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Live in the Cloud — probability samples display. In Free the switch needs A and B on different energy levels (NA ≠ NB); in Classic it is the exposé — the 2011 state's current is identically zero, so the tracers stand still while the cloud morphs through them. Full explanation in the notes below.

The three numbers

The quantum harmonic oscillator is a particle in a bowl-shaped potential — the quantum version of a mass on a spring. Its eigenstates are labeled nx, ny, nz: how many times the wavefunction crosses zero along each axis.

The energy depends only on the total N = nx+ny+nz, so states like 2,0,0 and 1,1,0 share an energy level — same energy, different shape.

The animation: superposition

Classic: the animation this page ran from 2011, Ψ = cos t·ψA + sin t·ψB with real weights. The cloud morphs A → B → A — but this is no Hamiltonian's evolution: a real wavefunction carries identically zero probability current, so the density teleports rather than flows.

Free: the true unitary superposition Ψ = (ψA + e−iωtψB)/√2, with ω the energy difference. The weights are fixed; only the relative phase winds, and the density sloshes through the interference term ψAψB cos ωt. Pick A and B on the same energy level and the cloud stands still.

Driven: a resonant field couples the two levels and the state Rabi-oscillates, Ψ = cos(Ωt/2)·ψA − i·sin(Ωt/2)·ψB. The weights themselves cycle, so the cloud morphs from A to B and back — the relative phase pinned at −π/2, which is why the morph is clean.

Reading the picture

Brightness follows the probability of finding the particle there. Blue marks regions where Re Ψ is positive, red where it is negative. Dark planes are nodes — the zero crossings counted by nx, ny, nz.

The Slice and Cutaway displays expose structure hidden inside the cloud, and lowering the brightness thins it.

Weak measurement & current

In the Cloud display, the probe slider softens the position measurement: a Gaussian meter of width σ applied to |ψ|². Each measure click drops a marker at the outcome and recentres the probe; run repeats this with a narrowing probe, collapsing the cloud onto a wandering point while the superposition sloshes underneath.

The current switch sets a particle ensemble flowing along the Bohmian velocity j/ρ — what a weak momentum measurement returns — integrated on the GPU, with the ensemble size adapted to your hardware. In free mode the ensemble stays Born-distributed as it moves (the continuity equation), so the flowing particles are the density: the cloud sloshes because the current carries it.

In classic mode the switch runs the same honest computation on the 2011 state, and the answer is the autopsy: that state is real, so j/ρ is identically zero. The tracers stand still while the cloud morphs through them — the continuity violation that fifteen years of morphing was hiding, made visible.

In driven mode the switch stays off, honestly: for the two-level Rabi state, no spatial current transports the density — population transfer runs through the drive coupling, and j/ρ for the truncated state fails the continuity equation. The exact driven state only conserves probability once the counter-rotating corrections are kept.