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Tensor maps preserve composition, identities, and adjoints
Statement
Let and be finite ordered families of linear maps between finite-dimensional complex inner-product spaces. Then
In the first formula, means . Here denotes the identity map . All adjoints use the repository pairing, linear in the first argument. The empty tensor-map identity is the identity map on .
Facts & Assumptions
Given: The finite ordered families of spaces and linear maps in the Statement.
The tensor map is the unique linear extension of its action on elementary tensors (Tensor products of finitely many linear maps).
Elementary tensors in the specified product basis form an orthonormal basis and span (The product basis is orthonormal and tensor dimensions multiply).
Every linear map between finite-dimensional inner-product spaces has a unique adjoint (Every linear map between finite-dimensional inner product spaces has a unique adjoint).
An adjoint satisfies (The adjoint is characterised by ).
Each root inner product is linear in the first argument and conjugate-linear in the second (Real and complex inner-product spaces and their induced length).
Every finite-dimensional real or complex inner-product space has an orthonormal basis, with the empty basis in dimension zero (Every finite-dimensional real or complex inner product space has an orthonormal basis).
Identity maps and compatible composites of linear maps are linear (Identity maps and composites of linear maps are linear).
Proof
By [F7], each is linear and the composite of the two tensor maps is linear, so [F1] applies to both sides. On an elementary tensor , the left side of the composition identity equals by [F1], which is the value of the right side. Since elementary tensors span by [F2], the two linear maps are equal.
By [F6], choose orthonormal bases for the finite factor spaces. For elementary tensors and , the product pairing in [F2] and the factor adjoint identities in [F4] give . The pairing is extended using the first-linear convention [F5].
Each factor identity and the identity on the tensor space are linear by [F7]. The tensor map fixes every elementary tensor by [F1]. The identity map does too; spanning in [F2] gives equality. If , both maps are the identity on .
Sesquilinearity and spanning extend the identity in step 1.2 to all . By existence and uniqueness in [F3] and the defining condition [F4], . For both sides are the identity on ; zero-dimensional factors are covered because the product bases may be empty.
Depends on
- Identity maps and composites of linear maps are linear
- Tensor products of finitely many linear maps
- Real and complex inner-product spaces and their induced length
- The adjoint $T^*:W\to V$ is characterised by $\langle Tv,w\rangle_W=\langle v,T^*w\rangle_V$
- Every linear map between finite-dimensional inner product spaces has a unique adjoint
- The product basis is orthonormal and tensor dimensions multiply
- Every finite-dimensional real or complex inner product space has an orthonormal basis
Used by
- Distance corrects unlocated errors and known erasures Corollary
- Partial trace over the first tensor factor Definition
- A local gate has a unique global wire embedding Lemma
- CNOT Pauli action Lemma
- Hadamard pauli action Lemma
- Phase gate pauli action Lemma
- Positive Marginals Imply Joint Support Lemma
- Preserving the logical marginal forces a gauge-only channel Lemma
- Symmetric Power Irreducible Lemma
- Trace distance is unchanged by a fixed tensor factor Lemma
- A finite Kraus sum is completely positive Theorem
- Binary Pauli quotient isomorphism Theorem
- Channel Composition Hybrid Bound Theorem
- Channel Diamond Norm One Theorem
- Channel Tensor Error Bound Theorem
- Diamond Norm Ancilla Dimension Bound Theorem
- Fidelity range equality and products Theorem
- Fingerprint swap-test error and communication cost Theorem
- Finite instruments can be coherently deferred Theorem
- Finite-dimensional channels compose and tensor Theorem
- Pauli product and adjoint Theorem
- Phase estimation on a superposition of eigenspaces Theorem
- Swap-test measurement and pure-state outcome law Theorem
- Symmetric Subspace Dimension And Haar Moment Theorem
- The Knill–Laflamme criterion for a protected subsystem Theorem
Dependency tree · two levels
21 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)