Qubit
A qubit (quantum bit) is the fundamental unit of quantum information, capable of existing in a superposition of the classical states 0 and 1.
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What it means
Unlike a classical bit that must be either 0 or 1, a qubit's state is a linear combination (superposition) of both basis states, described by the state vector |ψ⟩ = α|0⟩ + β|1⟩, where α and β are complex probability amplitudes satisfying |α|² + |β|² = 1.The amplitudes can interfere — adding up or cancelling — and quantum algorithms are built on arranging that interference; a single measurement, however, still yields only one classical bit.Physical implementations include superconducting circuits, trapped ions, photon polarization, and electron spin.Upon measurement, the qubit collapses to either |0⟩ or |1⟩ with probabilities |α|² and |β|² respectively.Everyday analogy
Common misconceptions
- A qubit is NOT simply 0 and 1 at the same time — it exists in a specific quantum state described by complex amplitudes that determine measurement probabilities.
- A qubit does NOT store infinite information — upon measurement, you only get a single classical bit of information (0 or 1).
- A qubit is NOT a spinning coin that is secretly heads or tails. A coin always has a definite hidden side, and classical probabilities can only add up; a qubit's amplitudes can cancel (interference), which no hidden-coin picture can reproduce.
Key takeaways
- A qubit is described by two complex amplitudes α and β with the normalization constraint |α|² + |β|² = 1.
- Measurement collapses the qubit to a definite classical state, yielding 0 with probability |α|² or 1 with probability |β|².
- Qubits are the building blocks of all quantum computation and quantum information protocols.
Check your understanding
A qubit is in the state |ψ⟩ = (1/√2)|0⟩ + (1/√2)|1⟩. What is the probability of measuring |0⟩?
- A.0
- B.1/4
- C.1/2
- D.1
Show the answer
Answer: C. 1/2
Why: The probability of measuring |0⟩ is |α|² = |1/√2|² = 1/2 = 50%.
Builds toward
Primary source: Schumacher, Quantum coding, Phys. Rev. A 51, 2738 (1995), doi:10.1103/PhysRevA.51.2738
Term and formalism per Schumacher 1995; state-vector treatment per Nielsen & Chuang (2010), doi:10.1017/CBO9780511976667.
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