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Quantum

intermediate · Interactive lab

Entanglement

Two gloves in two boxes are correlated: open one and you know the other. An entangled pair agrees in every question you can ask it, and still carries no message. Telling those apart is the lesson.

By the end: Tell an entangled pair from a pre-agreed one by the only thing that separates them: agreement in more than one basis.

Your challenge

Start here. This lab opens with every claim marked as shown by the bench, which is the wrong starting point: two of these the bench actually refuses, one is settled by the theory rather than by any run, and one would need a real Bell test. Read the experiment on each row and judge it.

See it happen

Two pairs, two questions

Pairs: not alike
Slowed down so you can follow
PAIR SOURCE|+⟩and a coin in a boxTHE PAIRSBOTH DETECTORSZ BASISanswers 0 and 1TALLYTHE QUBITTHE COIN
A source makes a pair and sends one side to each detector. Both sides are measured in the chosen basis, and the tally counts how often the two answers agreed — for an entangled pair and for a pre-agreed pair alike.
  1. Pair source → The pairs
  2. The pairs → Both detectors: one question
  3. Both detectors → Tally
STEP 1 / 6

Two kinds of pair

The Pair source makes both: an entangled pair, and a pre-agreed pair carrying one bit chosen when it was made. Watch how often the two sides agree.

Configure

Your verdict on each claim

Judge each claim about the two kinds of pair. Some the bench settles, some it refuses, and some need a different kind of answer altogether.

What does the bench say about the two pairs?
The bench shows it
· The experiment on this row supports it.
The bench refuses it
· The experiment on this row contradicts it.
Ruled out by the theory
· It follows from the model, not from these runs.
This bench cannot say
· It needs a real Bell test, or a real device.
  1. P-901 — Asked the Z question, both kinds of pair always agree

    The question the pre-agreed bit was written in.

    Experiment
    Measure both sides of each pair in the Z basis · 200 trials, for an entangled pair and a pre-agreed pair
    Entangled pair
    the two sides agreed 200 of 200 times
    Pre-agreed pair
    the two sides agreed 200 of 200 times
  2. P-902 — Asked the X question, both kinds still always agree

    The same two sources, the same number of pairs, one different question.

    Experiment
    Measure both sides of each pair in the X basis · 200 trials, for an entangled pair and a pre-agreed pair
    Entangled pair
    the two sides agreed 200 of 200 times
    Pre-agreed pair
    the two sides agreed 102 of 200 times
  3. P-903 — One bit agreed in advance explains the entangled pair too

    The gloves-in-boxes story, stated as a model of the entangled source.

    Experiment
    Measure both sides of each pair in the X basis · 200 trials, for an entangled pair and a pre-agreed pair
    Entangled pair
    the two sides agreed 200 of 200 times
    Pre-agreed pair
    the two sides agreed 94 of 200 times
  4. P-904 — The near side's own answers change when the far side is asked something else

    Only the near side is counted; the far detector is switched between runs.

    Experiment
    Entangled pair: measure the near side in X while the far side is measured in Z · 200 trials
    The near side alone
    95 × +, 105 × − — 48% +, against 50% predicted whatever the far side is asked
    What the far side did
    changed nothing here: the near side is a fair toss either way
  5. P-905 — Measuring one side sends something instantly to the other

    The claim that turns entanglement into a communications product.

    Experiment
    None. This one follows from the theory, not from trials.
  6. P-906 — These runs prove no local hidden-variable theory can explain the pair

    The strongest thing anyone could hope to conclude from an apparatus like this.

    Experiment
    None. It needs a real Bell test, or a real device.
  7. P-907 — Entangled pairs in a data centre stay correlated for hours

    A claim about a real device in a real building.

    Experiment
    None. It needs a real Bell test, or a real device.

Trials can show or refuse what happens. They do not establish what the theory establishes, and they say nothing about a real device.

Learn more

Why this pattern exists

Put a left glove in one box and a right glove in another, send them to opposite ends of the country, and open one: you instantly know what is in the other. Nothing travelled, and nobody is surprised. That is a pre-agreed pair, and most explanations of entanglement are describing exactly this without noticing. The bench holds both kinds of pair at once. Ask both sides the Z question and they are identical: each pair agrees every single time. Ask both sides the X question instead, and the entangled pair still agrees every time while the pre-agreed pair drops to a coin toss. One bit decided in advance cannot be right in two different questions at once. And through all of it, each side on its own is a fair toss, whatever the far side is asked — which is why nothing here is a channel.

A source in the middle makes pairs and sends one side each way. Two kinds are on the bench: an entangled pair, and a pre-agreed pair carrying one bit decided when it was made. Both sides of each pair are measured in a basis you choose, and the tally counts how often the two sides agreed. Every graded experiment runs on a fixed seed.

  • Tell an entangled pair from a pre-agreed one by the only thing that separates them: agreement in more than one basis.
  • See why each side on its own carries no information, however strong the correlation between them.
  • Say what this bench establishes, what the theory establishes, and what would need a real Bell test.

The rule this lesson applies: A pre-agreed pair carries one bit, written when the pair was made. It agrees perfectly in the basis that bit is written in, and is a coin toss in the other — because there is nothing there to agree about. An entangled pair agrees in both, and that is the observation a single shared bit cannot reproduce. Be careful about what follows. This bench refuses one particular classical model; it is not a Bell test, which uses measurement angles this apparatus does not offer, and which is where the impossibility of local hidden variables is actually established. What does follow, from the theory rather than from any run, is no-signalling: each side's own outcomes are 50/50 whatever the far side is asked, so the correlation cannot carry a message, and entanglement is not a faster-than-light channel. Its engineering uses are elsewhere — key distribution, where the correlation is used with a classical channel alongside it, and error correction, where entanglement across physical qubits is what makes a logical one. This page computes the statistics the standard model predicts; it models no noise, no decoherence and no hardware.