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Static updates: the one-site energy minimization is a generalized Rayleigh problem

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QAlgorithms.Papers.Independent.Intakethird100.P57.one_site_energy_minimum

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

prove2quantum

Fix N,D≥1N,D\ge1N,D≥1, a valid nonzero RAGE vector, a site kkk, and a Hermitian finite-qubit Hamiltonian HHH. Freeze all data except the two site tensors at kkk. Let x∈C2D2x\in\mathbb C^{2D^2}x∈C2D2 contain their entries, let LLL be the resulting physical-state linear map, and set F=L†HLF=L^\dagger HLF=L†HL, G=L†LG=L^\dagger LG=L†L. Then the updated raw vector is LxLxLx and, whenever x†Gx>0x^\dagger Gx>0x†Gx>0,

E(x)=x†Fxx†Gx.E(x)=\frac{x^\dagger Fx}{x^\dagger Gx}.E(x)=x†Gxx†Fx​.

There exist x∗x_*x∗​ with x∗†Gx∗>0x_*^\dagger Gx_*>0x∗†​Gx∗​>0 and a real λ\lambdaλ such that

Fx∗=λGx∗,E(x∗)=λ≤E(y)(y†Gy>0).Fx_*=\lambda Gx_*,\qquad E(x_*)=\lambda\le E(y)\quad(y^\dagger Gy>0).Fx∗​=λGx∗​,E(x∗​)=λ≤E(y)(y†Gy>0).

The norm matrix may be singular; only vectors with nonzero physical image are admissible. The minimum is an attained one-site optimum.

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.3, Static updates: the generalized Rayleigh reduction and an attained local
minimum. G may have a kernel. Eigenvectors are required to have positive G norm, preventing
common-kernel vectors from making arbitrary real numbers generalized eigenvalues. -/
theorem one_site_energy_minimum {N D : ℕ} (hN : 1 ≤ N) (hD : 1 ≤ D)
    (A : Tensors N D) (Gph : PhaseGraph N) (V : Fin N → Matrix.unitaryGroup Bool ℂ)
    (hv : rage A Gph V ≠ 0) (k : Fin N)
    (H : Matrix (Qubits N) (Qubits N) ℂ) (hH : H.IsHermitian) :
    let L := siteMap A Gph V k
    let F := L.conjTranspose * H * L
    let G := L.conjTranspose * L
    (∀ x : SiteCoordinates D → ℂ,
      rage (replaceSite A k x) Gph V = siteVector L x) ∧
    (∀ x : SiteCoordinates D → ℂ, 0 < (rageSiteQuadratic G x).re →
      rayleighEnergy H (rage (replaceSite A k x) Gph V) =
        (rageSiteQuadratic F x).re / (rageSiteQuadratic G x).re) ∧
    (∃ (x : SiteCoordinates D → ℂ) (lam : ℝ),
      0 < (rageSiteQuadratic G x).re ∧ F.mulVec x = (lam : ℂ) • G.mulVec x ∧
      (rageSiteQuadratic F x).re / (rageSiteQuadratic G x).re = lam ∧
      (∀ y : SiteCoordinates D → ℂ, 0 < (rageSiteQuadratic G y).re →
        lam ≤ (rageSiteQuadratic F y).re / (rageSiteQuadratic G y).re)) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P57

end
Source
Renormalization algorithm with graph enhancement, arXiv:0802.1211v1, PDF p. 3, Static updates: the one-site energy minimization is a generalized Rayleigh problem
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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 with 1≤N1\le N1≤N and 1≤D1\le D1≤D, let Ai(t)A_i(t)Ai​(t) be arbitrary complex D×DD\times DD×D matrices indexed by sites and Boolean values, let real weights wijw_{ij}wij​ satisfy wij=wjiw_{ij}=w_{ji}wij​=wji​, wii=0w_{ii}=0wii​=0, and 0≤wij<2π0\le w_{ij}<2\pi0≤wij​<2π, and let each ViV_iVi​ be a unitary complex 2×22\times22×2 matrix. For any such tensor family BBB, define a vector

v(B)b=∑a:{0,…,N−1}→{0,1}(∏i(Vi)biai)e i∑i<jwijaiajtr⁡ ⁣(B0(a0)⋯BN−1(aN−1)).v(B)_b = \sum_{a:\{0,\ldots,N-1\}\to\{0,1\}} \left(\prod_i(V_i)_{b_i a_i}\right) e^{\,\mathrm i\sum_{i<j}w_{ij}a_i a_j} \operatorname{tr}\!\left(B_0(a_0)\cdots B_{N-1}(a_{N-1})\right).v(B)b​=a:{0,…,N−1}→{0,1}∑​(i∏​(Vi​)bi​ai​​)ei∑i<j​wij​ai​aj​tr(B0​(a0​)⋯BN−1​(aN−1​)).

Assume v(A)≠0v(A)\ne0v(A)=0, choose a site kkk, and let HHH be any Hermitian complex matrix indexed by Boolean assignments on all sites. Write CD={0,1}×{0,…,D−1}×{0,…,D−1}C_D=\{0,1\}\times\{0,\ldots,D-1\}\times\{0,\ldots,D-1\}CD​={0,1}×{0,…,D−1}×{0,…,D−1}. For each x:CD→Cx:C_D\to\mathbb Cx:CD​→C, let A[x]A[x]A[x] retain all matrices away from site kkk and have entries A[x]k(t)ij=x(t,i,j)A[x]_k(t)_{ij}=x(t,i,j)A[x]k​(t)ij​=x(t,i,j). For c∈CDc\in C_Dc∈CD​, let ece_cec​ be 111 at ccc and 000 elsewhere, and define

Lbc=v(A[ec])b,F=L†HL,G=L†L,qM(x)=∑c,d∈CDxc‾Mcdxd.L_{bc}=v(A[e_c])_b,\qquad F=L^\dagger HL,\qquad G=L^\dagger L,\qquad q_M(x)=\sum_{c,d\in C_D}\overline{x_c}M_{cd}x_d.Lbc​=v(A[ec​])b​,F=L†HL,G=L†L,qM​(x)=c,d∈CD​∑​xc​​Mcd​xd​.

The theorem asserts that v(A[x])=Lxv(A[x])=Lxv(A[x])=Lx for every xxx; that whenever Re⁡qG(x)>0\operatorname{Re}q_G(x)>0ReqG​(x)>0,

Re⁡⟨v(A[x]),Hv(A[x])⟩∥v(A[x])∥2=Re⁡qF(x)Re⁡qG(x);\frac{\operatorname{Re}\langle v(A[x]),H v(A[x])\rangle}{\|v(A[x])\|^2} = \frac{\operatorname{Re}q_F(x)}{\operatorname{Re}q_G(x)};∥v(A[x])∥2Re⟨v(A[x]),Hv(A[x])⟩​=ReqG​(x)ReqF​(x)​;

and that there exist x:CD→Cx:C_D\to\mathbb Cx:CD​→C and a real number λ\lambdaλ such that

Re⁡qG(x)>0,Fx=λGx,Re⁡qF(x)Re⁡qG(x)=λ,\operatorname{Re}q_G(x)>0,\qquad Fx=\lambda Gx,\qquad \frac{\operatorname{Re}q_F(x)}{\operatorname{Re}q_G(x)}=\lambda,ReqG​(x)>0,Fx=λGx,ReqG​(x)ReqF​(x)​=λ,

with

λ≤Re⁡qF(y)Re⁡qG(y)for every y:CD→C satisfying Re⁡qG(y)>0.\lambda\le \frac{\operatorname{Re}q_F(y)}{\operatorname{Re}q_G(y)} \quad\text{for every }y:C_D\to\mathbb C \text{ satisfying }\operatorname{Re}q_G(y)>0.λ≤ReqG​(y)ReqF​(y)​for every y:CD​→C satisfying ReqG​(y)>0.

The identity v(A[x])=Lxv(A[x])=Lxv(A[x])=Lx includes choices yielding the zero vector; the quotient identity and the minimizing comparison are restricted to strictly positive denominators. No invertibility of GGG or uniqueness of xxx or λ\lambdaλ is assumed or asserted.

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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