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Finite wire permutations are unitary basis permutations

Statement

Let H0,…,Hn−1 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 σ of the factor positions, the map Pσ that reorders the factors is a bijective linear isometry from H0⊗⋯⊗Hn−1 to Hσ(0)⊗⋯⊗Hσ(n−1). When source and target are identified as the same register, Pσ 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 σ of the factor positions.

[F1]

Pσ 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).

[F2]

The ordered product vectors form an orthonormal basis, including the empty and zero-dimensional cases (The product basis is orthonormal and tensor dimensions multiply).

[F3]

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

1.1givenF1algebra

By [F1], Pσ 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 Pσ−1. The empty list gives the identity on C.

2.1step 1.1F2algebra

Write an arbitrary vector as ∑αcαeα in the orthonormal product basis from [F2]. Its squared norm is ∑α∣cα∣2. The map permutes that basis, so its image has the same coefficients in a permuted orthonormal basis and the same squared norm. Thus Pσ 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.

3.1step 1.1step 2.1F3∎

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].

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