Quantum Physics
Quantum Entanglement
Two particles linked so measuring one instantly determines the other — at any distance
Quantum entanglement — two or more particles can be in a joint state where measurement of one instantly determines the other's state, regardless of distance. Einstein called it "spooky action at a distance" (1935 EPR paper). Bell's theorem (1964) plus experiments (Aspect 1982, Zeilinger 2022 Nobel) confirm: entangled particles violate "local realism." Foundation of quantum cryptography, teleportation, quantum computing.
- EPR paperEinstein, Podolsky, Rosen (1935) — "spooky"
- Bell's theorem1964 — entanglement violates local realism
- Bell test experimentsAspect 1982; Zeilinger Nobel 2022
- Bell state|Ψ⁻⟩ = (|01⟩ - |10⟩) / √2
- Used inQuantum cryptography (BB84), teleportation, computing
- No FTL communicationCorrelations can't carry classical information
Interactive visualization
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Entangled states
A two-particle system in entangled state can't be written as product of individual states:
|Ψ⟩ = (|0⟩_A · |1⟩_B − |1⟩_A · |0⟩_B) / √2 (singlet state)
Both particles are in superposition; measurement of A's spin instantly determines B's (anti-correlated). Distance doesn't matter.
Bell states
| Bell state | Form | Properties |
|---|---|---|
| |Φ⁺⟩ | (|00⟩ + |11⟩) / √2 | Same (correlated) |
| |Φ⁻⟩ | (|00⟩ − |11⟩) / √2 | Same with phase |
| |Ψ⁺⟩ | (|01⟩ + |10⟩) / √2 | Anti-correlated |
| |Ψ⁻⟩ (singlet) | (|01⟩ − |10⟩) / √2 | Maximally anti-correlated |
These four are a complete basis for two-qubit entangled states.
Bell test experiments
Standard setup — entangled pair generated centrally; sent to Alice and Bob far apart. Each chooses random measurement direction. Correlations measured.
Bell inequality (CHSH form): for any local hidden-variable theory, |S| ≤ 2, where S is a specific combination of correlation measurements.
Quantum mechanics predicts |S| = 2√2 ≈ 2.83 for entangled states.
Experiments (Aspect 1982, Hensen 2015 loophole-free, etc.) consistently observe S ≈ 2.7-2.8, violating Bell's inequality — confirming quantum non-locality.
JavaScript — entanglement basics
// Two-qubit Bell state correlation simulation
function bellState_singlet() {
// Singlet: random outcomes, anti-correlated when measured in same basis
const outcome_A = Math.random() < 0.5 ? 0 : 1;
const outcome_B = 1 - outcome_A; // anti-correlated
return [outcome_A, outcome_B];
}
// Confirm anti-correlation
let same = 0, opposite = 0;
for (let i = 0; i < 10000; i++) {
const [a, b] = bellState_singlet();
if (a === b) same++;
else opposite++;
}
console.log(`Same: ${same}, Opposite: ${opposite}`); // 0, 10000 (perfect anti-correlation)
// CHSH inequality: classical hidden vars give ≤ 2; quantum can give up to 2√2 ≈ 2.83
function bellCorrelation(theta_A, theta_B) {
// For singlet, P(same) = sin²((θ_A - θ_B)/2)
// E(A,B) = -cos(θ_A - θ_B)
return -Math.cos(theta_A - theta_B);
}
// Compute S = E(a,b) - E(a,b') + E(a',b) + E(a',b')
function chshValue(theta_a, theta_aPrime, theta_b, theta_bPrime) {
return bellCorrelation(theta_a, theta_b)
- bellCorrelation(theta_a, theta_bPrime)
+ bellCorrelation(theta_aPrime, theta_b)
+ bellCorrelation(theta_aPrime, theta_bPrime);
}
// Optimal angles for max violation
const S = chshValue(0, Math.PI/2, Math.PI/4, 3*Math.PI/4);
console.log(`CHSH S = ${S.toFixed(4)}`); // 2.828 = 2√2
console.log(`Classical bound: 2; Quantum prediction: 2√2 = ${(2*Math.sqrt(2)).toFixed(4)}`);
// Quantum teleportation — high level (skip math)
// 1. Alice & Bob share entangled pair
// 2. Alice has qubit |Ψ⟩ to teleport
// 3. Alice does Bell measurement on her two qubits → 2 classical bits
// 4. Sends 2 bits to Bob
// 5. Bob applies one of 4 operations based on Alice's bits → his qubit becomes |Ψ⟩
// Result: state |Ψ⟩ moved from Alice to Bob, but classical comm needed.
// EPR paradox illustration
function eprPair(direction_A_deg, direction_B_deg) {
// Particles measured along chosen directions
const angle_diff = (direction_A_deg - direction_B_deg) * Math.PI / 180;
// P(same outcome) for entangled pair = sin²(angle_diff/2)
const P_same = Math.sin(angle_diff / 2) ** 2;
return P_same;
}
console.log(`Same direction: P_same = ${eprPair(0, 0)}`); // 0 (always opposite)
console.log(`Perpendicular: P_same = ${eprPair(0, 90)}`); // 0.5 (random)
console.log(`Same again: P_same = ${eprPair(45, 45)}`); // 0
Where entanglement matters
- Quantum cryptography. BB84 (Bennett-Brassard) and Ekert protocols use entanglement for unconditionally secure key distribution.
- Quantum computing. Quantum gates entangle qubits — essential for quantum algorithms (Shor's, Grover's).
- Quantum teleportation. State transfer via entangled pairs + classical bits.
- Quantum networks. Future internet of entangled nodes for secure communication.
- Foundations. Bell tests rule out local hidden variables; Zeilinger 2022 Nobel for "loophole-free" tests.
- Quantum sensing. Entanglement-enhanced metrology beats classical limits.
- Astrophysics. Hawking radiation entangles photons across event horizon (information paradox).
Common mistakes
- Believing entanglement transmits information FTL. NO. Each particle's outcome is random. Correlations only seen by combining results, which needs classical communication.
- Treating it as classical correlation. Classical correlations satisfy Bell inequalities. Entangled states violate them — different physics.
- Thinking "particles know" each other's state. Anthropomorphism. Quantum mechanics predicts correlations; "knowing" implies hidden variables which are ruled out.
- Confusing entanglement with superposition. Superposition — single particle in multiple states. Entanglement — multi-particle state where they share quantum information.
- Believing teleportation transfers matter. Just transfers the QUANTUM STATE. Original particle's state destroyed; recipient particle inherits info.
- Thinking Bell tests prove non-locality. They prove EITHER non-locality OR no realism (or both). Most physicists accept non-locality.
Frequently asked questions
What does "entangled" mean exactly?
Two particles share a joint quantum state that can't be factored. Their individual states are correlated — measurement of one IMMEDIATELY determines the other. The total state is described by ONE wave function for both, not separate ones. Examples — entangled photons in polarization (one vertical, other horizontal), entangled electrons in spin, etc.
Does entanglement allow faster-than-light communication?
NO. Each individual measurement gives a random outcome. The CORRELATIONS only become apparent when comparing results — which requires classical communication (limited by light speed). So entanglement doesn't transmit useful information faster than light. Special relativity preserved.
What is Bell's theorem?
John Bell (1964) — local hidden-variable theories cannot reproduce all quantum mechanics predictions. Specifically — they must satisfy Bell inequalities. Quantum predictions VIOLATE these. So nature is either non-local OR not realist (or both). Experiments since 1982 (Aspect) consistently violate Bell inequalities, supporting QM and ruling out local hidden variables.
How is entanglement created?
Particles need a common origin or interaction. Examples — (1) Photon pairs from spontaneous parametric down-conversion (one high-energy photon → two correlated lower-energy ones). (2) Atomic cascades (atom emits two photons in quick succession). (3) Cooper pairs (entangled electrons). (4) Direct interaction in coupled quantum systems.
How is entanglement used in quantum cryptography?
Ekert protocol (1991) — Alice and Bob share entangled photon pairs. Each measures their photon. Quantum correlations let them generate a secret key. ANY eavesdropping breaks the entanglement (measurement disturbs the state) — detectable. Provably secure based on physics, not computational hardness.
What's quantum teleportation?
Despite the name, NOT instantaneous transport of matter. Uses entanglement + classical bits to transfer the quantum STATE of a particle to another particle far away. Original particle's state is destroyed; recipient's particle inherits it. Demonstrated experimentally for photons, atoms. Key for quantum networks.
Why was Einstein bothered by entanglement?
It seemed to violate locality (no FTL influence) AND realism (objects have definite properties before measurement) — "elements of reality." Einstein expected nature to be local AND realist. Bell's theorem + experiments show: if QM is right, nature can't be both. EPR suspected QM was incomplete; Bell's experiments showed they were wrong.