Lean, informalized

Nielsen & Chuang · Chapter 2, Introduction to quantum mechanics · p. 79

Exercise 2.48 - The two factors of each, with the sign of a Hermitian matrix as its unitary factor

Polar decompositions of positive, unitary and Hermitian matrices.

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The Exercise

A square matrix AA has a polar decomposition: a unitary WW and two positive matrices JJ and KK with A=WJ=KW,J=A†A,K=AA†.A = WJ = KW, \qquad J = \sqrt{A^\dagger A}, \qquad K = \sqrt{A A^\dagger}.(1) The exercise asks what this decomposition is for a positive matrix PP, for a unitary matrix UU and for a Hermitian matrix HH.

The Square Root and the Sign

The positive square root B\sqrt{B} of a positive matrix BB is the positive matrix whose square is BB. If B=∑iμi|i⟩⟨i|B = \sum_i \mu_i |i\rangle\langle i| in an orthonormal eigenbasis, with eigenvalues μi≥0\mu_i \ge 0, then B=∑iμi|i⟩⟨i|.\sqrt{B} = \sum_i \sqrt{\mu_i}\,|i\rangle\langle i|.(2)

The sign sgn(H)\mathrm{sgn}(H) of a Hermitian matrix HH is the matrix with the eigenvectors of HH whose eigenvalues are +1+1 where those of HH are positive or zero and −1-1 where they are negative.✦ In an orthonormal eigenbasis, where H=∑iλi|i⟩⟨i|H = \sum_i \lambda_i |i\rangle\langle i|, sgn(H)=∑is(λi)|i⟩⟨i|,s(λ)={+1,λ≥0,−1,λ<0.\mathrm{sgn}(H) = \sum_i s(\lambda_i)\,|i\rangle\langle i|, \qquad s(\lambda) = \begin{cases} +1, & \lambda \ge 0, \\ -1, & \lambda < 0. \end{cases}(3)✦

The Claim

Theorem 1. Let PP, UU and HH be square matrices, PP positive, UU unitary and HH Hermitian. The polar decomposition of PP has the identity as unitary factor, P=IP†P,P = I\,\sqrt{P^\dagger P},(4)✦ and PP itself as both positive factors: P†P=P,\sqrt{P^\dagger P} = P,(5)✦ PP†=P.\sqrt{P P^\dagger} = P.(6)✦ The polar decomposition of UU has UU itself as unitary factor, U=UU†U,U = U\sqrt{U^\dagger U},(7)✦ and the identity as both positive factors: U†U=I,\sqrt{U^\dagger U} = I,(8)✦ UU†=I.\sqrt{U U^\dagger} = I.(9)✦ The sign of HH is unitary, sgn(H)†sgn(H)=sgn(H)sgn(H)†=I,\mathrm{sgn}(H)^\dagger\,\mathrm{sgn}(H) = \mathrm{sgn}(H)\,\mathrm{sgn}(H)^\dagger = I,(10)✦ and is the unitary factor of the polar decomposition of HH, H=sgn(H)H†H,H = \mathrm{sgn}(H)\sqrt{H^\dagger H},(11)✦ whose positive factor is the square root of H2H^2: H†H=H2.\sqrt{H^\dagger H} = \sqrt{H^2}.(12)✦

What Is Checked

The claim is stated over the positive square root (2) and over the sign of a Hermitian matrix (3). Of the sign, the library proves that it is a unitary, (10).