An Invisible Mark on the Lots

Original: "Mechanism of wavefunction collapse in measurements of separated quantum subsystems"
· Gregory D. Scholes
arXiv:2605.20111 · 2026-05-19 · CC BY 4.0 · 2 min
Two particles that always give matching results when measured may share a hidden phase chosen in advance, one that determines the outcome.

Picture two lots in a hat, and you and a friend draw them at the same time without looking at each other. Every time you get "yes," your friend gets "no," and vice versa. How is that possible if nobody is swapping the lots? In quantum mechanics, a similar puzzle arises for entangled particles: measuring one instantly determines the result for the other, even when they are kilometers apart.

The new idea says the pair of particles carries a shared hidden phase, like an invisible mark on the lots made before they were handed out. That mark is what decides which side each lot lands on.

It used to be thought that a measurement result pops up at random at the very moment of observation, and no one could explain why distant particles always produce matching outcomes. Now it has been shown that the phase of the superposition, meaning the way a particle's possible states are "tilted," can be randomly encoded in one of the particles when they are created. When the particles separate, this phase becomes shared by both and steers each measurement toward its own result. That is why the sequence of outcomes for one particle looks random, while for the pair it is always consistent, with no signals passing between them.

This view also explains experiments with three particles, where under some device settings all three pass, and under others only half do. It requires nothing supernatural: no hidden variables, no instantaneous messages. One question remains: when exactly does the phase get fixed? That can be tested by comparing how two excited atoms emit light when they are together and when they have been separated. If the emission rate of separated atoms matches that of a single atom, then the phase was set before the separation. And so the invisible mark on the lots becomes a testable part of quantum mechanics.

The contextual phase is invisible in the composite space: two different classes give the same entangled state, but when the subsystems are separated they lead to opposite measurement outcomes. It is like a coin whose two sides look identical until it lands on the table.

The idea of a hidden phase that predetermines the outcome of a measurement echoes Ted Chiang's story "Story of Your Life", where an alien language reveals the simultaneity of all events. Here, though, the phase does not grant access to the future; it merely explains correlations after the fact.

\Psi^- = \frac{1}{\sqrt{2}}(|H\rangle_A|V\rangle_B - |V\rangle_A|H\rangle_B)
An entangled pair in which the polarizations are always opposite
\Psi^-(class 1) = \frac{1}{\sqrt{2}}(|V'\rangle_A|H'\rangle_B + |H'\rangle_A|-V'\rangle_B)
An alternative way of writing the same state with the phase assigned to subsystem B
Concepts
Wave Function Collapse measurement problem quantum measurement superposition superposition principle gravitational decoherence wave function quantum properties entangled photon pairs squeezed state theorem on the monogamy of entanglement schrodinger cat state entanglement measure collapse bell states Born rule single spin manipulation flux quantization correlation phase separation