Amplitude amplification
Seven amplitude bars share one baseline; the marked accent bar climbs as the six unmarked bars sink by the share it takes, then the whole set retraces.
Seven amplitude bars share one baseline; the marked accent bar climbs as the six unmarked bars sink by the share it takes, then the whole set retraces.
Four nested entangling layers turn a quarter revolution per cycle in alternating directions, winding against each other like a mechanism.
A control wire drops onto each block of a doubling ladder in turn while the live block steps along the target rail and doubles its width.
A circuit stack grows layer by layer while the coherence ceiling settles toward it, and drops back to one layer at the moment they meet.
A probe wave slides half a period against a fixed reference and flattens as it goes, running from constructive to cancelling and back.
A token runs the measure, optimise and prepare circuit once per cycle while the cost read-out at the centre steps down a notch at each station.
A scan head crosses a row of register cells once per cycle and inverts the one marked cell as it passes, clearing it again on the next approach.
A bracket halves the interval holding the eigenphase three times until it closes on a single graduation, where the estimate lands.
A quarter-turn arc runs the ring once per cycle and the control node at the top takes a kick each time the arc's tail leaves it.
Five register words sit on full-width tracks; the estimate clears from the least significant end and redraws from the most significant, always reading as a prefix.
Four amplitude markers reflect across a mean rule, each landing as far beyond it as it started short of it, turning a falling set into a rising one.
The error whisker on a sampled estimate tightens onto the estimate rule as shots accumulate, then reopens for the next batch.
A sweep scrubs the cost axis while markers ride the classical and quantum curves, opening and closing the vertical gap that is the speedup.
An amplitude vector unwinds to the start axis then steps back toward the target axis in four equal kicks, holding on each graduation.
A parameter marker lifts to the rim of an energy curve and walks back down to the basin floor in shortening steps, with a drop rule following it along the floor.