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Gauged sheaf QLTC [1]

Description

Qubit code whose dimension has a prime divisor that grows with \(n\), obtained by gauging three sheaf-code QLTC blocks with a cup-product trilinear form [1; Lemma 11]. The family has constant rate, linear distance, and constant operator soundness [1; Thm. 4].

The blocks come from the \(c^3\)-QLTC construction of Ref. [2], with the choices of Ref. [3] that make the trilinear form nonzero [1; App. B.2]. Gauging keeps the \(Z\)-type checks of the blocks [1; Sec. 4.1]. Each \(X\)-type generator of a block is multiplied by a phase set by the trilinear form of its cochain with the other two blocks’ cochains [4][1; Sec. 4.1].

The third block, with cochains \(C^j\) and coboundary \(\delta\), is replaced by \(E^j=C^j\oplus C^{j-1}\) with \(\delta_E(y,x)=(\delta y,\,y-\rho y+\delta x)\), where \(\rho\) is a deck transformation of prime order \(p\) [1; App. B.3]. Cohomology classes of \(E\) then project to classes fixed by \(\rho\) [1; App. B.3]. The trilinear form is evaluated on \(b-\rho b\) for the second block’s cochain \(b\), and the third block’s generators are assigned eigenvalues \((-1)^{\mathrm{Tr}\,\lambda(w)}\) for a nonzero linear functional \(\lambda\) [1; App. B.3]. Acting with \(\rho\) on the first two blocks permutes the triples of cohomology classes labeling a codeword basis without fixed points, so \(p\) divides the code dimension [1; Lemma 11].

Notes

Hamiltonians of gauged sheaf QLTCs have no low-energy trivial magic (NLTM), which proves the NLTM conjecture [5][1; Cor. 5]. The energy density below which preparation from qudit stabilizer states requires circuit depth of order \(\Omega(\log n)\) does not depend on the bound on qudit dimensions [1; Cor. 5].

Cousin

  • Quantum locally testable code (QLTC)— Gauged sheaf QLTCs have linear distance, and their frustration-free Hamiltonians satisfy the operator-soundness form of local testability with constant soundness [1; Thm. 4].

Primary Hierarchy

Parents
Gauged sheaf QLTC codespaces are joint eigenspaces of \(Z\)-type Pauli strings and of \(X\)-type Pauli strings multiplied by constant-weight multi-controlled-\(Z\) phases [1; App. B.1].
Each dressed \(X\)-type generator of a gauged sheaf QLTC is a Pauli \(X\) string times a diagonal phase, so the codespace is a joint eigenspace of monomial operators [1; Sec. 4.1]. The dressed generators commute on the subspace satisfying the \(Z\)-type checks [1; Sec. 4.3].
Gauged sheaf QLTC

References

  1. [1]

    F. Wei, Z. Han, Z. Li, and Z.-W. Liu, “NLTM Hamiltonians from gauged sheaf quantum locally testable codes”, (2026) arXiv:2609.40220

  2. [2]

    W. Gay and F. G. Jeronimo, “Asymptotically Good Quantum Locally Testable Codes”, (2026) arXiv:2609.20780

  3. [3]

    Y. Li, Z. Li, Z. Han, and Z.-W. Liu, “Parallelizable and addressable transversal non-Clifford gates on good quantum LDPC codes”, (2026) arXiv:2609.26691

  4. [4]

    Z. Li, F. Wei, Z. Han, and Z.-W. Liu, “Non-Abelian sheaf quantum LDPC codes: good and magical”, (2026) arXiv:2609.30159

  5. [5]

    F. Wei and Z.-W. Liu, “Long-range nonstabilizerness and quantum codes, phases, and complexity”, (2026) arXiv:2503.04566

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Zoo Code ID: gauged_sheaf_qltc

Cite as:
“Gauged sheaf QLTC”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2026. https://errorcorrectionzoo.org/c/gauged_sheaf_qltc, arXiv:2606.11484
BibTeX:
@incollection{eczoo_gauged_sheaf_qltc,
title={Gauged sheaf QLTC},
booktitle={The Error Correction Zoo},
year={2026},
editor={Albert, Victor V. and Faist, Philippe},
eprint={2606.11484},
doi={10.48550/arXiv.2606.11484},
url={https://errorcorrectionzoo.org/c/gauged_sheaf_qltc}
}
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Cite as:

“Gauged sheaf QLTC”, The Error Correction Zoo (V. V. Albert & P. Faist, eds.), 2026. https://errorcorrectionzoo.org/c/gauged_sheaf_qltc, arXiv:2606.11484

Github: https://github.com/errorcorrectionzoo/eczoo_data/edit/main/codes/quantum/qubits/nonstabilizer/clifford_hierarchy/gauged_sheaf_qltc.yml.