Physlib

QuantumInfo.ForMathlib.Unitary

5 declarations

theorem

U∗Uv=vU^* U v = v for unitary linear maps UU

Let EE be a vector space over a field k\mathbf{k}, and let UU be a unitary linear map from EE to EE (U∈unitary(E→kE)U \in \text{unitary}(E \to_{\mathbf{k}} E)). For any vector v∈Ev \in E, applying the adjoint (star) of UU to the result of UU applied to vv returns the original vector vv. That is, U∗(U(v))=vU^*(U(v)) = v.

theorem

U(U∗v)=vU(U^* v) = v for unitary UU

Let EE be a vector space over a field k\mathbb{k}, and let UU be a unitary linear map from EE to EE. For any vector v∈Ev \in E, applying the map UU to the result of its adjoint (star) map applied to vv yields vv, i.e., U(U∗v)=vU(U^* v) = v. Since UU is unitary, its adjoint U∗U^* is its inverse, and this statement expresses the identity U∘U∗=idEU \circ U^* = \text{id}_E.

definition

Linear equivalence between eigenspaces of TT and UTU∗U T U^*

Let EE be a vector space over a field k\mathbf{k}, let T:E→ET: E \to E be a linear map, and let UU be a unitary operator on EE. For any scalar μ∈k\mu \in \mathbf{k}, there exists a linear equivalence between the μ\mu-eigenspace of TT and the μ\mu-eigenspace of the conjugated map UTU∗U T U^*. This equivalence maps an eigenvector vv of TT to UvUv, and its inverse maps an eigenvector ww of UTU∗U T U^* to U∗wU^* w. Elements in both spaces satisfy the condition Tv=μvT v = \mu v and (UTU∗)w=μw(U T U^*) w = \mu w respectively.

theorem

Symmetry is Preserved under Unitary Conjugation

Let EE be a Hilbert space over a field k\mathbb{k}, and let T:E→ET: E \to E be a linear operator. If TT is symmetric (hThT), then for any unitary operator UU on EE, the operator UTU∗U T U^* (the conjugation of TT by UU) is also symmetric. Here, U∗U^* denotes the adjoint of UU, represented as `star U.val`.

definition

Unitary conjugation of a symmetric operator preserves eigenvalues up to a permutation σ\sigma

Let EE be a finite-dimensional inner product space over k\mathbb{k} and T:E→ET: E \to E be a symmetric linear operator (hThT). Given a unitary operator UU, let T′=UTU∗T' = U T U^* be the conjugation of TT by UU. There exists a permutation σ∈Sn\sigma \in S_n (an element of `Equiv.Perm (Fin n)`) such that the sequence of eigenvalues of T′T', denoted by eigenvalues(UTU∗)\text{eigenvalues}(U T U^*), is equal to the sequence of eigenvalues of TT permuted by σ\sigma. In other words, the multiset of eigenvalues of a symmetric operator is invariant under unitary conjugation.