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Szegedy spectral mapping for one and two reflections

Statement

Let D=T∗ST be the discriminant of a finite row-stochastic kernel and let U=S(2TT∗−I) and W=U2. For every eigenvalue λ∈(−1,1) of D, counted with multiplicity, its invariant planes contribute eigenvalues

exp⁡(iarccos⁡λ), exp⁡(−iarccos⁡λ)for U,exp⁡(2iarccos⁡λ), exp⁡(−2iarccos⁡λ)for W.

For each eigendirection with λ=1 (respectively λ=−1), the plane collapses to a line on which U acts as +I (respectively −I), so W acts as +I. On the remaining subspace K=(ran⁡T+ran⁡(ST))⊥, U=−S and its eigenvalues lie in {+1,−1}; therefore all eigenvalues of W there are +1. If X=∅, both spaces are zero and the statements about eigenvalues are vacuous.

Facts & Assumptions

Given: A finite row-stochastic kernel (X,P), the maps T,S,D,U,W from Szegedy row-preparation map and discriminant and Szegedy reflection walk and its two-reflection square, and the root inner product linear in its first argument.

[F1]

The Szegedy discriminant is self-adjoint and contractive: D is self-adjoint, ∥D∥≤1, and T∗T=I.

[F2]

Szegedy walk invariant subspaces from discriminant eigenvectors: if Dv=λv, then span⁡{Tv,STv} is invariant with U(Tv)=STv and U(STv)=−Tv+2λSTv; the span is one-dimensional at λ=±1 and two-dimensional for ∣λ∣<1.

[F3]

Szegedy reflections and walk operators are unitary: U is unitary and equals −S on A⊥, where A=ran⁡T.

[F7]

Principal inverse sine and inverse cosine: arccos⁡:[−1,1]→[0,π] satisfies cos⁡(arccos⁡r)=r.

[F8]

Parity and the Pythagorean identity for sine and cosine: sin⁡2θ+cos⁡2θ=1 for real θ.

[F10]

Euler's formula: exp⁡(iθ)=cos⁡θ+isin⁡θ for every real θ: exp⁡(iθ)=cos⁡θ+isin⁡θ for real θ.

[F12]

Signs, monotonicity intervals, and ranges of sine and cosine: sine is strictly increasing on [−π/2,π/2] and strictly decreasing on [π/2,3π/2].

[F14]

Quarter-turn values and shifts by pi/2 and pi: sin⁡0=0, sin⁡(π/2)=1, and sin⁡π=0.

[F15]

Kernel and image of a linear map: im⁡T={T(v):v∈V}.

Proof

1.1F1F4F5choose

If X=∅, then CX=CX×X={0}, so there are no eigenvalues and the claims are vacuous. Assume now X≠∅. By [F1] and [F4], choose an orthonormal eigenbasis (vj) of the self-adjoint D, with real eigenvalues λj∈[−1,1]; the bound follows from ∥D∥≤1.

2.1F1F2step 1.1algebra

For distinct basis vectors vj,vk, the spans span⁡{Tvj,STvj} and span⁡{Tvk,STvk} are orthogonal: the T-images and their swapped images pair to ⟨vj,vk⟩=0, while the cross pairings equal ⟨vj,Dvk⟩=λk⟨vj,vk⟩=0. These spans together generate A+B, where A=ran⁡T and B=ran⁡(ST).

2.2F2F7F8F9F10F11F12F14step 1.1algebra

Fix an eigenvalue λj∈(−1,1) and its plane basis a=Tvj,b=STvj. By [F2], the matrix of U in the ordered basis (a,b) is (0−112λj), so its characteristic equation is z2−2λjz+1=0. Its roots are z=λj±i1−λj2; each root has eigenvector (1,−z) in these coordinates, and the roots are distinct because ∣λj∣<1. Put θj=arccos⁡λj∈(0,π). By [F7], cos⁡θj=λj. If 0<θj≤π/2, strict increase from sin⁡0=0 on [0,π/2] gives sin⁡θj>0; if π/2<θj<π, strict decrease to sin⁡π=0 on [π/2,π] gives the same. These monotonicity and endpoint facts are [F12] and [F14]. Then [F8] and uniqueness in [F9] yield sin⁡θj=1−λj2. [F10] identifies the roots as exp⁡(±iθj), and [F11] squares them to exp⁡(±2iθj) for W=U2.

2.3F2step 1.1algebra

If λj=±1, [F2] gives STvj=λjTvj, so the corresponding line contributes the single eigenvalue λj to U and +1 to W. This counts one endpoint eigenvalue per eigendirection, not two coincident plane eigenvalues.

3.1F3F6F13F15step 2.1algebra

Let H=A+B, the sum of the images of T and ST as identified by [F15]; both are subspaces by [F13], so their sum is a subspace. By [F6], CX×X=H⊕K with K=H⊥. Since K⊆A⊥, [F3] gives U∣K=−S∣K. The swap preserves K: for a∈A and w∈K, ⟨a,Sw⟩=⟨Sa,w⟩=0 because Sa∈B, and for b∈B and w∈K, ⟨b,Sw⟩=⟨Sb,w⟩=0 because Sb∈A.

4.1F3step 2.2step 2.3step 3.1algebra∎

On K, S2=I, so each w∈K decomposes as (w+Sw)/2+(w−Sw)/2; these summands lie in K by step 3.1 and satisfy S(w+Sw)=w+Sw and S(w−Sw)=−(w−Sw). Thus U=−S has eigenvalues only ±1 on K, and W=U2 is identity there. Combining this with steps 2.2–2.3 gives the complete eigenvalue multiset, including repeated eigenvalues and any overlap of endpoint values with the complement. No irreducibility, aperiodicity, or choice principle is used.

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