory never states which applies when. That gap is the measurement problem in one sentence, and every other interpretation on this page is an attempt to remove one of the two rules or to explain how they fit together.

Key assumptions

  • The wave function is a predictive tool, not an object
  • Measurement is a special, unanalysed act
  • A classical world of labs and screens is assumed, not derived

What it gets right

  • Matches every experiment with the least machinery
  • No extra worlds, particles, or equations
  • The working physicist's default for a century

What it gets questioned on

  • Never says what counts as a measurement
  • Puts a movable, unexplained cut through reality
  • Not one doctrine — Bohr and Heisenberg never fully agreed
06 · Bell's inequality
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