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Uniformly bounded finite-range quantum spin interaction — Examples

1 · Prerequisites

2 · Summary

The nearest-neighbor diagonal spin interaction gives an explicit finite-range example, nonzero when J≠0. Its support size, range, and per-site interaction norm are checked directly from the two-site Pauli matrix.

3 · Logical flowchart

4 · Definitions, postulates, theorems and proofs

None yet.

5 · Examples, experiments and counterexamples

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passjudge pass (gpt-6-luna)Open item page →

Nearest-neighbor Ising interaction satisfies the finite-range bounds

Example

Take d=1, q=2, Γ=Z, and let σz=(100−1). For every n∈Z, let En={n,n+1} and set Φ(En)=J σz⊗σz∈AEn for a fixed J∈R; set Φ(S)=0 for every other finite nonempty support S. If interpreted as an energy coefficient, J has units J, but no value or measurement is assumed. This is a nearest-neighbor diagonal spin interaction of the kind described by Uniformly bounded finite-range quantum spin interaction.

Facts & Assumptions

Given: The displayed Pauli matrix, J∈R, and the local tensor-factor conventions of Local spin matrix algebras and their factor inclusions.

[F1]

Local spin matrix algebras and their factor inclusions: the two-site algebra is the finite matrix algebra A{n,n+1} with the ordinary operator norm.

[F2]

Uniformly bounded finite-range quantum spin interaction: an interaction term must be self-adjoint, have uniformly bounded support size and diameter, and have finite per-site norm sum.

Verification

technique · direct finite-dimensional norm and support calculation

Given: [F1]–[F2] and the interaction in the Example.

1.1givenF1algebra

Since (σz)∗=σz and (σz)2=I, the tensor product σz⊗σz is a self-adjoint unitary in AEn and has norm one. Therefore every nonzero term Φ(En) is self-adjoint and has norm ∣J∣.

2.1givenF2step 1.1algebra∎

Each support En has cardinality two and max-metric diameter one. Each site belongs to exactly two such edges, so sup⁡x∈Z∑S∋x∥Φ(S)∥=2∣J∣. All other terms vanish. Hence the interaction satisfies the definition with M=2, R=1, and κ=2∣J∣, including the case J=0.

Sources