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Entanglement in quantum mechanics<br />

• A quantum system is in an entangled state if performing a localised measurement (in<br />

sp<strong>ac</strong>e and time) may instantaneously affect local measurements far away.<br />

A typical example: a pair <strong>of</strong> opposite-spin electrons:<br />

|ψ〉 = 1 √<br />

2<br />

(|↑ ↓ 〉 + |↓ ↑ 〉) ,<br />

〈Â〉 = 〈ψ|Â|ψ〉<br />

• What is special: Bell’s inequality says that this cannot be described by local variables.<br />

• A situation that looks similar to |ψ〉 but without <strong>entanglement</strong> is a f<strong>ac</strong>torizable state:<br />

| ˆψ〉 = 1 2 (|↑ ↓ 〉 + |↓ ↑ 〉 + |↑ ↑ 〉 + |↓ ↓ 〉) = 1 2<br />

(|↑ 〉 + |↓ 〉) ⊗ (|↑ 〉 + |↓ 〉)<br />

• This is particular to pure states. Mixed states are described by density matrices<br />

ρ = ∑ α<br />

p α |ψ α 〉〈ψ α | ,<br />

〈Â〉 = Tr(ρÂ)<br />

(for pure states, ρ = |ψ〉〈ψ|; for finite temperature, ρ = e −H/kT ).

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