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Partial Trace: First Encounter

The partial trace removes one subsystem’s indices from a joint density operator, leaving the state that predicts all measurements on the remaining subsystem. We work through the basic rule here; partial trace gives the basis-independence proof, block-matrix methods, and algorithms.

Helpful background. Reduced states explains why this operation is useful; bra–ket notation makes the calculation short.

Tracing out BB means taking the ordinary trace only on its factor. Thus

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

The order in the overlap matters for complex vectors. Apply this rule linearly to all terms in ρAB\rho_{AB}. If the input is a density operator, the result is positive and has unit trace; no extra normalization factor is needed.

Expand the projector onto ∣Φ+⟩=(∣00⟩+∣11⟩)/2|\Phi^+\rangle=(|00\rangle+|11\rangle)/\sqrt2. Its first diagonal term reduces as

Tr⁡B(∣00⟩⟨00∣)=∣0⟩⟨0∣⟨0∣0⟩=∣0⟩⟨0∣.\operatorname{Tr}_B(|00\rangle\langle00|) =|0\rangle\langle0|\langle0|0\rangle =|0\rangle\langle0|.

One cross term gives

Tr⁡B(∣00⟩⟨11∣)=∣0⟩⟨1∣⟨1∣0⟩=0.\operatorname{Tr}_B(|00\rangle\langle11|) =|0\rangle\langle1|\langle1|0\rangle=0.

The other two terms give ∣1⟩⟨1∣|1\rangle\langle1| and zero. Retaining the common factor 1/21/2,

ρA=12(∣0⟩⟨0∣+∣1⟩⟨1∣)=I/2.\rho_A=\tfrac12(|0\rangle\langle0|+|1\rangle\langle1|)=I/2.

The cross terms vanish because the two BB states are orthogonal. Partial trace does not delete every off-diagonal term indiscriminately.

For the product state ∣+⟩A∣0⟩B|+\rangle_A|0\rangle_B, what is ρA\rho_A? Does its ∣0⟩⟨1∣|0\rangle\langle1| coherence survive?

Solution

The joint density operator is ∣+⟩⟨+∣⊗∣0⟩⟨0∣|+\rangle\langle+|\otimes|0\rangle\langle0|. Its partial trace is ∣+⟩⟨+∣|+\rangle\langle+|, because Tr⁡∣0⟩⟨0∣=1\operatorname{Tr}|0\rangle\langle0|=1. The AA coherence survives: both terms carry the same BB ket, whose overlap is one, unlike the Bell example.

  • M. A. Nielsen and I. L. Chuang, Quantum Computation and Quantum Information, 10th anniversary ed., Cambridge University Press, 2010, sec. 2.4.3.
  • J. Watrous, The Theory of Quantum Information, Cambridge University Press, 2018, ch. 2. Author’s manuscript.