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A state you can explore.

Interactive / 01
|0⟩|1⟩50.0%50.0%

Measurement probabilities

For this real-amplitude family, |ψ⟩ = cos(θ/2)|0⟩ + sin(θ/2)|1⟩. Change θ to redistribute the measurement probabilities.

A measurement returns one outcome. The bars show probabilities, not two physical objects.

Your objective

Grasp how superposition enables a qubit to process multiple states at once and understand the mathematical representation of multiple‑qubit superpositions.

2.1 Single‑Qubit Superposition

Any single qubit state is α|0⟩ + β|1⟩ with normalization condition.

|ψ⟩ = α|0⟩ + β|1⟩, |α|²+|β|²=1
Concept notation / 01

2.2 Multi‑Qubit States

The state of n qubits lives in a 2ⁿ‑dimensional Hilbert space, described by the tensor product of individual qubit states.

n‑qubit state = |ψ₁⟩ ⊗ |ψ₂⟩ ⊗ … ⊗ |ψₙ⟩
Concept notation / 02

2.3 Measurement Probabilities

When measuring a multi‑qubit state, the probability of each basis outcome is the squared magnitude of its amplitude.

Probability of |101⟩ = |α₁₀₁|²
Concept notation / 03

Put it together

Worked example

Create a 2‑qubit superposition (|00⟩ + |11⟩)/√2. This is an entangled Bell state (see Module 4).

Key takeaways

• The state space grows exponentially with qubit count. • Tensor products combine individual qubit states. • Measurement extracts a single basis outcome probabilistically.

Knowledge check / 3 questions

Test your understanding.

1. The state of two entangled qubits is most naturally described as:
2. If a 3‑qubit system is in an equal superposition of all 8 basis states, what is the probability of measuring |101⟩?
3. Which operation creates a superposition from the |0⟩ state?
0 of 3 answered