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Quantum Information and Entanglement

Manual: General · Subject: Quantum Information

Qubits, quantum gates, entanglement, and cryptography

Quantum Computation and Information

Qubits and Quantum Gates

A qubit: ∣ψ⟩=α∣0⟩+β∣1⟩|\psi\rangle = \alpha|0\rangle + \beta|1\rangle with ∣α∣2+∣β∣2=1|\alpha|^2 + |\beta|^2 = 1. Unlike a classical bit, the qubit can exist in superposition. nn qubits can represent 2n2^n states simultaneously.

Single-qubit gates (unitary matrices): Hadamard H=12(111−1)H = \frac{1}{\sqrt{2}}\begin{pmatrix}1&1\\1&-1\end{pmatrix}, Pauli operators X,Y,ZX, Y, Z.<br>Two-qubit CNOT gate entangles qubits.

Entanglement and Bell States

Bell states are maximally entangled two-qubit states:<br>∣Φ+⟩=12(∣00⟩+∣11⟩)|\Phi^+\rangle = \frac{1}{\sqrt{2}}(|00\rangle + |11\rangle)<br>Measuring one qubit instantly determines the other, regardless of distance. This violates local hidden variable theories (Bell's theorem).

Applications: quantum teleportation, superdense coding, quantum key distribution (BB84, E91).

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No-Cloning Theorem

An unknown quantum state cannot be perfectly copied. This is a theorem (not just a limitation of technology) that underpins quantum cryptography security — eavesdropping disturbs the quantum state and is detectable.

Applying a Hadamard gate to ∣0⟩|0\rangle produces:

Bell's theorem rules out:

Why is quantum computing potentially faster for certain problems? Use Shor's algorithm as an example.