From one sentence to the sky · Step 13 of 15
The expansion rate
The shares and the age fix the rate. Arithmetic, not a choice. It lands on the oldest light’s side of the argument. An earlier rate died, and it is shown.
The universe is expanding. How fast, today? Physics has two answers that do not agree. The oldest light in the sky gives a lower number. The ladder of nearby stars gives a higher one. This is the Hubble tension.
The count does not pick a side. It closes. The shares of step eleven and the age of step twelve go into the standard equation that links them. Out comes a rate. That is arithmetic, not a fit.
It lands on the oldest light’s side. Its window is the age’s own window, turned into a rate.
The ladder’s higher number is not the expansion rate here. If it is confirmed, this row dies. And the age dies with it.
There is a corpse beside this row. An earlier rate came from the faint extra pull at the edges of galaxies, read backwards. It sat on the ladder’s side. On 3 September 2026 it fired, against the work’s own derived rate. It had been written down with a bar too narrow: the paper had left out a known uncertainty. The registration was the error. A fired switch is not repaired. It is shown.
The faint pull itself still stands. At the closed rate it sits inside its own measured bar.
What it stands on
What it predicts
The expansion rate today, with a window. And the faint floor of extra pull at the edges of galaxies, at that rate.
Paper: AP48
Paper: AP18
Paper: AP18
What would kill it
KS-ASM.1 fires if the expansion rate, as the data settle it, lands outside 64.4–70.8 in either directionFrom the frozen document, 2026-09-04-H0-KS-ASM.1. Frozen before the measurement.
It dies if a dark-matter particle turns up in the right amount (KS-42.1), or if galaxies break the floor or its formula (KS-3, KS-45).From the wall, the420code.org/physics/.