Quantum Lab
Quantum Lab

An interactive quantum mechanics learning platform and cryostat wiring co-design tool. From plain-language intuition to formal mathematics.

contact@quantumcircuitsimulator.com

Product

  • Circuit Lab
  • Learn
  • Hardware Studio
  • Pricing

Legal

  • Privacy Policy
  • Terms of Service

© 2026 Quantum Lab. All rights reserved.

This site, including its original quantum simulations, cryostat reference systems, 3D models, and interface design, contains protected proprietary material.

Home/Quantum Physics/Lessons/Measurement
M

Measurement

MeasurementSingle-qubitcollapse

Collapses quantum state to a classical result.

Intuition

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.

Matrix representation
∣ψ⟩→∣k⟩ with pk​=∣⟨k∣ψ⟩∣2
Action on states
α∣0⟩+β∣1⟩→0 (p=∣α∣2) or 1 (p=∣β∣2)
Bloch sphere
superposition
→
|0⟩ or |1⟩
Circuit
q0HM
State comparison
Before Measure
superposition
|0\u27E9
85%
|1\u27E9
15%
Bloch: (0.71, 0.00, 0.71)
→
After Measure
|0⟩ or |1⟩
|0\u27E9
100%
|1\u27E9
0%
Bloch: (0.00, 0.00, 1.00)
Precise explanation

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.

Observable effect

One outcome is sampled from the probability distribution.

Hidden effect

The full superposition information is irreversibly discarded.

Bloch sphere

Projects the Bloch vector to the nearest pole. The sphere collapses to |0⟩ (north) or |1⟩ (south).

Worked example

Measuring a superposition

  1. 1Start with H|0⟩ = (|0⟩ + |1⟩)/√2.
  2. 2The amplitudes are α = β = 1/√2.
  3. 3Probability of 0: |α|² = 1/2. Probability of 1: |β|² = 1/2.
  4. 4Measurement returns 0 or 1, each with 50% probability.
  5. 5If you got 0, the post-measurement state is |0⟩. The superposition is gone.
  6. 6Repeating the preparation and measurement many times confirms the 50/50 statistics.
Common use cases
  • Extracting classical results from quantum computation
  • Mid-circuit measurement for error correction syndrome extraction
  • Teleportation protocols (measuring in the Bell basis)
  • Adaptive circuits where later gates depend on earlier measurement results
Relation to other gates
  • Measurement is not a unitary gate — it is irreversible
  • Measuring in a different basis = apply a basis-change gate then measure computationally
  • Deferred measurement principle: measurements can be postponed to the end of a circuit without changing the outcome statistics
  • Measuring one qubit of an entangled pair collapses the other
Common misconception

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).

Why this gate matters

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.

Test your understanding

After measuring a qubit and getting result 0, you measure it again immediately. What do you get?

Quick reference →↗ Griffiths and Schroeter, Introduction to Quantum Mechanics↗ Nielsen and Chuang, Quantum Computation and Quantum Information
←
Previous
Controlled-Phase
← Back to all lessons