Curriculum / Quantum Foundations / Rotation Matrices

Lesson 10 of 17ReadingFree+75 XP

Rotation Matrices

Understand how single-qubit gates rotate states on the Bloch sphere.

Rotation Matrices on the Bloch Sphere

Every single-qubit gate is a rotation on the Bloch sphere. Understanding this gives you the ability to construct any gate from first principles.

The Three Rotation Axes

Rotation about X-axis by angle θ:

qc.rx(theta, qubit)   # theta in radians

Rotation about Y-axis by angle θ:

qc.ry(theta, qubit)

Rotation about Z-axis by angle θ:

qc.rz(theta, qubit)

Familiar Gates as Rotations

GateRotation
XRX(π)
YRY(π)
ZRZ(π)
HRZ(π) then RY(π/2)
SRZ(π/2)
TRZ(π/4)

The H row is a circuit-order sequence: apply RZ(π) first, then RY(π/2). As a matrix product that is RY(π/2)·RZ(π), which equals H up to a global phase: . The Pauli, S, and T rows also hold up to a global phase, since RZ uses the symmetric convention.

The Y gate in that table deserves a word, since this track has so far leaned on X and Z. Y is the third Pauli gate: a combined bit flip and phase flip (Y = iXZ), and it rotates about the Y axis exactly as X and Z rotate about theirs.

Key Insight

Any single-qubit unitary can be decomposed as:

for some angles α, β, γ and a global phase δ. This ZYZ decomposition is how quantum compilers translate arbitrary unitary matrices into physical gates.

Commutation and Non-Commutation

  • RX and RY do not commute: RX(θ)RY(φ) ≠ RY(φ)RX(θ) in general
  • RZ and RZ do commute: applying two Z-rotations is equivalent to one combined rotation
  • This is why gate ordering matters in quantum circuits!

How this lesson works

A guided reading lesson with interactive knowledge checks. Concepts are explained step by step with circuit diagrams and runnable examples, and you confirm understanding before moving on.

Part of: Quantum Foundations

Learn the basics: qubits, gates, superposition, and measurement.

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