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FUNDAMENTALS / 07 / STATES

See the qubit: Bloch sphere

Connect a pure qubit's direction to measurement probabilities and relative phase.

Intuition

The Bloch sphere is a map of single-qubit states, not the physical shape of a qubit. The north pole represents |0⟩ and the south pole |1⟩. Equatorial pure states have equal computational-basis probabilities.

Change θ to move between the poles. Change φ around the equator: the amplitudes' relative phase changes while the probabilities remain 50/50. Set θ to π/2 and φ to 0 for |+⟩. The sphere represents the same state described by its statevector.

The mathematics

∣ψ⟩=cos⁡(θ/2)∣0⟩+eiϕsin⁡(θ/2)∣1⟩,P(1)=sin⁡2(θ/2)|\psi\rangle=\cos(\theta/2)|0\rangle+e^{i\phi}\sin(\theta/2)|1\rangle,\quad P(1)=\sin^2(\theta/2)
Look a little deeper

This expression chooses a global-phase convention. At a pole, φ does not distinguish physical states. Pure states lie on the sphere; mixed states can lie inside it. The local state of an entangled qubit need not lie on the surface.

See a single qubit

The interactive state explorer requires the quantum simulator, which is not hosted in this preview.

Use it

Explore θ and φ above, then prepare |+⟩ using one H in the circuit lab. Inspect Bloch and Statevector.

This exercise uses the same server-side state and circuit checks as its linked practice problem.

Build your circuit

Click a gate to append it, or drag it onto a wire. CX uses the selected control; SWAP uses it as the second operand. Basis order: |qₙ … q₀⟩.

q0

Returned logical circuit · before transpilation · q0 on top

0 / 32 gates · terminal measurement of all qubits

Connect to code

qc = QuantumCircuit(1)
qc.h(0)

These operations go inside a circuit-building program. Practice problems provide a complete solve() template.

Solve the linked Qiskit problem →

Check your understanding

Changing only φ for a pure equatorial state changes…

First complete the circuit exercise successfully.