Training Quantum Physics Quantum States and the Bloch Sphere
2 / 3

Quantum States and the Bloch Sphere

15 min Quantum Physics

Quantum States and the Bloch Sphere

A qubit — the quantum analogue of a classical bit — can be in a superposition of $|0\rangle$ and $|1\rangle$. The most general single-qubit pure state is:

$$|\psi\rangle = \cos\!\frac{\theta}{2}|0\rangle + e^{i\phi}\sin\!\frac{\theta}{2}|1\rangle$$

where $\theta \in [0, \pi]$ is the polar angle and $\phi \in [0, 2\pi)$ is the azimuthal phase. This state corresponds to a unique point on the Bloch sphere — a unit sphere whose north pole is $|0\rangle$ and south pole is $|1\rangle$.

Expectation Values

For the state above, the spin expectation values are:

$$\langle\hat{S}_x\rangle = \frac{\hbar}{2}\sin\theta\cos\phi, \qquad \langle\hat{S}_y\rangle = \frac{\hbar}{2}\sin\theta\sin\phi, \qquad \langle\hat{S}_z\rangle = \frac{\hbar}{2}\cos\theta$$

The Bloch vector $(\sin\theta\cos\phi,\, \sin\theta\sin\phi,\, \cos\theta)$ points from the center of the sphere to the state.

Interactive Explorer: Bloch Sphere
⟨Sₓ⟩/ħ = 0.5000
⟨Sᵧ⟩/ħ = 0.0000
⟨Sᵨ⟩/ħ = 0.0000
P(↑) = 50.0 %

Quantum Gates

Quantum gates are unitary operations that rotate the Bloch vector. The six Pauli-based gates are:

GateMatrixEffect
H (Hadamard)$\frac{1}{\sqrt{2}}\begin{pmatrix}1&1\\1&-1\end{pmatrix}$$|0\rangle\leftrightarrow|+\rangle$
X (NOT)$\begin{pmatrix}0&1\\1&0\end{pmatrix}$Bit flip: $|0\rangle\leftrightarrow|1\rangle$
Z$\begin{pmatrix}1&0\\0&-1\end{pmatrix}$Phase flip
S$\begin{pmatrix}1&0\\0&i\end{pmatrix}$$\pi/2$ phase rotation
T$\begin{pmatrix}1&0\\0&e^{i\pi/4}\end{pmatrix}$$\pi/4$ phase rotation
R_z(\theta)$\begin{pmatrix}e^{-i\theta/2}&0\\0&e^{i\theta/2}\end{pmatrix}$Z-axis rotation
Interactive Explorer: Qubit Gate Playground
Output θ = 0.0000 rad
Output ϕ = 0.0000 rad
P(↑) = 50.0 %

Density Matrix and Mixed States

When a qubit interacts with its environment (decoherence), it transitions from a pure state to a mixed state, described by a $2\times2$ density matrix $\rho$. The key quantities are:

  • Purity: $\text{Tr}(\rho^2) = \frac{1+r^2}{2}$ where $r = |\mathbf{r}|$ is the Bloch vector length (1 = pure, 0.5 = maximally mixed)
  • Von Neumann entropy: $S = -\text{Tr}(\rho \log_2 \rho)$ (0 for pure, 1 bit for maximally mixed)
  • Coherence: $|\rho_{01}|$ — off-diagonal magnitude
Interactive Explorer: Density Matrix
Tr(ρ) = 1.000
Purity Tr(ρ²) = 1.0000
Entropy S = 0.0000 bits
Coherence |ρ₀₁| = 0.5000