Collapses quantum state to a classical result.
Measurement is where quantum meets classical. Before measurement, a qubit exists in a superposition of possibilities described by amplitudes. Measurement forces a definite outcome: 0 or 1. The probability of each outcome is determined by the Born rule — you square the magnitude of the amplitude. After measurement, the qubit is in the state corresponding to the result you observed. All the superposition information is gone. This irreversibility is what makes measurement fundamentally different from any gate.
Measurement in the computational basis projects the state onto |0⟩ or |1⟩. For state α|0⟩ + β|1⟩, the probability of outcome 0 is |α|² and outcome 1 is |β|² (Born rule). The post-measurement state is the eigenstate corresponding to the observed outcome. Measurement is not unitary — it is irreversible and destroys coherence. In multi-qubit systems, measuring one qubit can collapse entanglement, projecting the other qubits into a definite state.
One outcome is sampled from the probability distribution.
The full superposition information is irreversibly discarded.
Projects the Bloch vector to the nearest pole. The sphere collapses to |0⟩ (north) or |1⟩ (south).
Measurement does not reveal a pre-existing hidden value. The outcome is genuinely probabilistic according to the Born rule. The state before measurement is the complete description — there is no deeper hidden variable (in standard quantum mechanics).
Measurement is the only way to get information out of a quantum computer. Everything else — superposition, entanglement, interference — is preparation for the moment when measurement converts quantum amplitudes into classical data.
After measuring a qubit and getting result 0, you measure it again immediately. What do you get?