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Finite wire permutations are unitary basis permutations
Statement
Let be a finite ordered family of finite-dimensional complex inner-product spaces, with the product bases of Ordered tensor registers, their inner product, and wire permutations. For a permutation of the factor positions, the map that reorders the factors is a bijective linear isometry from to . When source and target are identified as the same register, is a unitary operator in the sense of Linear isometries, and orthogonal or unitary operators on finite-dimensional inner product spaces.
Facts & Assumptions
Given: The ordered factors, their specified orthonormal bases, and a permutation of the factor positions.
sends a product-basis vector to the product-basis vector with the same factor labels in permuted order (Ordered tensor registers, their inner product, and wire permutations).
The ordered product vectors form an orthonormal basis, including the empty and zero-dimensional cases (The product basis is orthonormal and tensor dimensions multiply).
A linear isometry preserves vector norms; an invertible linear isometry of a finite-dimensional complex inner-product space to itself is unitary (Linear isometries, and orthogonal or unitary operators on finite-dimensional inner product spaces).
Proof
By [F1], sends each product-basis vector to exactly one product-basis vector, and the inverse permutation sends it back. Thus the basis assignment extends to a bijective linear map whose inverse is . The empty list gives the identity on .
Write an arbitrary vector as in the orthonormal product basis from [F2]. Its squared norm is . The map permutes that basis, so its image has the same coefficients in a permuted orthonormal basis and the same squared norm. Thus is a linear isometry. If a factor is zero-dimensional, both tensor spaces are zero and the unique map between them is bijective and isometric.
When the source and target are the same register, steps 1.1 and 2.1 give an invertible linear isometry of that space, hence a unitary operator by [F3].
Depends on
Used by
- Distance corrects unlocated errors and known erasures Corollary
- Complementary channels and coherent information Definition
- Finite quantum mutual, conditional, and conditional mutual information Definition
- Partial trace over the first tensor factor Definition
- Support and weight of an operator on a finite register Definition
- Strong subadditivity for a pure GHZ tripartite state Example
- Coherent information equals output entropy minus environment entropy Lemma
- Every finite extension is obtained from a purification by a channel Lemma
- Operator Norm Is Unchanged by Spectator Registers Lemma
- Operator support weight is invariant under wire permutation Lemma
- Channel Tensor Error Bound Theorem
- Data processing for finite quantum mutual information Theorem
- Nonnegativity of finite-dimensional quantum conditional mutual information Theorem
- Operator-norm error of QFT truncation Theorem
Dependency tree · two levels
16 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- John Watrous, The Theory of Quantum Information (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes, Appendix A.6 (standard reference, not scraped)