Skip to content

Partial Trace: First Encounter

Canonical treatment: Partial Trace maintains the basis-independence proof, matrix rules, algorithms, exercises, and references.

This bridge is intentionally limited to the minimal partial-trace calculation needed before the full reduced-state treatment.

For a bipartite operator, tracing out BB leaves an operator on AA:

ρA=Tr⁡BρAB.\rho_A=\operatorname{Tr}_B\rho_{AB}.

On product dyads,

Tr⁡B ⁣(∣a⟩⟨a′∣⊗∣b⟩⟨b′∣)=⟨b′∣b⟩ ∣a⟩⟨a′∣.\operatorname{Tr}_B\!\left( \lvert a\rangle\langle a'\rvert\otimes \lvert b\rangle\langle b'\rvert \right) = \langle b'\vert b\rangle\, \lvert a\rangle\langle a'\rvert.

Apply this rule term by term and check that the result is Hermitian, positive, and has unit trace when the input is a density operator.

For ∣Φ+⟩=(∣00⟩+∣11⟩)/2\lvert\Phi^+\rangle=(\lvert00\rangle+\lvert11\rangle)/\sqrt2, the cross terms vanish under Tr⁡B\operatorname{Tr}_B and

ρA=12(∣0⟩⟨0∣+∣1⟩⟨1∣)=I2.\rho_A=\frac12\left(\lvert0\rangle\langle0\rvert+\lvert1\rangle\langle1\rvert\right)=\frac{I}{2}.

The canonical page develops why this answer is basis independent and how to compute it from blocks, indices, or software.