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Unnumbered main construction: RAGE contains MPS and weighted-graph/product-superposition states

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QAlgorithms.Papers.Independent.Intakethird100.P57.rage_contains_mps_wgs_products

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

prove2quantum

Let N,D≥1N,D\ge1N,D≥1. For site matrices Ak,b∈CD×DA_{k,b}\in\mathbb C^{D\times D}Ak,b​∈CD×D, let M(A)M(A)M(A) have amplitudes tr⁡(A1,b1⋯AN,bN)\operatorname{tr}(A_{1,b_1}\cdots A_{N,b_N})tr(A1,b1​​⋯AN,bN​​). Let WΦW_\PhiWΦ​ apply diag⁡(1,1,1,eiΦjk)\operatorname{diag}(1,1,1,e^{i\Phi_{jk}})diag(1,1,1,eiΦjk​) once per unordered pair, where Φ\PhiΦ is symmetric, has zero diagonal, and has entries in [0,2π)[0,2\pi)[0,2π). Let V=⨂kVkV=\bigotimes_k V_kV=⨂k​Vk​, Vk∈U(2)V_k\in U(2)Vk​∈U(2), and set R(A,Φ,V)=VWΦM(A)R(A,\Phi,V)=VW_\Phi M(A)R(A,Φ,V)=VWΦ​M(A). Then

R(A,0,I)=M(A),R(A(r),Φ,V)=VWΦ⨂k∣+⟩.R(A,0,I)=M(A),\qquad R(A(r),\Phi,V)=VW_\Phi\bigotimes_k|+\rangle.R(A,0,I)=M(A),R(A(r),Φ,V)=VWΦ​k⨂​∣+⟩.

Here the second equality uses bond-one tensors with both local amplitudes 1/21/\sqrt21/2​. More generally, for m≥1m\ge1m≥1, arbitrary coefficients ctc_tct​, and arbitrary product factors rt,k(b)r_{t,k}(b)rt,k​(b), the diagonal tensors Bk,b(t,t)=rt,k(b)B_{k,b}(t,t)=r_{t,k}(b)Bk,b​(t,t)=rt,k​(b), with an additional factor ctc_tct​ at the first site, satisfy

R(B,Φ,V)=VWΦ∑t=1mct⨂krt,k.R(B,\Phi,V)=VW_\Phi\sum_{t=1}^m c_t\bigotimes_k r_{t,k}.R(B,Φ,V)=VWΦ​t=1∑m​ct​k⨂​rt,k​.

These are exact raw-vector containments, with one common graph and rotation family. Physical states are obtained by normalizing nonzero vectors. In Eq.(3), the factors η(d)\eta(d)η(d) have amplitudes (1,ed)(1,e^d)(1,ed); the conflicting first-line exponent is not asserted.

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 pp.1–2, Eqs.(1)–(3): exact raw-vector containments, including finite
superpositions under one common graph and common rotations. Only the unambiguous second
line of Eq.(3) is used; its conflicting first-line quadratic exponent is deferred. -/
theorem rage_contains_mps_wgs_products {N D : ℕ} (hN : 1 ≤ N) (hD : 1 ≤ D)
    (A : Tensors N D) (G : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ) :
    rage A (emptyPhaseGraph N) (fun _ => 1) = traceMPS A ∧
    rage (productTensors (plusFactors N)) G V =
      enhance G V (productVec (plusFactors N)) ∧
    (∀ (m : ℕ), 1 ≤ m → ∀ (c : Fin m → ℂ)
      (r : Fin m → Fin N → Bool → ℂ),
      rage (diagonalTensors c r) G V = enhance G V (∑ t, c t • productVec (r t))) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P57

end
Source
Renormalization algorithm with graph enhancement, arXiv:0802.1211v1, PDF p. 1, Unnumbered main construction: RAGE contains MPS and weighted-graph/product-superposition states
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What the Lean code literally says, in plain math · gpt-6.1-sol

For all natural numbers N,DN,DN,D satisfying 1≤N1\le N1≤N and 1≤D1\le D1≤D, every family Ak,bA_{k,b}Ak,b​ of complex D×DD\times DD×D matrices indexed by sites k<Nk<Nk<N and Booleans bbb, every real weight function wjkw_{jk}wjk​ satisfying wjk=wkjw_{jk}=w_{kj}wjk​=wkj​, wjj=0w_{jj}=0wjj​=0, and 0≤wjk<2π0\le w_{jk}<2\pi0≤wjk​<2π, and every family of unitary 2×22\times22×2 complex matrices VkV_kVk​ with Boolean row and column indices, the following three statements hold jointly. For a bit string a∈{false,true}Na\in\{\mathrm{false},\mathrm{true}\}^Na∈{false,true}N, write

MA(a)=tr⁡ ⁣(A0,a0A1,a1⋯AN−1,aN−1),Ew,V(v)(b)=∑a∈{false,true}N(∏k=0N−1(Vk)bk,ak)exp⁡ ⁣(i ⁣∑j<kaj=ak=truewjk)v(a);M_A(a)=\operatorname{tr}\!\left(A_{0,a_0}A_{1,a_1}\cdots A_{N-1,a_{N-1}}\right), \qquad E_{w,V}(v)(b)= \sum_{a\in\{\mathrm{false},\mathrm{true}\}^N} \left(\prod_{k=0}^{N-1}(V_k)_{b_k,a_k}\right) \exp\!\left(i\!\sum_{\substack{j<k\\a_j=a_k=\mathrm{true}}}w_{jk}\right)v(a);MA​(a)=tr(A0,a0​​A1,a1​​⋯AN−1,aN−1​​),Ew,V​(v)(b)=a∈{false,true}N∑​(k=0∏N−1​(Vk​)bk​,ak​​)exp​ij<kaj​=ak​=true​∑​wjk​​v(a);

thus the vector denoted by rage⁡(A,G,V)\operatorname{rage}(A,G,V)rage(A,G,V) is Ew,V(MA)E_{w,V}(M_A)Ew,V​(MA​). First, using all-zero weights and identity matrices at every site gives E0,I(MA)=MAE_{0,I}(M_A)=M_AE0,I​(MA​)=MA​. Second, if every site matrix is the 1×11\times11×1 matrix with entry (2)−1(\sqrt2)^{-1}(2​)−1, then its resulting vector is Ew,V(v+)E_{w,V}(v_+)Ew,V​(v+​), where v+(a)=∏k=0N−1(2)−1v_+(a)=\prod_{k=0}^{N-1}(\sqrt2)^{-1}v+​(a)=∏k=0N−1​(2​)−1. Third, for every natural number m≥1m\ge1m≥1, every c:{0,…,m−1}→Cc:\{0,\ldots,m-1\}\to\mathbb Cc:{0,…,m−1}→C, and every complex family r(t,k,b)r(t,k,b)r(t,k,b), form diagonal m×mm\times mm×m site matrices Bk,bB_{k,b}Bk,b​ with diagonal entry ctr(t,k,b)c_t r(t,k,b)ct​r(t,k,b) at k=0k=0k=0 and r(t,k,b)r(t,k,b)r(t,k,b) at k≠0k\ne0k=0; then

Ew,V(MB)=Ew,V ⁣(a⟼∑t=0m−1ct∏k=0N−1r(t,k,ak)).E_{w,V}(M_B)= E_{w,V}\!\left(a\longmapsto \sum_{t=0}^{m-1}c_t\prod_{k=0}^{N-1}r(t,k,a_k)\right).Ew,V​(MB​)=Ew,V​(a⟼t=0∑m−1​ct​k=0∏N−1​r(t,k,ak​)).

The matrices AAA, the coefficients ccc, the factors rrr, and the vectors in these equalities need not be normalized; the hypotheses exclude N=0N=0N=0, D=0D=0D=0, and, in the third statement, m=0m=0m=0.

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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