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12.3 Entangled and separable states

Source: Ideas from Computational Physics (Landau, Páez, Bordeianu), §12.3. Rewritten in original wording — no textbook Entangle.py dump. Continues 12.2b. Next: 12.3b.

A state built as a tensor product ∣ψA⟩⊗∣ψB⟩|\psi_A\rangle\otimes|\psi_B\rangle is separable. If two qubits interact so the joint state cannot be written as such a product, they are entangled. Distant spins in a total-spin-zero state remain correlated — measuring one constrains the other (Bell / Nobel 2022 context).

Separability test and Bell states​

For ∣Ψ⟩=[w,x,y,z]T|\Psi\rangle=[w,x,y,z]^T in the computational basis, the state is separable iff a simple amplitude condition holds. Bell states fail that test. Pick wz=xywz=xy and ∣β00⟩|\beta_{00}\rangle among lookalikes.

Product states satisfy the test identically. The four Bell states are the usual maximally entangled basis (sign and pairing variants of ∣00⟩±∣11⟩|00\rangle\pm|11\rangle and ∣01⟩±∣10⟩|01\rangle\pm|10\rangle).

Density matrix (preview)​

ρ=∑ipi ∣ψi⟩⟨ψi∣\rho=\sum_i p_i\,|\psi_i\rangle\langle\psi_i|

encodes ensembles of pure states (useful later for mixed / noisy QC).

Pauli gates (QC names)​

X=[0110], Y=[0−ii0], Z=[100−1].X=\begin{bmatrix}0&1\\1&0\end{bmatrix},\ Y=\begin{bmatrix}0&-i\\i&0\end{bmatrix},\ Z=\begin{bmatrix}1&0\\0&-1\end{bmatrix}.

Actions: X∣0⟩=∣1⟩X|0\rangle=|1\rangle, X∣1⟩=∣0⟩X|1\rangle=|0\rangle, Z∣0⟩=∣0⟩Z|0\rangle=|0\rangle, Z∣1⟩=−∣1⟩Z|1\rangle=-|1\rangle, etc.

Physics: two dipoles​

Dipole–dipole H∝σA⋅σB−3(σA⋅r^)(σB⋅r^)H\propto \boldsymbol\sigma_A\cdot\boldsymbol\sigma_B-3(\boldsymbol\sigma_A\cdot\hat r)(\boldsymbol\sigma_B\cdot\hat r). For r^=z^\hat r=\hat z,

H=μ2r3(X⊗X+Y⊗Y+Z⊗Z−3 Z⊗Z)=μ2r3[−200002200220000−2].H=\frac{\mu^2}{r^3}\bigl(X\otimes X+Y\otimes Y+Z\otimes Z-3\,Z\otimes Z\bigr) =\frac{\mu^2}{r^3} \begin{bmatrix}-2&0&0&0\\0&2&2&0\\0&2&2&0\\0&0&0&-2\end{bmatrix}.

Eigenvalues of H/(μ2/r3)H/(\mu^2/r^3): 4,0,−2,−24,0,-2,-2. Eigenvectors include Bell-like

∣01⟩+∣10⟩2,∣11⟩,∣00⟩,∣01⟩−∣10⟩2\frac{|01\rangle+|10\rangle}{\sqrt2},\quad |11\rangle,\quad |00\rangle,\quad \frac{|01\rangle-|10\rangle}{\sqrt2}

— some separable, some entangled. Labs lock matrix entries and the separability measure.

Takeaway​

IdeaTest / fact
Separablewz=xywz=xy for two-qubit amplitudes
BellMaximally entangled examples
X,Y,ZX,Y,ZSingle-qubit Pauli gates
DipolesHH in ⊗\otimes space; mixed eigenstates
Quiz

Entanglement

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Two-qubit [w,x,y,z] is separable iff…

Pick an answer to see if you are right.

Next: 12.3b Entanglement labs.