Alphabeta Math
ExampleConstruction: AI-adaptedVerification: AI-adaptedPipeline-generatedprecheck passjudge pass (gpt-6-luna)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

A norm-convergent observable with no finite localization region

Statement

Take d=1 and q=2. For n≥1, let Zn be the one-site Pauli matrix Z=diag⁡(1,−1) embedded at site n∈Z. The sequence

HN:=∑n=1N2−nZn

converges in norm in the quasi-local algebra to an element H. This element is self-adjoint but has no finite localization region. Thus norm completion adds observables that are not strictly local.

Facts & Assumptions

Given: d=1, q=2, the local algebras and factor inclusions, and the norm completion A.

[F1]

A localization region for d=1 is a finite subset Λ⊆Z (Local spin matrix algebras and their factor inclusions). Integer addition and 1 are defined by Arithmetic on the integers, the integer order is defined by Order on the integers, and it is a total order compatible with addition by The integers form a totally ordered ring.

[F2]

The integer 1=[(1,0)] is positive: by Order on the integers this is equivalent to 0<1 in N, which holds because 1=σ(0)={0} (Arithmetic on the integers, The integers as equivalence classes of pairs of naturals, The natural numbers N (von Neumann), On N the order is membership: m<n  ⟺  m∈n).

[F3]

Each one-site Pauli matrix Z is self-adjoint and has operator norm one; the factor inclusions are isometric (Local spin matrix algebras and their factor inclusions, Local spin factor inclusions preserve the operator norm).

[F4]

Aloc is dense in its norm completion A, multiplication and adjoint extend continuously, and disjoint local factors commute (Norm-completed quasi-local quantum spin algebra, Quasi-local algebra completion and locality).

Proof

technique · direct

Given: The sequence (HN) and facts [F1]–[F4].

1.1givenF1F2constructalgebra

Fix any finite region Λ⊆Z. Enumerate the finite set F:=Λ∩{n∈Z:0<n} as n1,…,nr, and put S:=∑j=1rnj, taking S=0 when r=0. By induction on the number of terms, every finite sum of positive integers is nonnegative: the empty sum is 0, and if a partial sum R≥0 then adding a positive integer n gives R+n>R≥0, since 0<n translates to R+0≤R+n by [F1], and equality would cancel R in the additive group Z to give 0=n. If k∈F, write S=k+R, where R is the sum of the remaining positive terms; the same induction gives R≥0, and order-compatibility yields S≥k. Set m:=S+1. Since 1>0 by [F2] and S≥0, order-compatibility gives m>S≥0, so m>0. If m∈Λ, then m∈F and the preceding bound gives S≥m, contradicting m>S. Thus every finite region omits a positive integer site.

1.2givenF3F4algebra

If M>N, the triangle inequality and isometric inclusions give ∥HM−HN∥≤∑n=N+1M2−n<2−N. Thus (HN) is Cauchy in Aloc and converges to some H∈A by completion. Since each HN is self-adjoint and the adjoint extends continuously, H∗=H.

2.1F3F4step 1.2algebra

Fix k≥1 and define X=(0110) on C2, and let Xk be its one-site embedding at site k. For N≥k, every Zn with n≠k commutes with Xk by disjoint locality, while direct multiplication gives [Z,X]=ZX−XZ=2iY, where Y=(0−ii0) and Y∗Y=I. Hence [HN,Xk]=2−k(2iY)k for all N≥k. By continuity of multiplication and norm convergence, [H,Xk]=21−kiYk, whose norm is 21−k>0.

3.1F1F4step 1.1step 2.1∎

If H had a finite localization region Λ, step 1.1 supplies k≥1 outside Λ. Then [F4] would give [H,Xk]=0, contradicting step 2.1. Therefore H has no finite localization region.

Depends on

Dependency tree · 2 levels

Sources