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Critical PSD phases: kernel inequality and half-circle rigidity

Statement

Let G have n>0 vertices and symmetric binary adjacency matrix A, with possible loops. Let d>0, 0≤a<1/32 and ∥A−(d/n)J∥≤ad, where J is the all-ones matrix. Let θ be a critical point of E=12∑x,yAxy(1−cos⁡(θx−θy)) with positive-semidefinite angular Hessian. Choose phase representatives in (−π,π] after rotation so that ρ=n−1∑xeiθx is real and nonnegative. These are the hypotheses of the critical-PSD quadratic-test and mass lemma.

The off-diagonal graph has vertex set V(G) and an edge {x,y} precisely when x≠y and Axy=1; connectedness means that every two vertices are joined by a finite path of such edges, with a path of length zero allowed. A configuration is synchronized when all phases are equal modulo 2π. For u,v∈(−π,π], put K(u,v)=sin⁡(∣u∣−min⁡(∣v∣,π/2)). Then ∑xAxyK(θx,θy)≥0 for every y. If the off-diagonal graph is connected and every ∣θx∣<π/2, all representatives equal zero under the normalization ρ≥0. Thus a normalized nonsynchronized critical PSD state on a connected off-diagonal graph has ∣{x:∣θx∣≥π/2}∣>0.

Facts & Assumptions

[F1]

Under the stated graph, energy and phase hypotheses, the critical-PSD quadratic-test and mass lemma gives ry=∑xAxycos⁡(θx−θy)≥0 and ∑xAxyeiθx=ryeiθy (Critical PSD phases: quadratic tests and small-alpha mass bound). No local-minimum hypothesis is assumed.

[F2]

Phases are angles modulo 2π, and eit=cos⁡t+isin⁡t for real t, with exp⁡(0)=1 (Phasors, trigonometric identities and periodic derivatives). In particular sin⁡0=0, cos⁡0=1, and real and imaginary parts commute with finite sums.

[F3]

Sine and cosine satisfy their addition formulas and the parity identities sin⁡(−t)=−sin⁡t, cos⁡(−t)=cos⁡t (The addition formulas for sine and cosine, Parity and the Pythagorean identity for sine and cosine).

[F4]

Sine is strictly increasing on [−π/2,π/2] and strictly decreasing on [π/2,3π/2]; cosine is strictly decreasing on [0,π] (Signs, monotonicity intervals, and ranges of sine and cosine). The quarter-turn values include sin⁡(π/2)=1, cos⁡(π/2)=0 and sin⁡π=0, and sin⁡(t+π/2)=cos⁡t (Quarter-turn values and shifts by pi/2 and pi). Sine is nonnegative on [0,π] (Angular order and elementary inverse-trigonometric bounds). Together with [F2] and [F3], these facts imply sin⁡t>0 for 0<t<π, sin⁡t<0 for −π/2<t<0, and cos⁡t≤0 for π/2≤∣t∣≤π.

[F5]

A nonempty simple graph is connected when every pair of vertices can be joined by a path; the one-vertex graph permits the path of length zero (Connected graphs and connected components defined by the existence of vertex paths). This definition applies to the off-diagonal graph specified in the Statement.

Proof

Given: The graph, critical PSD configuration, representatives and normalization in the Statement.

Goal: Prove the kernel inequality and half-circle rigidity, and then its stated contrapositive.

1.1F1F2F3F4algebra

Taking real and imaginary parts of the phasor identity in [F1], both directly and after multiplication by e−iθy, gives ∑xAxycos⁡θx=rycos⁡θy and ∑xAxysin⁡(θx−θy)=0. For ∣θy∣≤π/2, put b=∣θy∣. Parity gives cos⁡∣θx∣=cos⁡θx, and nonnegativity of sine on [0,π] gives sin⁡∣θx∣≥∣sin⁡θx∣. If θy≥0, the addition formulas yield K(θx,θy)−sin⁡(θx−θy)=(sin⁡∣θx∣−sin⁡θx)cos⁡b≥0. If θy≤0, they yield K(θx,θy)+sin⁡(θx−θy)=(sin⁡∣θx∣+sin⁡θx)cos⁡b≥0. Here cos⁡b≥0 by [F4]. Since Axy≥0, summing and using the zero sine sum proves the kernel inequality in this region.

2.1F1F3F4step 1.1algebra

If ∣θy∣≥π/2, the quarter-turn and parity identities give K(θx,θy)=sin⁡(∣θx∣−π/2)=−cos⁡θx. Therefore ∑xAxyK(θx,θy)=−rycos⁡θy≥0, since ry≥0 and cos⁡θy≤0. This includes the boundary ∣θy∣=π/2 and completes the kernel inequality.

3.1F4F5step 1.1step 2.1algebra

Suppose the off-diagonal graph is connected and every absolute phase is below π/2. The finite nonempty vertex set has a vertex with maximal absolute phase c<π/2. At any vertex y attaining c, the kernel inequality reads ∑xAxysin⁡(∣θx∣−c)≥0. Each argument lies in [−c,0], so each term is nonpositive, and an off-diagonal neighbor of smaller absolute phase would contribute a strictly negative term. Consequently every neighbor also attains c. Along a path from y to any vertex this property propagates one edge at a time; connectedness therefore gives ∣θx∣=c for every vertex. Loops contribute zero and do not affect the argument.

4.1F2F4F5step 1.1step 3.1algebra∎

If c>0 and both classes V−={x:θx=−c} and V+={x:θx=c} are nonempty, a path between them has an edge crossing the classes. Hence q=∑y∈V−,x∈V+Axy>0. Sum the zero sine identities of step 1.1 over y∈V−: terms within V− vanish and every term from V+ equals Axysin⁡(2c), giving 0=qsin⁡(2c). This contradicts q>0 and sin⁡(2c)>0 for 0<2c<π. Thus all representatives have one common value t with ∣t∣<π/2, including t=0 if c=0. Now ρ=eit is real, so sin⁡t=0; strict monotonicity of sine on [−π/2,π/2] and sin⁡0=0 force t=0. This proves the rigidity assertion. A nonsynchronized normalized state on a connected off-diagonal graph therefore cannot have every absolute phase below π/2, which is exactly the asserted positive cardinality.

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