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Bell-State Entanglement Visualizer
Quantumon followed by . Toggling the initialization ports selects which Bell pair is prepared; amplitudes and the correlation index are derived, and a measure button accumulates real Born-rule shots.
6 components · 5 connections · state-vector + Born sampler
the ahaMeasure one qubit and you instantly know the other — not because a signal raced across, but because they were never really two things.
why it works
Start with , apply to the first qubit, then a CNOT, and you reach . Notice what is missing: there is no and no . The two qubits have no state of their own — only the pair has a state. A skeptic says "they were secretly agreed in advance," like two gloves in sealed boxes. Quantum mechanics answers with the CHSH test: local hidden agreements can never push the correlation witness above , yet this state reaches . Watching climb past is watching local realism fail in front of you.
governing model
structural inventory
- qubit register line
- Hadamard gate
- CNOT control/target
- measurement ports
boundaries
- Bell states
- amplitudes
- CHSH witness
fault relay CNOT entangler offline
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Prepare and measure ×64 repeatedly.
Only and ever appear, roughly half each — perfectly correlated outcomes from a state with no definite value beforehand. -
Run the CHSH witness.
The empirical settles near . Any glove-in-a-box explanation is capped at ; you are past it. That gap is the whole of quantum non-locality. -
Take the entangler offline.
Skip the CNOT and you get a plain product state — the correlation collapses back below . No entanglement, no violation.
causal signal trace paused
Prepare Both qubits begin separable and deterministic.
step 1 / 4 Prepare |00⟩
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