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Main properties (ii): sufficient conditions for exact cyclic translation invariance

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QAlgorithms.Papers.Independent.Intakethird100.P57.cyclic_translation_invariance

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Let N,D≥1N,D\ge1N,D≥1 and consider the periodic trace MPS vector M(A)M(A)M(A) and the RAGE vector R(A,Φ,V)R(A,\Phi,V)R(A,Φ,V). Suppose that M(A)M(A)M(A) is exactly invariant under one cyclic shift, that the graph weights are circulant, and that all local unitaries are the same:

Φj+1,k+1=Φj,k,Vj=Vk,\Phi_{j+1,k+1}=\Phi_{j,k},\qquad V_j=V_k,Φj+1,k+1​=Φj,k​,Vj​=Vk​,

with indices taken modulo NNN. Then

TR(A,Φ,V)=R(A,Φ,V),T R(A,\Phi,V)=R(A,\Phi,V),TR(A,Φ,V)=R(A,Φ,V),

where TTT is the cyclic permutation of qubits. This is a sufficient condition on the underlying MPS vector, graph, and rotations; it does not require identical site tensors. It is an exact raw-vector identity and also covers N=1N=1N=1.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P57
Formal statement
noncomputable section

open scoped ComplexConjugate Matrix

namespace QAlgorithms.Papers.Independent.Intakethird100.P57

attribute [local instance] Classical.propDecidable

/-- PDF p.2, Main properties (ii): sufficient conditions only. Invariance of the MPS
vector is assumed, rather than the narrower requirement that all tensors be equal. -/
theorem cyclic_translation_invariance {N D : ℕ} (hN : 1 ≤ N) (hD : 1 ≤ D)
    (A : Tensors N D) (G : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ)
    (hA : CyclicInvariant (traceMPS A))
    (hG : ∀ i j, G.weight (nextSite i) (nextSite j) = G.weight i j)
    (hV : ∀ i j, V i = V j) : CyclicInvariant (rage A G V) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P57

end
Source
Renormalization algorithm with graph enhancement, arXiv:0802.1211v1, PDF p. 2, Main properties (ii): sufficient conditions for exact cyclic translation invariance
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every pair of natural numbers N,DN,DN,D with N≥1N\ge1N≥1 and D≥1D\ge1D≥1, take arbitrary complex D×DD\times DD×D matrices Ak(t)A_k(t)Ak​(t) for sites k∈{0,…,N−1}k\in\{0,\ldots,N-1\}k∈{0,…,N−1} and bits ttt, real weights wkℓw_{k\ell}wkℓ​ satisfying symmetry, zero diagonal, and 0≤wkℓ<2π0\le w_{k\ell}<2\pi0≤wkℓ​<2π, and unitary 2×22\times22×2 matrices VkV_kVk​. Write σ(k)=(k+1) mod N\sigma(k)=(k+1)\bmod Nσ(k)=(k+1)modN and

m(b)=tr⁡ ⁣(A0(b0)⋯AN−1(bN−1)).m(b)=\operatorname{tr}\!\left(A_0(b_0)\cdots A_{N-1}(b_{N-1})\right).m(b)=tr(A0​(b0​)⋯AN−1​(bN−1​)).

Assume that m(b∘σ)=m(b)m(b\circ\sigma)=m(b)m(b∘σ)=m(b) for every bit string bbb, that wσ(k),σ(ℓ)=wkℓw_{\sigma(k),\sigma(\ell)}=w_{k\ell}wσ(k),σ(ℓ)​=wkℓ​ for every pair of sites, and that Vk=VℓV_k=V_\ellVk​=Vℓ​ for every pair of sites. Then the vector

r(b)=∑c∈{0,1}N(∏k=0N−1Vk(bk,ck))exp⁡ ⁣(i∑k<ℓwkℓckcℓ)m(c)r(b)= \sum_{c\in\{0,1\}^N} \left(\prod_{k=0}^{N-1}V_k(b_k,c_k)\right) \exp\!\left(\mathrm{i}\sum_{k<\ell}w_{k\ell}c_kc_\ell\right)m(c)r(b)=c∈{0,1}N∑​(k=0∏N−1​Vk​(bk​,ck​))exp(ik<ℓ∑​wkℓ​ck​cℓ​)m(c)

satisfies r(b∘σ)=r(b)r(b\circ\sigma)=r(b)r(b∘σ)=r(b) for every bbb. Products of the matrices AkA_kAk​ are in increasing site order, and the statement includes N=1N=1N=1, when the cyclic shift is the identity.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

    Confirmed by the mission captain (proposal self-audit).

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