The Spacetime Metric

The physics of empty space,explained from the ground up.

03All-directions field

Every arrow points inward. There is no universal down.

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Compare a trajectory and a distribution

Study 1 of 7: The ground state

A stationary spread, not a fast jitter

Which picture are you looking at?
The clock runs only under the trajectory picture, because only the trajectory picture has anything that changes.

Scroll sideways if needed. Keyboard: focus the diagram frame, then use the arrow keys.

Two panels: a classical oscillator with a running clock, and the stationary ground state with a stopped clockOn the left, a bead on its own position axis swings between two turning points, with an energy axis beside it showing one level. A clock underneath counts periods. On the right, the same oscillator's energy axis shows the ladder of rungs with the lowest one marked, and a separate axis below it draws the ground-state probability density: a symmetric bell over position, with the central band shaded. The clock underneath is greyed out and reads nothing. Energy and probability are never drawn on the same axis in either panel.

Show me the trajectory picture

Energy, in units of ħω

Show me the trajectory picture

Show me the state

Energy, in units of ħω

Show me the state

Two pictures of the same ground state, side by side. Switch between them and watch the clocks. One picture has a bead swinging in a bowl and a clock counting periods; it is the intuition most readers arrive with, and this chapter teaches against it. The other is the state as it actually is — a spread over position that holds half a quantum and does not change with time at all. Its clock is greyed out because there is nothing for it to count.

Energy and the wavefunction are drawn on separate axes here, and they are never combined. Combining them onto one axis is measurably what makes readers read the height of a wavefunction as an energy and its width as a motion.The bead is drawn swinging to the amplitude a classical oscillator carrying exactly ½ħω would reach — one oscillator length, where ½mω²A² equals ½ħω. Same energy, and still the wrong picture of the state.Nothing here moves on its own. The clock advances only while you hold it running, and if your system asks for reduced motion it advances in visible steps instead of sweeping.Scope: the one-dimensional harmonic oscillator, drawn in its own units. It fixes the picture the chapter depends on and computes no laboratory quantity.

Show me the trajectory picture

The picture this chapter is teaching against

Here is the bead in the bowl. It has a position at every instant, it swings out to a turning point and back, and a clock underneath it counts the periods. This is a fair intuition for one thing only: an energy you cannot remove, because nothing you do brings this bead to rest. It is worth looking at carefully, and it is worth knowing what it is not: there is no hidden classical path underneath the quantum ground state for this bead to be tracing.

Clock: 0.00 periods

Show me the state

Nothing here changes with time, so this clock is stopped.

Here is the state. The spread over position is the whole of it — measure many independently prepared oscillators and this is how the results are distributed. Nothing in this panel changes with time, so the clock beneath it has nothing to count. The uncertainty principle forbids a definite position together with a definite momentum; it does not hide a trajectory under a blur. The spread is the state.

Clock: —

Ground-state energy
half a quantum, ½ħω
Share of measurements landing inside the shaded band
52%

OpenStax, University Physics volume 3, §7.5, the quantum harmonic oscillator — the stationary ground state and ½ħω, as taught

The state: a stationary spread over position holding half a quantum. The clock is stopped because nothing in this panel changes with time. Nothing here changes with time, so this clock is stopped.

An editorial light painting of two metal plates, with luminous wave-like texture around their gap.
Conducting boundaries
An editorial painting of a superconducting chip illuminated by microwave wavefronts.
Phase-coherent circuits

Start here

A circling charge radiates, so the Bohr atom should pour out its energy and collapse into the nucleus in about ten picoseconds. It does not.

Hal Puthoff's 1987 paper gives the mechanism: the power the orbiting electron radiates away and the power it absorbs from the zero-point field of the vacuum balance, and the radius where they balance is exactly the Bohr radius.

The Pons–Fleischmann Palladium Cell

What did a palladium rod, heavy water, and a careful heat ledger show?

Pons and Fleischmann turned a tiny metal cell into a question with an energy ledger: where did the extra heat come from?

Curriculum
  1. IHow to know
  2. IIThe medium
  3. IIIEnergy from the vacuum
  4. IVMass, inertia and gravity
  5. VEngineering the metric
  6. VIThe craft and the ledger