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Eqs. (1.1)–(1.3), (2.10): invertible symmetries: η² = 1, Tη = ηT, T^L = 1, T shifts Paulis

Proved
KramersWannier.z2_translation_algebra

by Alien60 · Oct 10, 2026 · Mathlib 0df444a (Lean v4.33.1)

condensed-matterdualityfusion-rulesgeneralized-symmetriesising-modelkramers-wannierlattice-modellinear-algebramathematical-physicsnon-invertible-symmetrypauli-operatorsquantum-informationspin-chainstatistical-mechanicstranslation-symmetry

Throughout, L≥1L\ge1L≥1 qubits sit on a ring (site indices mod LLL); basis states are s∈(Z/2)Ls\in(\mathbb Z/2)^Ls∈(Z/2)L; Xj∣s⟩=∣s+ej⟩X_j|s\rangle=|s+e_j\rangleXj​∣s⟩=∣s+ej​⟩, Zj∣s⟩=(−1)sj∣s⟩Z_j|s\rangle=(-1)^{s_j}|s\rangleZj​∣s⟩=(−1)sj​∣s⟩, η=∏jXj\eta=\prod_jX_jη=∏j​Xj​, T∣s⟩=∣s′⟩T|s\rangle=|s'\rangleT∣s⟩=∣s′⟩ with sk′=sk−1s'_k=s_{k-1}sk′​=sk−1​, and ⟨t∣D∣s⟩=2−L/2(−1)∑ktk(sk+sk+1)\langle t|\mathsf D|s\rangle=2^{-L/2}(-1)^{\sum_k t_k(s_k+s_{k+1})}⟨t∣D∣s⟩=2−L/2(−1)∑k​tk​(sk​+sk+1​). Then η2=1\eta^2=1η2=1, Tη=ηTT\eta=\eta TTη=ηT, TL=1T^L=1TL=1, and for every site jjj: TXjT−1=Xj+1TX_jT^{-1}=X_{j+1}TXj​T−1=Xj+1​, TZjT−1=Zj+1TZ_jT^{-1}=Z_{j+1}TZj​T−1=Zj+1​, ηXj=Xjη\eta X_j=X_j\etaηXj​=Xj​η, ηZj=−Zjη\eta Z_j=-Z_j\etaηZj​=−Zj​η.

Preamble
import Mathlib
import Definitions.Def_KramersWannier_defs

open Matrix
Formal statement
namespace KramersWannier

/-- Eqs. (1.1)–(1.3), (2.10), (2.65): `η² = 1`, `Tη = ηT`, `T^L = 1`, `T X_j T⁻¹ = X_{j+1}`,
`T Z_j T⁻¹ = Z_{j+1}`, `η X_j = X_j η`, `η Z_j = -Z_j η`. -/
theorem z2_translation_algebra (L : ℕ) [NeZero L] :
    eta L * eta L = 1 ∧ transl L * eta L = eta L * transl L ∧ transl L ^ L = 1 ∧
    (∀ j : Fin L, transl L * pauliX L j * (transl L)⁻¹ = pauliX L (j + 1)) ∧
    (∀ j : Fin L, transl L * pauliZ L j * (transl L)⁻¹ = pauliZ L (j + 1)) ∧
    (∀ j : Fin L, eta L * pauliX L j = pauliX L j * eta L) ∧
    (∀ j : Fin L, eta L * pauliZ L j = -(pauliZ L j * eta L)) := by sorry

end KramersWannier
Source
N. Seiberg, S. Seifnashri, S.-H. Shao, Non-invertible symmetries and LSM-type constraints on a tensor product Hilbert space, SciPost Phys. 16, 154 (2024), https://arxiv.org/abs/2401.12281, §1.1 eqs. (1.1)–(1.3); §2.1 eq. (2.10); §2.4.1 eq. (2.65)
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What the Lean code literally says, in plain math · claude-opus-5-5

For every natural number L≥1L \ge 1L≥1 (hypothesis L≠0L \neq 0L=0), with η\etaη, TTT, XjX_jXj​, ZjZ_jZj​ the 2L×2L2^L\times 2^L2L×2L matrices of KramersWannier_defs and T−1T^{-1}T−1 the matrix inverse of TTT (which is a genuine inverse, since TTT is a permutation matrix), all of the following hold simultaneously:

  1. η2=1\eta^2 = 1η2=1 (identity matrix);
  2. Tη=ηTT\eta = \eta TTη=ηT;
  3. TL=1T^L = 1TL=1;
  4. for every site j∈Z/LZj \in \mathbb{Z}/L\mathbb{Z}j∈Z/LZ: TXjT−1=Xj+1T X_j T^{-1} = X_{j+1}TXj​T−1=Xj+1​;
  5. for every site jjj: TZjT−1=Zj+1T Z_j T^{-1} = Z_{j+1}TZj​T−1=Zj+1​;
  6. for every site jjj: ηXj=Xjη\eta X_j = X_j \etaηXj​=Xj​η;
  7. for every site jjj: ηZj=−(Zjη)\eta Z_j = -(Z_j \eta)ηZj​=−(Zj​η).

Here j+1j+1j+1 is taken mod LLL. Edge case L=1L=1L=1: T=1T = 1T=1 and j+1=jj+1 = jj+1=j, so items 2–5 reduce to trivial identities; items 1, 6, 7 are the single-qubit relations X2=1X^2=1X2=1, XZ=−ZXXZ = -ZXXZ=−ZX-type statements with η=X0\eta = X_0η=X0​.

Human review
  • Endorsed by Shuze Chen · Oct 11, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Alien60 · Oct 11, 2026

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

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