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Two particles · one quantum state

Quantum Entanglement

When two particles become entangled, neither has a definite value of its own. Measure one, and you instantly know what the other will show, however far apart they are. Einstein called it “spooky action at a distance.” Experiments say it is real.

|Ψ⁻⟩ = (|↑↓⟩ − |↓↑⟩) / √2the singlet state
01 · The idea

What is entanglement?

In quantum mechanics, a particle's properties such as spin or polarisation are described by a state that can hold several possibilities at once. When two particles interact in the right way, they can end up sharing a single state. From then on you cannot describe either particle on its own. Only the pair has a description.

Take the singlet state above. Each electron, measured alone, shows spin up or down at random, 50/50. Yet if you measure both along the same direction, the results are always opposite. Measure along different directions, and the agreement changes smoothly with the angle between them, following a cosine curve.

That cosine curve is the fingerprint. No theory in which each particle secretly carries pre-set answers can reproduce it. This was proved by John Bell in 1964 and confirmed in the lab many times since.

The glove analogy, and where it breaks

Put a left and a right glove into two boxes and send them apart. Open one, see “left”, and you know the other is “right”. That is ordinary correlation: the answer was fixed all along.

Why quantum is stranger

Entangled particles let you choose which question to ask: any angle you like. Pre-set answers cannot match the quantum statistics for every possible pair of angles at once. The gloves had no left or right until someone looked.

But no messages travel

Each side alone sees pure randomness. The correlation only appears when the two lists of results are compared, which needs an ordinary, light-speed channel. Entanglement cannot send a signal faster than light.

02 · Interactive lab

Measure entangled pairs yourself

A source creates electron pairs in the singlet state and sends one to Alice (green) and one to Bob (pink). Set each detector's angle, then measure. Your results are plotted against the quantum prediction and the best any “pre-set answers” model can do.

Source and detectors

Same angle → always opposite. Try 0° and 180° for always equal.

Pairs at this angle0
Results opposite–
Quantum predicts–

Correlation vs angle difference

Correlation E = (agree − disagree) / total

Quantum: −cos θ Best pre-set answers model Your measurements

Run a Bell test (CHSH)

Four angle settings, 4,000 pairs. Any pre-set answers model gives |S| ≤ 2. Quantum mechanics allows up to 2√2 ≈ 2.83.

02 · classical limit2.83

Press the button to collect data.

03 · Timeline

From paradox to Nobel Prize

  1. 1935

    The EPR paradox

    Einstein, Podolsky and Rosen argue that quantum mechanics must be incomplete: if measuring one particle fixes the other's result, the values must have existed in advance.

  2. 1935

    Schrödinger names it

    Erwin Schrödinger coins the word “entanglement” (Verschränkung) and calls it the characteristic trait of quantum mechanics.

  3. 1964

    Bell's theorem

    John Stewart Bell shows the question can be tested. Local hidden-variable theories obey an inequality that quantum mechanics violates.

  4. 1972

    First Bell test

    Stuart Freedman and John Clauser measure entangled photons from calcium atoms. The results side with quantum mechanics.

  5. 1982

    Switching detectors in flight

    Alain Aspect's team in Paris changes measurement settings while the photons travel, closing a key loophole.

  6. 1997

    Quantum teleportation

    Anton Zeilinger's group in Innsbruck teleports the quantum state of a photon using entanglement plus a classical message.

  7. 2015

    Loophole-free tests

    Teams in Delft, Vienna and at NIST close the main loopholes at the same time. Local realism is ruled out.

  8. 2017

    Entanglement from space

    China's Micius satellite distributes entangled photons to ground stations about 1,200 km apart.

  9. 2022

    Nobel Prize in Physics

    Aspect, Clauser and Zeilinger share the prize “for experiments with entangled photons, establishing the violation of Bell inequalities and pioneering quantum information science.”

04 · Applications

What entanglement is good for

Security

Quantum cryptography

Protocols such as E91 (Ekert, 1991) build secret keys from entangled pairs. An eavesdropper disturbs the correlations and shows up in the Bell statistics.

Communication

Quantum teleportation

Moves a quantum state from one place to another using a shared entangled pair and two classical bits. Matter does not travel, and nothing goes faster than light.

Computing

Quantum computers

Entangling gates link qubits so a computer can work with correlations no classical machine can store efficiently. Without entanglement there is no quantum speed-up.

Measurement

Quantum sensing

Entangled atoms and photons can beat the standard noise limit, sharpening atomic clocks, interferometers and gravitational-wave detectors.

05 · Clearing things up

Myths and facts

MythEntanglement lets you send messages faster than light.
FactThe no-communication theorem forbids it. Each side's results look random until compared over a normal channel.
MythThe particles were just like the gloves: the answers were fixed from the start.
FactBell tests rule out every local pre-set-answer model. The lab above shows the gap: |S| above 2.
MythOnce entangled, always entangled.
FactEntanglement is fragile. Stray interactions with the environment (decoherence) destroy it, which is why quantum hardware is kept so cold and isolated.
MythIt only works for tiny distances.
FactEntanglement has been shared over more than 1,000 km via satellite, and the correlations do not weaken with distance.
06 · Key terms

A short glossary

Superposition
A quantum system holding a combination of possible states until it is measured.
Qubit
The quantum version of a bit, which can be 0, 1, or a superposition of both.
Singlet state
The two-particle state |Ψ⁻⟩ with total spin zero. Measured along the same axis, the two spins always come out opposite.
Bell inequality
A limit on correlations that every local hidden-variable theory must respect. The CHSH form says |S| ≤ 2.
Tsirelson's bound
The largest value quantum mechanics allows for S: 2√2 ≈ 2.83.
Decoherence
Loss of quantum behaviour as a system becomes entangled with its noisy surroundings.